Sample records for ideal pressure gradient

  1. Theory and discretization of ideal magnetohydrodynamic equilibria with fractal pressure profiles

    NASA Astrophysics Data System (ADS)

    Kraus, B. F.; Hudson, S. R.

    2017-09-01

    In three-dimensional ideal magnetohydrodynamics, closed flux surfaces cannot maintain both rational rotational-transform and pressure gradients, as these features together produce unphysical, infinite currents. A proposed set of equilibria nullifies these currents by flattening the pressure on sufficiently wide intervals around each rational surface. Such rational surfaces exist at every scale, which characterizes the pressure profile as self-similar and thus fractal. The pressure profile is approximated numerically by considering a finite number of rational regions and analyzed mathematically by classifying the irrational numbers that support gradients into subsets. Applying these results to a given rotational-transform profile in cylindrical geometry, we find magnetic field and current density profiles compatible with the fractal pressure.

  2. Theory and discretization of ideal magnetohydrodynamic equilibria with fractal pressure profiles

    DOE PAGES

    Kraus, B. F.; Hudson, S. R.

    2017-09-29

    In three-dimensional ideal magnetohydrodynamics, closed flux surfaces cannot maintain both rational rotational-transform and pressure gradients, as these features together produce unphysical, infinite currents. A proposed set of equilibria nullifies these currents by flattening the pressure on sufficiently wide intervals around each rational surface. Such rational surfaces exist at every scale, which characterizes the pressure profile as self-similar and thus fractal. The pressure profile is approximated numerically by considering a finite number of rational regions and analyzed mathematically by classifying the irrational numbers that support gradients into subsets. As a result, applying these results to a given rotational-transform profile in cylindricalmore » geometry, we find magnetic field and current density profiles compatible with the fractal pressure.« less

  3. Theory and discretization of ideal magnetohydrodynamic equilibria with fractal pressure profiles

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Kraus, B. F.; Hudson, S. R.

    In three-dimensional ideal magnetohydrodynamics, closed flux surfaces cannot maintain both rational rotational-transform and pressure gradients, as these features together produce unphysical, infinite currents. A proposed set of equilibria nullifies these currents by flattening the pressure on sufficiently wide intervals around each rational surface. Such rational surfaces exist at every scale, which characterizes the pressure profile as self-similar and thus fractal. The pressure profile is approximated numerically by considering a finite number of rational regions and analyzed mathematically by classifying the irrational numbers that support gradients into subsets. As a result, applying these results to a given rotational-transform profile in cylindricalmore » geometry, we find magnetic field and current density profiles compatible with the fractal pressure.« less

  4. Analytic study on low- external ideal infernal modes in tokamaks with large edge pressure gradients

    NASA Astrophysics Data System (ADS)

    Brunetti, Daniele; Graves, J. P.; Lazzaro, E.; Mariani, A.; Nowak, S.; Cooper, W. A.; Wahlberg, C.

    2018-04-01

    The problem of pressure driven infernal type perturbations near the plasma edge is addressed analytically for a circular limited tokamak configuration which presents an edge flattened safety factor. The plasma is separated from a metallic wall, either ideally conducting or resistive, by a vacuum region. The dispersion relation for such types of instabilities is derived and discussed for two classes of equilibrium profiles for pressure and mass density.

  5. Generation of region 1 current by magnetospheric pressure gradients

    NASA Technical Reports Server (NTRS)

    Yang, Y. S.; Spiro, R. W.; Wolf, R. A.

    1994-01-01

    The Rice Convection Model (RCM) is used to illustrate theoretical possibilities for generating region 1 Birkeland currents by pressure gradients on closed field lines in the Earth's magnetosphere. Inertial effects and viscous forces are neglected. The RCM is applied to idealized cases, to emphasize the basic physical ideas rather than realistic representation of the actual magnetosphere. Ionospheric conductance is taken to be uniform, and the simplest possible representations of the magnetospheric plasma are used. Three basic cases are considered: (1) the case of pure northward Interplanetary Magnetic Field (IMF), with cusp merging assumed to create new closed field lines near the nose of the magnetosphere, following the suggestion by Song and Russell (1992); (2) the case where Dungey-type reconnection occurs at the nose, but magnetosheath plasma somehow enters closed field lines on the dawnside and duskside of the merging region, causing a pressure-driven low-latitude boundary layer; and (3) the case where Dungey-type reconnection occurs at the nose, but region 1 currents flow on sunward drifting plasma sheet field lines. In case 1, currents of region 1 sense are generated by pressure gradients, but those currents do not supply the power for ionospheric convection. Results for case 2 suggest that pressure gradients at the inner edge of the low-latitude boundary layer might generate a large fraction of the region 1 Birkeland currents that drive magnetospheric convection. Results for case 3 indicate that pressure gradients in the plasma sheet could provide part of the region 1 current.

  6. Statistics of pressure and pressure gradient in homogeneous isotropic turbulence

    NASA Technical Reports Server (NTRS)

    Gotoh, T.; Rogallo, R. S.

    1994-01-01

    The statistics of pressure and pressure gradient in stationary isotropic turbulence are measured within direct numerical simulations at low to moderate Reynolds numbers. It is found that the one-point pdf of the pressure is highly skewed and that the pdf of the pressure gradient is of stretched exponential form. The power spectrum of the pressure P(k) is found to be larger than the corresponding spectrum P(sub G)(k) computed from a Gaussian velocity field having the same energy spectrum as that of the DNS field. The ratio P(k)/P(sub G)(k), a measure of the pressure-field intermittence, grows with wavenumber and Reynolds number as -R(sub lambda)(exp 1/2)log(k/k(sub d)) for k less than k(sub d)/2 where k(sub d) is the Kolmogorov wavenumber. The Lagrangian correlations of pressure gradient and velocity are compared and the Lagrangian time scale of the pressure gradient is observed to be much shorter than that of the velocity.

  7. Incorporating high-pressure electroosmotic pump and a nano-flow gradient generator into a miniaturized liquid chromatographic system for peptide analysis.

    PubMed

    Chen, Apeng; Lynch, Kyle B; Wang, Xiaochun; Lu, Joann J; Gu, Congying; Liu, Shaorong

    2014-09-24

    We integrate a high-pressure electroosmotic pump (EOP), a nanoflow gradient generator, and a capillary column into a miniaturized liquid chromatographic system that can be directly coupled with a mass spectrometer for proteomic analysis. We have recently developed a low-cost high-pressure EOP capable of generating pressure of tens of thousands psi, ideal for uses in miniaturized HPLC. The pump worked smoothly when it was used for isocratic elutions. When it was used for gradient elutions, generating reproducible gradient profiles was challenging; because the pump rate fluctuated when the pump was used to pump high-content organic solvents. This presents an issue for separating proteins/peptides since high-content organic solvents are often utilized. In this work, we solve this problem by incorporating our high-pressure EOP with a nano-flow gradient generator so that the EOP needs only to pump an aqueous solution. With this combination, we develop a capillary-based nano-HPLC system capable of performing nano-flow gradient elution; the pump rate is stable, and the gradient profiles are reproducible and can be conveniently tuned. To demonstrate its utility, we couple it with either a UV absorbance detector or a mass spectrometer for peptide separations. Copyright © 2014. Published by Elsevier B.V.

  8. “Breakthrough” osmosis and unusually high power densities in Pressure-Retarded Osmosis in non-ideally semi-permeable supported membranes

    PubMed Central

    Yaroshchuk, Andriy

    2017-01-01

    Osmosis is the movement of solvent across a membrane induced by a solute-concentration gradient. It is very important for cell biology. Recently, it has started finding technological applications in the emerging processes of Forward Osmosis and Pressure-Retarded Osmosis. They use ultrathin and dense membranes supported mechanically by much thicker porous layers. Until now, these processes have been modelled by assuming the membrane to be ideally-semipermeable. We show theoretically that allowing for even minor deviations from ideal semipermeability to solvent can give rise to a previously overlooked mode of “breakthrough” osmosis. Here the rate of osmosis is very large (compared to the conventional mode) and practically unaffected by the so-called Internal Concentration Polarization. In Pressure-Retarded Osmosis, the power densities can easily exceed the conventional mode by one order of magnitude. Much more robust support layers can be used, which is an important technical advantage (reduced membrane damage) in Pressure-Retarded Osmosis. PMID:28332607

  9. Pressure gradients fail to predict diffusio-osmosis

    NASA Astrophysics Data System (ADS)

    Liu, Yawei; Ganti, Raman; Frenkel, Daan

    2018-05-01

    We present numerical simulations of diffusio-osmotic flow, i.e. the fluid flow generated by a concentration gradient along a solid-fluid interface. In our study, we compare a number of distinct approaches that have been proposed for computing such flows and compare them with a reference calculation based on direct, non-equilibrium molecular dynamics simulations. As alternatives, we consider schemes that compute diffusio-osmotic flow from the gradient of the chemical potentials of the constituent species and from the gradient of the component of the pressure tensor parallel to the interface. We find that the approach based on treating chemical potential gradients as external forces acting on various species agrees with the direct simulations, thereby supporting the approach of Marbach et al (2017 J. Chem. Phys. 146 194701). In contrast, an approach based on computing the gradients of the microscopic pressure tensor does not reproduce the direct non-equilibrium results.

  10. Relationship between exercise pressure gradient and haemodynamic progression of aortic stenosis.

    PubMed

    Ringle, Anne; Levy, Franck; Ennezat, Pierre-Vladimir; Le Goffic, Caroline; Castel, Anne-Laure; Delelis, François; Menet, Aymeric; Malaquin, Dorothée; Graux, Pierre; Vincentelli, André; Tribouilloy, Christophe; Maréchaux, Sylvestre

    We hypothesized that large exercise-induced increases in aortic mean pressure gradient can predict haemodynamic progression during follow-up in asymptomatic patients with aortic stenosis. We retrospectively identified patients with asymptomatic moderate or severe aortic stenosis (aortic valve area<1.5cm 2 or<1cm 2 ) and normal ejection fraction, who underwent an exercise stress echocardiography at baseline with a normal exercise test and a resting echocardiography during follow-up. The relationship between exercise-induced increase in aortic mean pressure gradient and annualised changes in resting mean pressure gradient during follow-up was investigated. Fifty-five patients (mean age 66±15 years; 45% severe aortic stenosis) were included. Aortic mean pressure gradient significantly increased from rest to peak exercise (P<0.001). During a median follow-up of 1.6 [1.1-3.2] years, resting mean pressure gradient increased from 35±13mmHg to 48±16mmHg, P<0.0001. Median annualised change in resting mean pressure gradient during follow-up was 5 [2-11] mmHg. Exercise-induced increase in aortic mean pressure gradient did correlate with annualised changes in mean pressure gradient during follow-up (r=0.35, P=0.01). Hemodynamic progression of aortic stenosis was faster in patients with large exercise-induced increase in aortic mean pressure gradient (≥20mmHg) as compared to those with exercise-induced increase in aortic mean pressure gradient<20mmHg (median annualised increase in mean pressure gradient 19 [6-28] vs. 4 [2-10] mmHg/y respectively, P=0.002). Similar results were found in the subgroup of 30 patients with moderate aortic stenosis. Large exercise-induced increases in aortic mean pressure gradient correlate with haemodynamic progression of stenosis during follow-up in patients with asymptomatic aortic stenosis. Further studies are needed to fully establish the role of ESE in the decision-making process in comparison to other prognostic markers in asymptomatic

  11. Flow-related Right Ventricular - Pulmonary Arterial Pressure Gradients during Exercise.

    PubMed

    Wright, Stephen P; Opotowsky, Alexander R; Buchan, Tayler A; Esfandiari, Sam; Granton, John T; Goodman, Jack M; Mak, Susanna

    2018-06-06

    The assumption of equivalence between right ventricular and pulmonary arterial systolic pressure is fundamental to several assessments of right ventricular or pulmonary vascular hemodynamic function. Our aims were to 1) determine whether systolic pressure gradients develop across the right ventricular outflow tract in healthy adults during exercise, 2) examine the potential correlates of such gradients, and 3) consider the effect of such gradients on calculated indices of right ventricular function. Healthy untrained and endurance-trained adult volunteers were studied using right-heart catheterization at rest and during submaximal cycle ergometry. Right ventricular and pulmonary artery pressures were simultaneously transduced, and cardiac output was determined by thermodilution. Systolic pressures, peak and mean gradients, and indices of chamber, vascular, and valve function were analyzed offline. Summary data are reported as mean ± standard deviation or median [interquartile range]. No significant right ventricular outflow tract gradients were observed at rest (mean gradient = 4 [3-5] mmHg), and calculated effective orifice area was 3.6±1.0 cm2. Right ventricular systolic pressure increases during exercise were greater than that of pulmonary artery systolic pressure. Accordingly, mean gradients developed during light exercise (8 [7-9] mmHg) and increased during moderate exercise (12 [9-14] mmHg, p < 0.001). The magnitude of the mean gradient was linearly related to cardiac output (r2 = 0.70, p < 0.001). In healthy adults without pulmonic stenosis, systolic pressure gradients develop during exercise, and the magnitude is related to blood flow rate.

  12. Optimal disturbances in boundary layers subject to streamwise pressure gradient

    NASA Technical Reports Server (NTRS)

    Ashpis, David E.; Tumin, Anatoli

    2003-01-01

    An analysis of the optimal non-modal growth of perturbations in a boundary layer in the presence of a streamwise pressure gradient is presented. The analysis is based on PSE equations for an incompressible fluid. Examples with Falkner-Scan profiles indicate that a favorable pressure gradient decreases the non-modal growth, while an unfavorable pressure gradient leads to an increase of the amplification. It is suggested that the transient growth mechanism be utilized to choose optimal parameters of tripping elements on a low-pressure turbine (LPT) airfoil. As an example, a boundary layer flow with a streamwise pressure gradient corresponding to the pressure distribution over a LPT airfoil is considered. It is shown that there is an optimal spacing of the tripping elements and that the transient growth effect depends on the starting point.

  13. Application of ideal pressure distribution in development process of automobile seats.

    PubMed

    Kilincsoy, U; Wagner, A; Vink, P; Bubb, H

    2016-07-19

    In designing a car seat the ideal pressure distribution is important as it is the largest contact surface between the human and the car. Because of obstacles hindering a more general application of the ideal pressure distribution in seating design, multidimensional measuring techniques are necessary with extensive user tests. The objective of this study is to apply and integrate the knowledge about the ideal pressure distribution in the seat design process for a car manufacturer in an efficient way. Ideal pressure distribution was combined with pressure measurement, in this case pressure mats. In order to integrate this theoretical knowledge of seating comfort in the seat development process for a car manufacturer a special user interface was defined and developed. The mapping of the measured pressure distribution in real-time and accurately scaled to actual seats during test setups directly lead to design implications for seat design even during the test situation. Detailed analysis of the subject's feedback was correlated with objective measurements of the subject's pressure distribution in real time. Therefore existing seating characteristics were taken into account as well. A user interface can incorporate theoretical and validated 'state of the art' models of comfort. Consequently, this information can reduce extensive testing and lead to more detailed results in a shorter time period.

  14. Fifty shades of gradients: does the pressure gradient in venous sinus stenting for idiopathic intracranial hypertension matter? A systematic review.

    PubMed

    McDougall, Cameron M; Ban, Vin Shen; Beecher, Jeffrey; Pride, Lee; Welch, Babu G

    2018-03-02

    OBJECTIVE The role of venous sinus stenting (VSS) for idiopathic intracranial hypertension (IIH) is not well understood. The aim of this systematic review is to attempt to identify subsets of patients with IIH who will benefit from VSS based on the pressure gradients of their venous sinus stenosis. METHODS MEDLINE/PubMed was searched for studies reporting venous pressure gradients across the stenotic segment of the venous sinus, pre- and post-stent pressure gradients, and clinical outcomes after VSS. Findings are reported according to the PRISMA (Preferred Reporting Items for Systematic Reviews and Meta-Analyses) guidelines. RESULTS From 32 eligible studies, a total of 186 patients were included in the analysis. Patients who had favorable outcomes had higher mean pressure gradients (22.8 ± 11.5 mm Hg vs 17.4 ± 8.0 mm Hg, p = 0.033) and higher changes in pressure gradients after stent placement (19.4 ± 10.0 mm Hg vs 12.0 ± 6.0 mm Hg, p = 0.006) compared with those with unfavorable outcomes. The post-stent pressure gradients between the 2 groups were not significantly different (2.8 ± 4.0 mm Hg vs 2.7 ± 2.0 mm Hg, p = 0.934). In a multivariate stepwise logistic regression controlling for age, sex, body mass index, CSF opening pressure, pre-stent pressure gradient, and post-stent pressure gradient, the change in pressure gradient with stent placement was found to be an independent predictor of favorable outcome (p = 0.028). Using a pressure gradient of 21 as a cutoff, 81/86 (94.2%) of patients with a gradient > 21 achieved favorable outcomes, compared with 82/100 (82.0%) of patients with a gradient ≤ 21 (p = 0.022). CONCLUSIONS There appears to be a relationship between the pressure gradient of venous sinus stenosis and the success of VSS in IIH. A randomized controlled trial would help elucidate this relationship and potentially guide patient selection.

  15. Optimal Disturbances in Boundary Layers Subject to Streamwise Pressure Gradient

    NASA Technical Reports Server (NTRS)

    Ashpis, David E.; Tumin, Anatoli

    2003-01-01

    An analysis of the non-modal growth of perturbations in a boundary layer in the presence of a streamwise pressure gradient is presented. The analysis is based on PSE equations for an incompressible fluid. Examples with Falkner- Skan profiles indicate that a favorable pressure gradient decreases the non-modal growth while an unfavorable pressure gradient leads to an increase of the amplification. It is suggested that the transient growth mechanism be utilized to choose optimal parameters of tripping elements on a low-pressure turbine (LPT) airfoil. As an example, a boundary-layer flow with a streamwise pressure gradient corresponding to the pressure distribution over a LPT airfoil is considered. It is shown that there is an optimal spacing of the tripping elements and that the transient growth effect depends on the starting point. The amplification is found to be small at the LPT s very low Reynolds numbers, but there is a possibility to enhance the transient energy growth by means of wall cooling.

  16. Accurate pressure gradient calculations in hydrostatic atmospheric models

    NASA Technical Reports Server (NTRS)

    Carroll, John J.; Mendez-Nunez, Luis R.; Tanrikulu, Saffet

    1987-01-01

    A method for the accurate calculation of the horizontal pressure gradient acceleration in hydrostatic atmospheric models is presented which is especially useful in situations where the isothermal surfaces are not parallel to the vertical coordinate surfaces. The present method is shown to be exact if the potential temperature lapse rate is constant between the vertical pressure integration limits. The technique is applied to both the integration of the hydrostatic equation and the computation of the slope correction term in the horizontal pressure gradient. A fixed vertical grid and a dynamic grid defined by the significant levels in the vertical temperature distribution are employed.

  17. Large-eddy simulations of adverse pressure gradient turbulent boundary layers

    NASA Astrophysics Data System (ADS)

    Bobke, Alexandra; Vinuesa, Ricardo; Örlü, Ramis; Schlatter, Philipp

    2016-04-01

    Adverse pressure-gradient (APG) turbulent boundary layers (TBL) are studied by performing well-resolved large-eddy simulations. The pressure gradient is imposed by defining the free-stream velocity distribution with the description of a power law. Different inflow conditions, box sizes and upper boundary conditions are tested in order to determine the final set-up. The statistics of turbulent boundary layers with two different power-law coefficients and thus magnitudes of adverse pressure gradients are then compared to zero pressure-gradient (ZPG) data. The effect of the APG on TBLs is manifested in the mean flow through a much more prominent wake region and in the Reynolds stresses through the existence of an outer peak. The pre-multiplied energy budgets show that more energy is transported from the near-wall region to farther away from the wall.

  18. Pressure Gradient Effects on Hypersonic Cavity Flow Heating

    NASA Technical Reports Server (NTRS)

    Everhart, Joel L.; Alter, Stephen J.; Merski, N. Ronald; Wood, William A.; Prabhu, Ramadas K.

    2006-01-01

    The effect of a pressure gradient on the local heating disturbance of rectangular cavities tested at hypersonic freestream conditions has been globally assessed using the two-color phosphor thermography method. These experiments were conducted in the Langley 31-Inch Mach 10 Tunnel and were initiated in support of the Space Shuttle Return-To-Flight Program. Two blunted-nose test surface geometries were developed, including an expansion plate test surface with nearly constant negative pressure gradient and a flat plate surface with nearly zero pressure gradient. The test surface designs and flow characterizations were performed using two-dimensional laminar computational methods, while the experimental boundary layer state conditions were inferred using the measured heating distributions. Three-dimensional computational predictions of the entire model geometry were used as a check on the design process. Both open-flow and closed-flow cavities were tested on each test surface. The cavity design parameters and the test condition matrix were established using the computational predictions. Preliminary conclusions based on an analysis of only the cavity centerline data indicate that the presence of the pressure gradient did not alter the open cavity heating for laminar-entry/laminar-exit flows, but did raise the average floor heating for closed cavities. The results of these risk-reduction studies will be used to formulate a heating assessment of potential damage scenarios occurring during future Space Shuttle flights.

  19. Pressure Gradient Effects on Hypersonic Cavity Flow Heating

    NASA Technical Reports Server (NTRS)

    Everhart, Joel L.; Alter, Stephen J.; Merski, N. Ronald; Wood, William A.; Prabhu, Ramdas K.

    2007-01-01

    The effect of a pressure gradient on the local heating disturbance of rectangular cavities tested at hypersonic freestream conditions has been globally assessed using the two-color phosphor thermography method. These experiments were conducted in the Langley 31-Inch Mach 10 Tunnel and were initiated in support of the Space Shuttle Return-To-Flight Program. Two blunted-nose test surface geometries were developed, including an expansion plate test surface with nearly constant negative pressure gradient and a flat plate surface with nearly zero pressure gradient. The test surface designs and flow characterizations were performed using two-dimensional laminar computational methods, while the experimental boundary layer state conditions were inferred using the measured heating distributions. Three-dimensional computational predictions of the entire model geometry were used as a check on the design process. Both open-flow and closed-flow cavities were tested on each test surface. The cavity design parameters and the test condition matrix were established using the computational predictions. Preliminary conclusions based on an analysis of only the cavity centerline data indicate that the presence of the pressure gradient did not alter the open cavity heating for laminar-entry/laminar-exit flows, but did raise the average floor heating for closed cavities. The results of these risk-reduction studies will be used to formulate a heating assessment of potential damage scenarios occurring during future Space Shuttle flights.

  20. Acoustic waves in gases with strong pressure gradients

    NASA Technical Reports Server (NTRS)

    Zorumski, William E.

    1989-01-01

    The effect of strong pressure gradients on the acoustic modes (standing waves) of a rectangular cavity is investigated analytically. When the cavity response is represented by a sum of modes, each mode is found to have two resonant frequencies. The lower frequency is near the Viaesaela-Brundt frequency, which characterizes the buoyant effect, and the higher frequency is above the ordinary acoustic resonance frequency. This finding shows that the propagation velocity of the acoustic waves is increased due to the pressure gradient effect.

  1. Pressure gradient induced generation of microbubbles

    NASA Astrophysics Data System (ADS)

    Evangelio, Alvaro; Campo-Cortes, Francisco; Gordillo, Jose Manuel

    2015-11-01

    It is well known that the controlled production of monodisperse bubbles possesses uncountable applications in medicine, pharmacy and industry. Here we provide with a detailed physical description of the bubble formation processes taking place in a type of flow where the liquid pressure gradient can be straightforwardly controlled. In our experiments, a gas flow rate discharges through a cylindrical needle into a pressurized chamber. The pressure gradient created from the exit of the injection needle towards the entrance of a extraction duct promotes the stretching of the gas ligament downstream. In our analysis, which is supported by an exhaustive experimental study in which the liquid viscosity is varied by three orders of magnitude, different regimes can be distinguished depending mainly on the Reynolds number. Through our physical modeling, we provide closed expressions for both the bubbling frequencies and for the bubble diameters as well as the conditions under which a monodisperse generation is obtained in all regimes found. The excellent agreement between our expressions and the experimental data fully validates our physical modeling.

  2. Evolution of a Planar Wake in Adverse Pressure Gradient

    NASA Technical Reports Server (NTRS)

    Driver, David M.; Mateer, George G.

    2016-01-01

    In the interest of improving the predictability of high-lift systems at maximum lift conditions, a series of fundamental experiments were conducted to study the effects of adverse pressure gradient on a wake flow. Mean and fluctuating velocities were measured with a two-component laser-Doppler velocimeter. Data were obtained for several cases of adverse pressure gradient, producing flows ranging from no reversed flow to massively reversed flow. While the turbulent Reynolds stresses increase with increasing size of the reversed flow region, the gradient of Reynolds stress does not. Computations using various turbulence models were unable to reproduce the reversed flow.

  3. A Study of Wake Development and Structure in Constant Pressure Gradients

    NASA Technical Reports Server (NTRS)

    Thomas, Flint O.; Nelson, R. C.; Liu, Xiaofeng

    2000-01-01

    Motivated by the application to high-lift aerodynamics for commercial transport aircraft, a systematic investigation into the response of symmetric/asymmetric planar turbulent wake development to constant adverse, zero, and favorable pressure gradients has been conducted. The experiments are performed at a Reynolds number of 2.4 million based on the chord of the wake generator. A unique feature of this wake study is that the pressure gradients imposed on the wake flow field are held constant. The experimental measurements involve both conventional LDV and hot wire flow field surveys of mean and turbulent quantities including the turbulent kinetic energy budget. In addition, similarity analysis and numerical simulation have also been conducted for this wake study. A focus of the research has been to isolate the effects of both pressure gradient and initial wake asymmetry on the wake development. Experimental results reveal that the pressure gradient has a tremendous influence on the wake development, despite the relatively modest pressure gradients imposed. For a given pressure gradient, the development of an initially asymmetric wake is different from the initially symmetric wake. An explicit similarity solution for the shape parameters of the symmetric wake is obtained and agrees with the experimental results. The turbulent kinetic energy budget measurements of the symmetric wake demonstrate that except for the convection term, the imposed pressure gradient does not change the fundamental flow physics of turbulent kinetic energy transport. Based on the turbulent kinetic energy budget measurements, an approach to correct the bias error associated with the notoriously difficult dissipation estimate is proposed and validated through the comparison of the experimental estimate with a direct numerical simulation result.

  4. Quantifying Dynamic Changes in Plantar Pressure Gradient in Diabetics with Peripheral Neuropathy.

    PubMed

    Lung, Chi-Wen; Hsiao-Wecksler, Elizabeth T; Burns, Stephanie; Lin, Fang; Jan, Yih-Kuen

    2016-01-01

    Diabetic foot ulcers remain one of the most serious complications of diabetes. Peak plantar pressure (PPP) and peak pressure gradient (PPG) during walking have been shown to be associated with the development of diabetic foot ulcers. To gain further insight into the mechanical etiology of diabetic foot ulcers, examination of the pressure gradient angle (PGA) has been recently proposed. The PGA quantifies directional variation or orientation of the pressure gradient during walking and provides a measure of whether pressure gradient patterns are concentrated or dispersed along the plantar surface. We hypothesized that diabetics at risk of foot ulceration would have smaller PGA in key plantar regions, suggesting less movement of the pressure gradient over time. A total of 27 participants were studied, including 19 diabetics with peripheral neuropathy and 8 non-diabetic control subjects. A foot pressure measurement system was used to measure plantar pressures during walking. PPP, PPG, and PGA were calculated for four foot regions - first toe (T1), first metatarsal head (M1), second metatarsal head (M2), and heel (HL). Consistent with prior studies, PPP and PPG were significantly larger in the diabetic group compared with non-diabetic controls in the T1 and M1 regions, but not M2 or HL. For example, PPP was 165% (P = 0.02) and PPG was 214% (P < 0.001) larger in T1. PGA was found to be significantly smaller in the diabetic group in T1 (46%, P = 0.04), suggesting a more concentrated pressure gradient pattern under the toe. The proposed PGA may improve our understanding of the role of pressure gradient on the risk of diabetic foot ulcers.

  5. Arterial Pressure Gradients during Upright Posture and 30 deg Head Down Tilt

    NASA Technical Reports Server (NTRS)

    Sanchez, E. R; William, J. M.; Ueno, T.; Ballard, R. E.; Hargens, A. R.; Holton, Emily M. (Technical Monitor)

    1997-01-01

    Gravity alters local blood pressure within the body so that arterial pressures in the head and foot are lower and higher, respectively, than that at heart level. Furthermore, vascular responses to local alterations of arterial pressure are probably important to maintain orthostatic tolerance upon return to the Earth after space flight. However, it has been difficult to evaluate the body's arterial pressure gradient due to the lack of noninvasive technology. This study was therefore designed to investigate whether finger arterial pressure (FAP), measured noninvasively, follows a normal hydrostatic pressure gradient above and below heart level during upright posture and 30 deg head down tilt (HDT). Seven healthy subjects gave informed consent and were 19 to 52 years old with a height range of 158 to 181 cm. A Finapres device measured arterial pressure at different levels of the body by moving the hand from 36 cm below heart level (BH) to 72 cm above heart level (AH) in upright posture and from 36 cm BH to 48 cm AH during HDT in increments of 12 cm. Mean FAP creased by 85 mmHg transitioning from BH to AH in upright posture, and the pressure gradient calculated from hydrostatic pressure difference (rho(gh)) was 84 mmHg. In HDT, mean FAP decreased by 65 mmHg from BH to AH, and the calculated pressure gradient was also 65 mmHg. There was no significant difference between the measured FAP gradient and the calculated pressure gradient, although a significant (p = 0.023) offset was seen for absolute arterial pressure in upright posture. These results indicate that arterial pressure at various levels can be obtained from the blood pressure at heart level by calculating rho(gh) + an offset. The offset equals the difference between heart level and the site of measurement. In summary, we conclude that local blood pressure gradients can be measured by noninvasive studies of FAP.

  6. Estimation of pressure gradients at renal artery stenoses

    NASA Astrophysics Data System (ADS)

    Yim, Peter J.; Cebral, Juan R.; Weaver, Ashley; Lutz, Robert J.; Vasbinder, G. Boudewijn C.

    2003-05-01

    Atherosclerotic disease of the renal artery can reduce the blood flow leading to renovascular hypertension and ischemic nephopathy. The kidney responds to a decrease in blood flow by activation of the renin-angiotensin system that increases blood pressure and can result in severe hypertension. Percutaneous translumenal angioplasty (PTA) may be indicated for treatment of renovascular hypertension (RVH). However, direct measurement of renal artery caliber and degree of stenosis has only moderate specificity for detection of RVH. A confounding factor in assessment of the proximal renal artery is that diffuse atherosclerotic disease of the distal branches of the renal artery can produce the same effect on blood-flow as atherosclerotic disease of the proximal renal artery. A methodology is proposed for estimation of pressure gradients at renal artery stenoses from magnetic resonance imaging that could improve the evaluation of renal artery disease. In the proposed methodology, pressure gradients are estimated using computational fluid dynamics (CFD) modeling. Realistic CFD models are constructed from images of vessel shape and measurements of blood-flow rates which are available from magnetic resonance angiography (MRA) and phase-contrast magnetic resonance (MR) imaging respectively. CFD measurement of renal artery pressure gradients has been validated in a physical flow-through model.

  7. On the impact of adverse pressure gradient on the supersonic turbulent boundary layer

    NASA Astrophysics Data System (ADS)

    Wang, Qian-Cheng; Wang, Zhen-Guo; Zhao, Yu-Xin

    2016-11-01

    By employing the particle image velocimetry, the mean and turbulent characteristics of a Mach 2.95 turbulent boundary layer are experimentally investigated without the impact of curvature. The physical mechanism with which the streamwise adverse pressure gradient affects the supersonic boundary layer is revealed. The data are compared to that of the concave boundary layer with similar streamwise distributions of wall static pressure to clarify the separate impacts of the adverse pressure gradient and the concave curvature. The logarithmic law is observed to be well preserved for both of the cases. The dip below the logarithmic law is not observed in present investigation. Theoretical analysis indicates that it could be the result of compromise between the opposite impacts of the compression wave and the increased turbulent intensity. Compared to the zero pressure gradient boundary layer, the principal strain rate and the turbulent intensities are increased by the adverse pressure gradient. The shear layer formed due the hairpin packets could be sharpened by the compression wave, which leads to higher principal strain rate and the associated turbulent level. Due to the additional impact of the centrifugal instability brought by the concave wall, even higher turbulent intensities than that of the adverse pressure gradient case are introduced. The existence of velocity modes within the zero pressure gradient boundary layer suggests that the large scale motions are statistically well organized. The generation of new velocity modes due to the adverse pressure gradient indicates that the turbulent structure is changed by the adverse pressure gradient, through which more turbulence production that cannot be effectively predicted by the Reynolds-stress transport equations could be brought.

  8. High-pressure liquid chromatographic gradient mixer

    DOEpatents

    Daughton, C.G.; Sakaji, R.H.

    1982-09-08

    A gradient mixer effects the continuous mixing of any two miscible solvents without excessive decay or dispersion of the resultant isocratic effluent or of a linear or exponential gradient. The two solvents are fed under low or high pressure by means of two high performance liquid chromatographic pumps. The mixer comprises a series of ultra-low dead volume stainless steel tubes and low dead volume chambers. The two solvent streams impinge head-on at high fluxes. This initial nonhomogeneous mixture is then passed through a chamber packed with spirally-wound wires which cause turbulent mixing thereby homogenizing the mixture with minimum band-broadening.

  9. Axisymmetric magnetorotational instability in ideal and viscous laboratory plasmas

    NASA Astrophysics Data System (ADS)

    Mikhailovskii, A. B.; Lominadze, J. G.; Churikov, A. P.; Erokhin, N. N.; Pustovitov, V. D.; Konovalov, S. V.

    2008-10-01

    The original analysis of the axisymmetric magnetorotational instability (MRI) by Velikhov (Sov. Phys. JETP 9, 995 (1959)) and Chandrasekhar (Proc. Nat. Acad. Sci. 46, 253 (1960)), applied to the ideally conducting magnetized medium in the laboratory conditions and restricted to the incompressible approximation, is extended by allowing for the compressibility. Thereby, two additional driving mechanisms of MRI are revealed in addition to the standard drive due to the negative medium rotation frequency gradient (the Velikhov effect). One is due to the squared medium pressure gradient and another is a combined effect of the pressure and density gradients. For laboratory applications, the expression for the MRI boundary with all the above driving mechanisms and the stabilizing magnetoacoustic effect is derived. The effects of parallel and perpendicular viscosities on the MRI in the laboratory plasma are investigated. It is shown that, for strong viscosity, there is a family of MRI driven for the same condition as the ideal one. It is also revealed that the presence of strong viscosity leads to additional family of instabilities called the viscosity-driven MRI. Then the parallel-viscositydriven MRI looks as an overstability (oscillatory instability) possessing both the growth rate and the real part of oscillation frequency, while the perpendicular-viscosity MRI is the aperiodical instability.

  10. Analytic Formulation and Numerical Implementation of an Acoustic Pressure Gradient Prediction

    NASA Technical Reports Server (NTRS)

    Lee, Seongkyu; Brentner, Kenneth S.; Farassat, Fereidoun

    2007-01-01

    The scattering of rotor noise is an area that has received little attention over the years, yet the limited work that has been done has shown that both the directivity and intensity of the acoustic field may be significantly modified by the presence of scattering bodies. One of the inputs needed to compute the scattered acoustic field is the acoustic pressure gradient on a scattering surface. Two new analytical formulations of the acoustic pressure gradient have been developed and implemented in the PSU-WOPWOP rotor noise prediction code. These formulations are presented in this paper. The first formulation is derived by taking the gradient of Farassat's retarded-time Formulation 1A. Although this formulation is relatively simple, it requires numerical time differentiation of the acoustic integrals. In the second formulation, the time differentiation is taken inside the integrals analytically. The acoustic pressure gradient predicted by these new formulations is validated through comparison with the acoustic pressure gradient determined by a purely numerical approach for two model rotors. The agreement between analytic formulations and numerical method is excellent for both stationary and moving observers case.

  11. On Localized Vapor Pressure Gradients Governing Condensation and Frost Phenomena.

    PubMed

    Nath, Saurabh; Boreyko, Jonathan B

    2016-08-23

    Interdroplet vapor pressure gradients are the driving mechanism for several phase-change phenomena such as condensation dry zones, interdroplet ice bridging, dry zones around ice, and frost halos. Despite the fundamental nature of the underlying pressure gradients, the majority of studies on these emerging phenomena have been primarily empirical. Using classical nucleation theory and Becker-Döring embryo formation kinetics, here we calculate the pressure field for all possible modes of condensation and desublimation in order to gain fundamental insight into how pressure gradients govern the behavior of dry zones, condensation frosting, and frost halos. Our findings reveal that in a variety of phase-change systems the thermodynamically favorable mode of nucleation can switch between condensation and desublimation depending upon the temperature and wettability of the surface. The calculated pressure field is used to model the length of a dry zone around liquid or ice droplets over a broad parameter space. The long-standing question of whether the vapor pressure at the interface of growing frost is saturated or supersaturated is resolved by considering the kinetics of interdroplet ice bridging. Finally, on the basis of theoretical calculations, we propose that there exists a new mode of frost halo that is yet to be experimentally observed; a bimodal phase map is developed, demonstrating its dependence on the temperature and wettability of the underlying substrate. We hope that the model and predictions contained herein will assist future efforts to exploit localized vapor pressure gradients for the design of spatially controlled or antifrosting phase-change systems.

  12. High pressure liquid chromatographic gradient mixer

    DOEpatents

    Daughton, Christian G.; Sakaji, Richard H.

    1985-01-01

    A gradient mixer which effects the continuous mixing of any two miscible solvents without excessive decay or dispersion of the resultant isocratic effluent or of a linear or exponential gradient. The two solvents are fed under low or high pressure by means of two high performance liquid chromatographic pumps. The mixer comprises a series of ultra-low dead volume stainless steel tubes and low dead volume chambers. The two solvent streams impinge head-on at high fluxes. This initial nonhomogeneous mixture is then passed through a chamber packed with spirally-wound wires which cause turbulent mixing thereby homogenizing the mixture with minimum "band-broadening".

  13. Direct measurements of local bed shear stress in the presence of pressure gradients

    NASA Astrophysics Data System (ADS)

    Pujara, Nimish; Liu, Philip L.-F.

    2014-07-01

    This paper describes the development of a shear plate sensor capable of directly measuring the local mean bed shear stress in small-scale and large-scale laboratory flumes. The sensor is capable of measuring bed shear stress in the range 200 Pa with an accuracy up to 1 %. Its size, 43 mm in the flow direction, is designed to be small enough to give spatially local measurements, and its bandwidth, 75 Hz, is high enough to resolve time-varying forcing. Typically, shear plate sensors are restricted to use in zero pressure gradient flows because secondary forces on the edge of the shear plate caused by pressure gradients can introduce large errors. However, by analysis of the pressure distribution at the edges of the shear plate in mild pressure gradients, we introduce a new methodology for correcting for the pressure gradient force. The developed sensor includes pressure tappings to measure the pressure gradient in the flow, and the methodology for correction is applied to obtain accurate measurements of bed shear stress under solitary waves in a small-scale wave flume. The sensor is also validated by measurements in a turbulent flat plate boundary layer in open channel flow.

  14. Ideal resuscitation pressure for uncontrolled hemorrhagic shock in different ages and sexes of rats

    PubMed Central

    2013-01-01

    Introduction Our previous studies demonstrated that 50-60 mmHg mean arterial blood pressure was the ideal target hypotension for uncontrolled hemorrhagic shock during the active hemorrhage in sexually mature rats. The ideal target resuscitation pressure for immature and older rats has not been determined. Methods To elucidate this issue, using uncontrolled hemorrhagic-shock rats of different ages and sexes (6 weeks, 14 weeks and 1.5 years representing pre-adult, adult and older rats, respectively), the resuscitation effects of different target pressures (40, 50, 60, 70 and 80 mmHg) on uncontrolled hemorrhagic shock during active hemorrhage and the age and sex differences were observed. Results Different target resuscitation pressures had different resuscitation outcomes for the same age and sex of rats. The optimal target resuscitation pressures for 6-week-old, 14-week-old and 1.5-year-old rats were 40 to 50 mmHg, 50 to 60 mmHg and 70 mmHg respectively. Ideal target resuscitation pressures were significantly superior to other resuscitation pressures in improving the hemodynamics, blood perfusion, organ function and animal survival of uncontrolled hemorrhagic-shock rats (P < 0.01). For same target resuscitation pressures, the beneficial effect on hemorrhagic shock had a significant age difference (P < 0.01) but no sex difference (P > 0.05). Different resuscitation pressures had no effect on coagulation function. Conclusion Hemorrhagic-shock rats at different ages have different target resuscitation pressures during active hemorrhage. The ideal target resuscitation hypotension for 6-week-old, 14-week-old and 1.5-year-old rats was 40 to 50 mmHg, 50 to 60 mmHg and 70 mmHg, respectively. Their resuscitation effects have significant age difference but had no sex difference. PMID:24020401

  15. Buoyancy-Driven Heat Transfer During Application of a Thermal Gradient for the Study of Vapor Deposition at Low Pressure Using and Ideal Gas

    NASA Technical Reports Server (NTRS)

    Frazier, D. O.; Hung, R. J.; Paley, M. S.; Penn, B. G.; Long, Y. T.

    1996-01-01

    A mathematical model has been developed to determine heat transfer during vapor deposition of source materials under a variety of orientations relative to gravitational accelerations. The model demonstrates that convection can occur at total pressures as low as 10-2 mm Hg. Through numerical computation, using physical material parameters of air, a series of time steps demonstrates the development of flow and temperature profiles during the course of vapor deposition. These computations show that in unit gravity vapor deposition occurs by transport through a fairly complicated circulating flow pattern when applying heat to the bottom of the vessel with parallel orientation with respect to the gravity vector. The model material parameters for air predict the effect of kinematic viscosity to be of the same order as thermal diffusivity, which is the case for Prandtl number approx. 1 fluids. Qualitative agreement between experiment and the model indicates that 6-(2-methyl-4-nitroanilino)-2,4-hexadiyn-l-ol (DAMNA) at these pressures indeed approximates an ideal gas at the experiment temperatures, and may validate the use of air physical constants. It is apparent that complicated nonuniform temperature distribution in the vapor could dramatically affect the homogeneity, orientation, and quality of deposited films. The experimental test i's a qualitative comparison of film thickness using ultraviolet-visible spectroscopy on films generated in appropriately oriented vapor deposition cells. In the case where heating of the reaction vessel occurs from the top, deposition of vapor does not normally occur by convection due to a stable stratified medium. When vapor deposition occurs in vessels heated at the bottom, but oriented relative to the gravity vector between these two extremes, horizontal thermal gradients induce a complex flow pattern. In the plane parallel to the tilt axis, the flow pattern is symmetrical and opposite in direction from that where the vessel is

  16. A wet/wet differential pressure sensor for measuring vertical hydraulic gradient.

    PubMed

    Fritz, Brad G; Mackley, Rob D

    2010-01-01

    Vertical hydraulic gradient is commonly measured in rivers, lakes, and streams for studies of groundwater-surface water interaction. While a number of methods with subtle differences have been applied, these methods can generally be separated into two categories; measuring surface water elevation and pressure in the subsurface separately or making direct measurements of the head difference with a manometer. Making separate head measurements allows for the use of electronic pressure sensors, providing large datasets that are particularly useful when the vertical hydraulic gradient fluctuates over time. On the other hand, using a manometer-based method provides an easier and more rapid measurement with a simpler computation to calculate the vertical hydraulic gradient. In this study, we evaluated a wet/wet differential pressure sensor for use in measuring vertical hydraulic gradient. This approach combines the advantage of high-temporal frequency measurements obtained with instrumented piezometers with the simplicity and reduced potential for human-induced error obtained with a manometer board method. Our results showed that the wet/wet differential pressure sensor provided results comparable to more traditional methods, making it an acceptable method for future use.

  17. Experimental analysis of the boundary layer transition with zero and positive pressure gradient

    NASA Technical Reports Server (NTRS)

    Arnal, D.; Jullen, J. C.; Michel, R.

    1980-01-01

    The influence of a positive pressure gradient on the boundary layer transition is studied. The mean velocity and turbulence profiles of four cases are examined. As the intensity of the pressure gradient is increased, the Reynolds number of the transition onset and the length of the transition region are reduced. The Tollmein-Schlichting waves disturb the laminar regime; the amplification of these waves is in good agreement with the stability theory. The three dimensional deformation of the waves leads finally to the appearance of turbulence. In the case of zero pressure gradient, the properties of the turbulent spots are studied by conditional sampling of the hot-wire signal; in the case of positive pressure gradient, the turbulence appears in a progressive manner and the turbulent spots are much more difficult to characterize.

  18. Secondary subharmonic instability of boundary layers with pressure gradient and suction

    NASA Technical Reports Server (NTRS)

    El-Hady, Nabil M.

    1988-01-01

    Three-dimensional linear secondary instability is investigated for boundary layers with pressure gradient and suction in the presence of a finite amplitude TS wave. The focus is on principal parametric resonance responsible for a strong growth of subharmonics in a low disturbance environment. Calculations are presented for the effect of pressure gradients and suction on controlling the onset and amplification of the secondary instability.

  19. Thermodynamic and energy efficiency analysis of power generation from natural salinity gradients by pressure retarded osmosis.

    PubMed

    Yip, Ngai Yin; Elimelech, Menachem

    2012-05-01

    The Gibbs free energy of mixing dissipated when fresh river water flows into the sea can be harnessed for sustainable power generation. Pressure retarded osmosis (PRO) is one of the methods proposed to generate power from natural salinity gradients. In this study, we carry out a thermodynamic and energy efficiency analysis of PRO work extraction. First, we present a reversible thermodynamic model for PRO and verify that the theoretical maximum extractable work in a reversible PRO process is identical to the Gibbs free energy of mixing. Work extraction in an irreversible constant-pressure PRO process is then examined. We derive an expression for the maximum extractable work in a constant-pressure PRO process and show that it is less than the ideal work (i.e., Gibbs free energy of mixing) due to inefficiencies intrinsic to the process. These inherent inefficiencies are attributed to (i) frictional losses required to overcome hydraulic resistance and drive water permeation and (ii) unutilized energy due to the discontinuation of water permeation when the osmotic pressure difference becomes equal to the applied hydraulic pressure. The highest extractable work in constant-pressure PRO with a seawater draw solution and river water feed solution is 0.75 kWh/m(3) while the free energy of mixing is 0.81 kWh/m(3)-a thermodynamic extraction efficiency of 91.1%. Our analysis further reveals that the operational objective to achieve high power density in a practical PRO process is inconsistent with the goal of maximum energy extraction. This study demonstrates thermodynamic and energetic approaches for PRO and offers insights on actual energy accessible for utilization in PRO power generation through salinity gradients. © 2012 American Chemical Society

  20. Rotation and kinetic modifications of the tokamak ideal-wall pressure limit.

    PubMed

    Menard, J E; Wang, Z; Liu, Y; Bell, R E; Kaye, S M; Park, J-K; Tritz, K

    2014-12-19

    The impact of toroidal rotation, energetic ions, and drift-kinetic effects on the tokamak ideal wall mode stability limit is considered theoretically and compared to experiment for the first time. It is shown that high toroidal rotation can be an important destabilizing mechanism primarily through the angular velocity shear; non-Maxwellian fast ions can also be destabilizing, and drift-kinetic damping can potentially offset these destabilization mechanisms. These results are obtained using the unique parameter regime accessible in the spherical torus NSTX of high toroidal rotation speed relative to the thermal and Alfvén speeds and high kinetic pressure relative to the magnetic pressure. Inclusion of rotation and kinetic effects significantly improves agreement between measured and predicted ideal stability characteristics and may provide new insight into tearing mode triggering.

  1. Experimental feasibility of investigating acoustic waves in Couette flow with entropy and pressure gradients

    NASA Technical Reports Server (NTRS)

    Parrott, Tony L.; Zorumski, William E.; Rawls, John W., Jr.

    1990-01-01

    The feasibility is discussed for an experimental program for studying the behavior of acoustic wave propagation in the presence of strong gradients of pressure, temperature, and flow. Theory suggests that gradients effects can be experimentally observed as resonant frequency shifts and mode shape changes in a waveguide. A convenient experimental geometry for such experiments is the annular region between two co-rotating cylinders. Radial temperature gradients in a spinning annulus can be generated by differentially heating the two cylinders via electromagnetic induction. Radial pressure gradients can be controlled by varying the cylinder spin rates. Present technology appears adequate to construct an apparatus to allow independent control of temperature and pressure gradients. A complicating feature of a more advanced experiment, involving flow gradients, is the requirement for independently controlled cylinder spin rates. Also, the boundary condition at annulus terminations must be such that flow gradients are minimally disturbed. The design and construction of an advanced apparatus to include flow gradients will require additional technology development.

  2. Analytic Formulation and Numerical Implementation of an Acoustic Pressure Gradient Prediction

    NASA Technical Reports Server (NTRS)

    Lee, Seongkyu; Brentner, Kenneth S.; Farassat, F.; Morris, Philip J.

    2008-01-01

    Two new analytical formulations of the acoustic pressure gradient have been developed and implemented in the PSU-WOPWOP rotor noise prediction code. The pressure gradient can be used to solve the boundary condition for scattering problems and it is a key aspect to solve acoustic scattering problems. The first formulation is derived from the gradient of the Ffowcs Williams-Hawkings (FW-H) equation. This formulation has a form involving the observer time differentiation outside the integrals. In the second formulation, the time differentiation is taken inside the integrals analytically. This formulation avoids the numerical time differentiation with respect to the observer time, which is computationally more efficient. The acoustic pressure gradient predicted by these new formulations is validated through comparison with available exact solutions for a stationary and moving monopole sources. The agreement between the predictions and exact solutions is excellent. The formulations are applied to the rotor noise problems for two model rotors. A purely numerical approach is compared with the analytical formulations. The agreement between the analytical formulations and the numerical method is excellent for both stationary and moving observer cases.

  3. Sociocultural pressures, thin-ideal internalization, self-objectification, and body dissatisfaction: could feminist beliefs be a moderating factor?

    PubMed

    Myers, Taryn A; Crowther, Janis H

    2007-09-01

    Theory and research suggest that sociocultural pressures, thin-ideal internalization, and self-objectification are associated with body dissatisfaction, while feminist beliefs may serve a protective function. This research examined thin-ideal internalization and self-objectification as mediators and feminist beliefs as a moderator in the relationship between sociocultural pressures to meet the thin-ideal and body dissatisfaction. Female undergraduate volunteers (N=195) completed self-report measures assessing sociocultural influences, feminist beliefs, thin-ideal internalization, self-objectification, and body dissatisfaction. Multisample structural equation modeling showed that feminist beliefs moderate the relationship between media awareness and thin-ideal internalization, but not the relationship between social influence and thin-ideal internalization. Research and clinical implications of these findings are discussed.

  4. Computation of Turbulent Wake Flows in Variable Pressure Gradient

    NASA Technical Reports Server (NTRS)

    Duquesne, N.; Carlson, J. R.; Rumsey, C. L.; Gatski, T. B.

    1999-01-01

    Transport aircraft performance is strongly influenced by the effectiveness of high-lift systems. Developing wakes generated by the airfoil elements are subjected to strong pressure gradients and can thicken very rapidly, limiting maximum lift. This paper focuses on the effects of various pressure gradients on developing symmetric wakes and on the ability of a linear eddy viscosity model and a non-linear explicit algebraic stress model to accurately predict their downstream evolution. In order to reduce the uncertainties arising from numerical issues when assessing the performance of turbulence models, three different numerical codes with the same turbulence models are used. Results are compared to available experimental data to assess the accuracy of the computational results.

  5. Thermophoresis of dissolved molecules and polymers: Consideration of the temperature-induced macroscopic pressure gradient

    NASA Astrophysics Data System (ADS)

    Semenov, Semen; Schimpf, Martin

    2004-01-01

    The movement of molecules and homopolymer chains dissolved in a nonelectrolyte solvent in response to a temperature gradient is considered a consequence of temperature-induced pressure gradients in the solvent layer surrounding the solute molecules. Local pressure gradients are produced by nonuniform London van der Waals interactions, established by gradients in the concentration (density) of solvent molecules. The density gradient is produced by variations in solvent thermal expansion within the nonuniform temperature field. The resulting expression for the velocity of the solute contains the Hamaker constants for solute-solvent and solute-solute interactions, the radius of the solute molecule, and the viscosity and cubic coefficient of thermal expansion of the solvent. In this paper we consider an additional force that arises from directional asymmetry in the interaction between solvent molecules. In a closed cell, the resulting macroscopic pressure gradient gives rise to a volume force that affects the motion of dissolved solutes. An expression for this macroscopic pressure gradient is derived and the resulting force is incorporated into the expression for the solute velocity. The expression is used to calculate thermodiffusion coefficients for polystyrene in several organic solvents. When these values are compared to those measured in the laboratory, the consistency is better than that found in previous reports, which did not consider the macroscopic pressure gradient that arises in a closed thermodiffusion cell. The model also allows for the movement of solute in either direction, depending on the relative values of the solvent and solute Hamaker constants.

  6. Observations of wave-induced pore pressure gradients and bed level response on a surf zone sandbar

    NASA Astrophysics Data System (ADS)

    Anderson, Dylan; Cox, Dan; Mieras, Ryan; Puleo, Jack A.; Hsu, Tian-Jian

    2017-06-01

    Horizontal and vertical pressure gradients may be important physical mechanisms contributing to onshore sediment transport beneath steep, near-breaking waves in the surf zone. A barred beach was constructed in a large-scale laboratory wave flume with a fixed profile containing a mobile sediment layer on the crest of the sandbar. Horizontal and vertical pore pressure gradients were obtained by finite differences of measurements from an array of pressure transducers buried within the upper several centimeters of the bed. Colocated observations of erosion depth were made during asymmetric wave trials with wave heights between 0.10 and 0.98 m, consistently resulting in onshore sheet flow sediment transport. The pore pressure gradient vector within the bed exhibited temporal rotations during each wave cycle, directed predominantly upward under the trough and then rapidly rotating onshore and downward as the wavefront passed. The magnitude of the pore pressure gradient during each phase of rotation was correlated with local wave steepness and relative depth. Momentary bed failures as deep as 20 grain diameters were coincident with sharp increases in the onshore-directed pore pressure gradients, but occurred at horizontal pressure gradients less than theoretical critical values for initiation of the motion for compact beds. An expression combining the effects of both horizontal and vertical pore pressure gradients with bed shear stress and soil stability is used to determine that failure of the bed is initiated at nonnegligible values of both forces.Plain Language SummaryThe <span class="hlt">pressure</span> <span class="hlt">gradient</span> present within the seabed beneath breaking waves may be an important physical mechanism transporting sediment. A large-scale laboratory was used to replicate realistic surfzone conditions in controlled tests, allowing for horizontal and vertical <span class="hlt">pressure</span> <span class="hlt">gradient</span> magnitudes and the resulting sediment bed response to be observed with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/8160828','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/8160828"><span>Intramyocardial <span class="hlt">pressure</span> <span class="hlt">gradients</span> in working and nonworking isolated cat hearts.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mihailescu, L S; Abel, F L</p> <p>1994-03-01</p> <p>This study presents an improved method for the measurement of intramyocardial <span class="hlt">pressure</span> (IMP) using the servo-nulling mechanism. Glass micropipettes (20-24 microns OD) were used as transducers, coated to increase their mechanical resistance to breakage, and placed inside the left ventricular wall with a micropipette holder and manipulator. IMP was measured at the base of the left ventricle in working and nonworking isolated cat hearts that were perfused with Krebs-Henseleit buffer. In working hearts a transmural <span class="hlt">gradient</span> of systolic IMP oriented from endocardium toward the epicardium was found; the endocardial values for systolic IMP were slightly higher than systolic left ventricular <span class="hlt">pressure</span> (LVP), by 11-18%. Increases in afterload induced increases in IMP, without changing the systolic IMP-to-LVP ratio. In nonworking hearts with drained left ventricles, the systolic transmural <span class="hlt">gradient</span> for IMP described for working hearts persisted, but at lower values, and was directly dependent on coronary perfusion <span class="hlt">pressure</span>. Systolic IMP-to-LVP ratios were always > 1. The diastolic IMP of both working and nonworking hearts exhibited irregular transmural <span class="hlt">gradients</span>. Our results support the view that generated systolic IMP is largely independent of LVP development.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..DFDL22008C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..DFDL22008C"><span>Assessment of fluctuating <span class="hlt">pressure</span> <span class="hlt">gradient</span> using acceleration spectra in near wall flows</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cadel, Daniel; Lowe, K. Todd</p> <p>2015-11-01</p> <p>Separation of contributions to the fluctuating acceleration from <span class="hlt">pressure</span> <span class="hlt">gradient</span> fluctuations and viscous shear fluctuations in the frequency domain is examined in a turbulent boundary layer. Past work leveraging turbulent accelerations for <span class="hlt">pressure</span> <span class="hlt">gradient</span> measurements has neglected the viscous shear term from the momentum equation--an invalid assumption in the case of near wall flows. The present study seeks to account for the influence of the viscous shear term and spectrally reject its contribution, which is thought to be concentrated at higher frequencies. Spectra of velocity and acceleration fluctuations in a flat plate, zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> turbulent boundary layer at a momentum thickness Reynolds number of 7500 are measured using a spatially resolving three-component laser Doppler velocimeter. This canonical case data is applied for validation of the spectral approach for future application in more complex aerodynamic flows.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013APS..DFDA25002K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013APS..DFDA25002K"><span>Plasma Streamwise Vortex Generators in an Adverse <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kelley, Christopher; Corke, Thomas; Thomas, Flint</p> <p>2013-11-01</p> <p>A wind tunnel experiment was conducted to compare plasma streamwise vortex generators (PSVGs) and passive vortex generators (VGs). These devices were installed on a wing section by which the angle of attack could be used to vary the streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The experiment was performed for freestream Mach numbers 0.1-0.2. Three-dimensional velocity components were measured using a 5-hole Pitot probe in the boundary layer. These measurements were used to quantify the production of streamwise vorticity and the magnitude of the reorientation term from the vorticity transport equation. The effect of Mach number, <span class="hlt">pressure</span> <span class="hlt">gradient</span>, operating voltage, and electrode length was then investigated for the PSVGs. The results indicate that the PSVGs could easily outperform the passive VGs and provide a suitable alternative for flow control.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhCS.821a2005G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhCS.821a2005G"><span>Non-<span class="hlt">Ideal</span> Compressible-Fluid Dynamics of Fast-Response <span class="hlt">Pressure</span> Probes for Unsteady Flow Measurements in Turbomachinery</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gori, G.; Molesini, P.; Persico, G.; Guardone, A.</p> <p>2017-03-01</p> <p>The dynamic response of <span class="hlt">pressure</span> probes for unsteady flow measurements in turbomachinery is investigated numerically for fluids operating in non-<span class="hlt">ideal</span> thermodynamic conditions, which are relevant for e.g. Organic Rankine Cycles (ORC) and super-critical CO2 applications. The step response of a fast-response <span class="hlt">pressure</span> probe is investigated numerically in order to assess the expected time response when operating in the non-<span class="hlt">ideal</span> fluid regime. Numerical simulations are carried out exploiting the Non-<span class="hlt">Ideal</span> Compressible Fluid-Dynamics (NICFD) solver embedded in the open-source fluid dynamics code SU2. The computational framework is assessed against available experimental data for air in dilute conditions. Then, polytropic <span class="hlt">ideal</span> gas (PIG), i.e. constant specific heats, and Peng-Robinson Stryjek-Vera (PRSV) models are applied to simulate the flow field within the probe operating with siloxane fluid octamethyltrisiloxane (MDM). The step responses are found to depend mainly on the speed of sound of the working fluid, indicating that molecular complexity plays a major role in determining the promptness of the measurement devices. According to the PRSV model, non-<span class="hlt">ideal</span> effects can increase the step response time with respect to the acoustic theory predictions. The fundamental derivative of gas-dynamic is confirmed to be the driving parameter for evaluating non-<span class="hlt">ideal</span> thermodynamic effects related to the dynamic calibration of fast-response aerodynamic <span class="hlt">pressure</span> probes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24861781','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24861781"><span>Constant <span class="hlt">pressure</span> mode extended simple <span class="hlt">gradient</span> liquid chromatography system for micro and nanocolumns.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Šesták, Jozef; Kahle, Vladislav</p> <p>2014-07-11</p> <p>Performing <span class="hlt">gradient</span> liquid chromatography at constant <span class="hlt">pressure</span> instead of constant flow rate has serious potential for shortening the analysis time and increasing the productivity of HPLC instruments that use <span class="hlt">gradient</span> methods. However, in the constant <span class="hlt">pressure</span> mode the decreasing column permeability during a long period of time negatively affects the repeatability of retention time. Thus a volume-based approach, in which the detector signal is plotted as a function of retention volume, must be taken into consideration. Traditional HPLC equipment, however, requires quite complex hardware and software modifications in order to work at constant <span class="hlt">pressure</span> and in the volume-based mode. In this short communication, a low cost and easily feasible <span class="hlt">pressure</span>-controlled extension of the previously described simple <span class="hlt">gradient</span> liquid chromatography platform is proposed. A test mixture of four nitro esters was separated by 10-60% (v/v) acetone/water <span class="hlt">gradient</span> and a high repeatability of retention volumes at 20MPa (RSD less than 0.45%) was realized. Separations were also performed at different values of <span class="hlt">pressure</span> (20, 25, and 31MPa), and only small variations of the retention volumes (up to 0.8%) were observed. In this particular case, the gain in the analysis speed of 7% compared to the constant flow mode was realized at a constant <span class="hlt">pressure</span>. Copyright © 2014 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28296135','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28296135"><span>Assessment of trans-aortic <span class="hlt">pressure</span> <span class="hlt">gradient</span> using a coronary <span class="hlt">pressure</span> wire in patients with mechanical aortic and mitral valve prostheses.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kherada, Nisharahmed; Brenes, Juan Carlos; Kini, Annapoorna S; Dangas, George D</p> <p>2017-03-15</p> <p>Accurate evaluation of trans-aortic valvular <span class="hlt">pressure</span> <span class="hlt">gradients</span> is challenging in cases where dual mechanical aortic and mitral valve prostheses are present. Non-invasive Doppler echocardiographic imaging has its limitations due to multiple geometric assumptions. Invasive measurement of trans-valvular <span class="hlt">gradients</span> with cardiac catheterization can provide further information in patients with two mechanical valves, where simultaneous <span class="hlt">pressure</span> measurements in the left ventricle and ascending aorta must be obtained. Obtaining access to the left ventricle via the mitral valve after a trans-septal puncture is not feasible in the case of a concomitant mechanical mitral valve, whereas left ventricular apical puncture technique is associated with high procedural risks. Retrograde crossing of a bileaflet mechanical aortic prosthesis with standard catheters is associated with the risk of catheter entrapment and acute valvular regurgitation. In these cases, the assessment of trans-valvular <span class="hlt">gradients</span> using a 0.014˝ diameter coronary <span class="hlt">pressure</span> wire technique has been described in a few case reports. We present the case of a 76-year-old female with rheumatic valvular heart disease who underwent mechanical aortic and mitral valve replacement in the past. She presented with decompensated heart failure and echocardiographic findings suggestive of elevated <span class="hlt">pressure</span> <span class="hlt">gradient</span> across the mechanical aortic valve prosthesis. The use of a high-fidelity 0.014˝ diameter coronary <span class="hlt">pressure</span> guidewire resulted in the detection of a normal trans-valvular <span class="hlt">pressure</span> <span class="hlt">gradient</span> across the mechanical aortic valve. This avoided a high-risk third redo valve surgery in our patient. © 2017 Wiley Periodicals, Inc. © 2017 Wiley Periodicals, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70179130','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70179130"><span>Barrier island breach evolution: Alongshore transport and bay-ocean <span class="hlt">pressure</span> <span class="hlt">gradient</span> interactions</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Safak, Ilgar; Warner, John C.; List, Jeffrey</p> <p>2016-01-01</p> <p>Physical processes controlling repeated openings and closures of a barrier island breach between a bay and the open ocean are studied using aerial photographs and atmospheric and hydrodynamic observations. The breach site is located on Pea Island along the Outer Banks, separating Pamlico Sound from the Atlantic Ocean. Wind direction was a major control on the <span class="hlt">pressure</span> <span class="hlt">gradients</span> between the bay and the ocean to drive flows that initiate or maintain the breach opening. Alongshore sediment flux was found to be a major contributor to breach closure. During the analysis period from 2011 to 2016, three hurricanes had major impacts on the breach. First, Hurricane Irene opened the breach with wind-driven flow from bay to ocean in August 2011. Hurricane Sandy in October 2012 quadrupled the channel width from <span class="hlt">pressure</span> <span class="hlt">gradient</span> flows due to water levels that were first higher on the ocean side and then higher on the bay side. The breach closed sometime in Spring 2013, most likely due to an event associated with strong alongshore sediment flux but minimal ocean-bay <span class="hlt">pressure</span> <span class="hlt">gradients</span>. Then, in July 2014, Hurricane Arthur briefly opened the breach again from the bay side, in a similar fashion to Irene. In summary, opening and closure of breaches are shown to follow a dynamic and episodic balance between along-channel <span class="hlt">pressure</span> <span class="hlt">gradient</span> driven flows and alongshore sediment fluxes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=cooking&pg=7&id=EJ921513','ERIC'); return false;" href="https://eric.ed.gov/?q=cooking&pg=7&id=EJ921513"><span>Cooking under <span class="hlt">Pressure</span>: Applying the <span class="hlt">Ideal</span> Gas Law in the Kitchen</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Chen, Ling; Anderson, Jennifer Y.; Wang, Diane R.</p> <p>2010-01-01</p> <p>This case study uses a daily cooking scenario to demonstrate how the boiling point of water is directly related to the external <span class="hlt">pressures</span> in order to reinforce the concepts of boiling and boiling point, apply <span class="hlt">ideal</span> gas law, and relate chemical reaction rates with temperatures. It also extends its teaching to autoclaves used to destroy…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29770413','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29770413"><span>Effect of <span class="hlt">pressure</span> <span class="hlt">gradient</span> and new phases for 1,3,5-trinitrohexahydro-s-triazine (RDX) under high <span class="hlt">pressures</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gao, Chan; Zhang, Xueyong; Zhang, Chuanchao; Sui, Zhilei; Hou, Meng; Dai, Rucheng; Wang, Zhongping; Zheng, Xianxu; Zhang, Zengming</p> <p>2018-05-17</p> <p>Herein, <span class="hlt">pressure</span>-induced phase transitions of RDX up to 50 GPa were systematically studied under different compression conditions. Precise phase transition points were obtained based on high-quality Raman spectra with small <span class="hlt">pressure</span> intervals. This favors the correctness of the theoretical formula for detonation and the design of a precision weapon. The experimental results indicated that α-RDX immediately transformed to γ-RDX at 3.5 GPa due to hydrostatic conditions and possible interaction between the penetrating helium and RDX, with helium gas as the <span class="hlt">pressure</span>-transmitting medium (PTM). Mapping of <span class="hlt">pressure</span> distribution in samples demonstrates that the <span class="hlt">pressure</span> <span class="hlt">gradient</span> is generated in the chamber and independent of other PTMs. The <span class="hlt">gradient</span> induced the first phase transition starts at 2.3 GPa and completed at 4.1 GPa. The larger <span class="hlt">pressure</span> <span class="hlt">gradient</span> promoted phase transition in advance under higher <span class="hlt">pressures</span>. Experimental results supported that there existed two conformers of AAI and AAE for γ-RDX, as proposed by another group. δ-RDX was considered to only occur in a hydrostatic environment around 18 GPa using helium as the PTM. This study confirms that δ-RDX is independent of PTM and exists under non-hydrostatic conditions. Evidence for a new phase (ζ) was found at about 28 GPa. These 4 phases have also been verified via XRD under high <span class="hlt">pressures</span>. In addition to this, another new phase (η) may exist above 38 GPa, and it needs to be further confirmed in the future. Moreover, all the phase transitions were reversible after the <span class="hlt">pressure</span> was released, and original α-RDX was always obtained at ambient <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012NucFu..52f3027P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012NucFu..52f3027P"><span><span class="hlt">Ideal</span> MHD stability and performance of ITER steady-state scenarios with ITBs</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Poli, F. M.; Kessel, C. E.; Chance, M. S.; Jardin, S. C.; Manickam, J.</p> <p>2012-06-01</p> <p>Non-inductive steady-state scenarios on ITER will need to operate with internal transport barriers (ITBs) in order to reach adequate fusion gain at typical currents of 9 MA. The large <span class="hlt">pressure</span> <span class="hlt">gradients</span> at the location of the internal barrier are conducive to the development of <span class="hlt">ideal</span> MHD instabilities that may limit the plasma performance and may lead to plasma disruptions. Fully non-inductive scenario simulations with five combinations of heating and current drive sources are presented in this work, with plasma currents in the range 7-10 MA. For each configuration the linear, <span class="hlt">ideal</span> MHD stability is analysed for variations of the Greenwald fraction and of the <span class="hlt">pressure</span> peaking factor around the operating point, aiming at defining an operational space for stable, steady-state operations at optimized performance. It is shown that plasmas with lower hybrid heating and current drive maintain the minimum safety factor above 1.5, which is desirable in steady-state operations to avoid neoclassical tearing modes. Operating with moderate ITBs at 2/3 of the minor radius, these plasmas have a minimum safety factor above 2, are <span class="hlt">ideal</span> MHD stable and reach Q ≳ 5 operating above the <span class="hlt">ideal</span> no-wall limit.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhCS1001a2020S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS1001a2020S"><span>Characterisation of minimal-span plane Couette turbulence with <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sekimoto, Atsushi; Atkinson, Callum; Soria, Julio</p> <p>2018-04-01</p> <p>The turbulence statistics and dynamics in the spanwise-minimal plane Couette flow with <span class="hlt">pressure</span> <span class="hlt">gradients</span>, so-called, Couette-Poiseuille (C-P) flow, are investigated using direct numerical simulation. The large-scale motion is limited in the spanwise box dimension as in the minimal-span channel turbulence of Flores & Jiménez (Phys. Fluids, vol. 22, 2010, 071704). The effect of the top wall, where normal <span class="hlt">pressure</span>-driven Poiseuille flow is realised, is distinguished from the events on the bottom wall, where the <span class="hlt">pressure</span> <span class="hlt">gradient</span> results in mild or almost-zero wall-shear stress. A proper scaling of turbulence statistics in minimal-span C-P flows is presented. Also the ‘shear-less’ wall-bounded turbulence, where the Corrsin shear parameter is very weak compared to normal wall-bounded turbulence, represents local separation, which is also observed as spanwise streaks of reversed flow in full-size plane C-P turbulence. The local separation is a multi-scale event, which grows up to the order of the channel height even in the minimal-span geometry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18089281','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18089281"><span>Relationships amongst body dissatisfaction, internalisation of the media body <span class="hlt">ideal</span> and perceived <span class="hlt">pressure</span> from media in adolescent girls and boys.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Knauss, Christine; Paxton, Susan J; Alsaker, Françoise D</p> <p>2007-12-01</p> <p>Sociocultural factors that underpin gender differences in body dissatisfaction have not frequently been explored. We examined the relative contribution of internalization of media body <span class="hlt">ideals</span> and perceived <span class="hlt">pressure</span> to achieve this <span class="hlt">ideal</span> in explaining body dissatisfaction in adolescent boys and girls. A sample of 819 boys and 791 girls completed measures of internalization of body <span class="hlt">ideals</span>, perceived <span class="hlt">pressure</span>, body mass index (BMI) and body dissatisfaction. As expected, girls showed higher body dissatisfaction, internalization and <span class="hlt">pressure</span> than boys. Internalization, <span class="hlt">pressure</span> and BMI contributed to the prediction of body dissatisfaction in boys and in girls although these variables explained less variance in body dissatisfaction in boys. In addition, for girls the strongest predictor of body dissatisfaction was internalization, whilst for boys the strongest predictor was <span class="hlt">pressure</span>. Differences in extent of internalization and <span class="hlt">pressure</span> may contribute to higher body dissatisfaction in girls than boys. These sociocultural factors may affect girls and boys differently.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26378495','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26378495"><span>Hand-Portable <span class="hlt">Gradient</span> Capillary Liquid Chromatography Pumping System.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sharma, Sonika; Plistil, Alex; Barnett, Hal E; Tolley, H Dennis; Farnsworth, Paul B; Stearns, Stanley D; Lee, Milton L</p> <p>2015-10-20</p> <p>In this work, a novel splitless nanoflow <span class="hlt">gradient</span> generator integrated with a stop-flow injector was developed and evaluated using an on-column UV-absorption detector. The <span class="hlt">gradient</span> pumping system consisted of two nanoflow pumps controlled by micro stepper motors, a mixer connected to a serpentine tube, and a high-<span class="hlt">pressure</span> valve. The <span class="hlt">gradient</span> system weighed only 4 kg (9 lbs) and could generate up to 55 MPa (8000 psi) <span class="hlt">pressure</span>. The system could operate using a 24 V DC battery and required 1.2 A for operation. The total volume capacity of the pump was 74 μL, and a sample volume of 60 nL could be injected. The system provided accurate nanoflow rates as low as 10 nL/min without employing a splitter, making it <span class="hlt">ideal</span> for capillary column use. The <span class="hlt">gradient</span> dwell volume was calculated to be 1.3 μL, which created a delay of approximately 4 min with a typical flow rate of 350 nL/min. <span class="hlt">Gradient</span> performance was evaluated for <span class="hlt">gradient</span> step accuracy, and excellent reproducibility was obtained in day-to-day experiments (RSD < 1.2%, n = 4). Linear <span class="hlt">gradient</span> reproducibility was tested by separating a three-component pesticide mixture on a poly(ethylene glycol) diacrylate (PEGDA) monolithic column. The retention time reproducibility was very good in run-to-run experiments (RSD < 1.42%, n = 4). Finally, excellent separation of five phenols was demonstrated using the nanoflow <span class="hlt">gradient</span> system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDA24008M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDA24008M"><span>Evaluation of the accuracy of the Rotating Parallel Ray Omnidirectional Integration for instantaneous <span class="hlt">pressure</span> reconstruction from the measured <span class="hlt">pressure</span> <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moreto, Jose; Liu, Xiaofeng</p> <p>2017-11-01</p> <p>The accuracy of the Rotating Parallel Ray omnidirectional integration for <span class="hlt">pressure</span> reconstruction from the measured <span class="hlt">pressure</span> <span class="hlt">gradient</span> (Liu et al., AIAA paper 2016-1049) is evaluated against both the Circular Virtual Boundary omnidirectional integration (Liu and Katz, 2006 and 2013) and the conventional Poisson equation approach. Dirichlet condition at one boundary point and Neumann condition at all other boundary points are applied to the Poisson solver. A direct numerical simulation database of isotropic turbulence flow (JHTDB), with a homogeneously distributed random noise added to the entire field of DNS <span class="hlt">pressure</span> <span class="hlt">gradient</span>, is used to assess the performance of the methods. The random noise, generated by the Matlab function Rand, has a magnitude varying randomly within the range of +/-40% of the maximum DNS <span class="hlt">pressure</span> <span class="hlt">gradient</span>. To account for the effect of the noise distribution pattern on the reconstructed <span class="hlt">pressure</span> accuracy, a total of 1000 different noise distributions achieved by using different random number seeds are involved in the evaluation. Final results after averaging the 1000 realizations show that the error of the reconstructed <span class="hlt">pressure</span> normalized by the DNS <span class="hlt">pressure</span> variation range is 0.15 +/-0.07 for the Poisson equation approach, 0.028 +/-0.003 for the Circular Virtual Boundary method and 0.027 +/-0.003 for the Rotating Parallel Ray method, indicating the robustness of the Rotating Parallel Ray method in <span class="hlt">pressure</span> reconstruction. Sponsor: The San Diego State University UGP program.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_1");'>1</a></li> <li><a href="#" onclick='return showDiv("page_2");'>2</a></li> <li class="active"><span>3</span></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_3 --> <div id="page_4" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_2");'>2</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li class="active"><span>4</span></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="61"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1433222','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1433222"><span>Effect of Valsalva's manoeuvre and hyoscinbutylbromide on the <span class="hlt">pressure</span> <span class="hlt">gradient</span> across the wall of oesophageal varices.</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Hosking, S W; Robinson, P; Johnson, A G</p> <p>1987-01-01</p> <p>To assess whether Valsalva's manoeuvre might cause variceal bleeding, 22 patients with oesophageal varices were studied. In 12 patients who received no previous treatment to their varices the median <span class="hlt">pressure</span> <span class="hlt">gradient</span> across the varix wall at rest was 19 (6-36) mmHg, and in 10 patients whose varices were thrombosed at their distal end the median <span class="hlt">pressure</span> <span class="hlt">gradient</span> in the proximal patent varix was 8 (1-6) mmHg. In untreated patients groups, the <span class="hlt">pressure</span> <span class="hlt">gradient</span> rose by 6-12 mmHg during Valsalva's manoeuvre in four patients, fell by 4-11 mmHg in five patients and was virtually unchanged in the remainder. These changes seem unlikely to cause variceal bleeding. Patients who repeated Valsalva's manoeuvre showed similar changes on each occasion. Six patients in the untreated group also received hyoscinbutylbromide 20 mg iv. No change was seen in the <span class="hlt">pressure</span> <span class="hlt">gradient</span> in five patients, suggesting that it is of little value in preventing variceal bleeding. PMID:3500098</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19750006501','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19750006501"><span>A model for jet-noise analysis using <span class="hlt">pressure-gradient</span> correlations on an imaginary cone</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Norum, T. D.</p> <p>1974-01-01</p> <p>The technique for determining the near and far acoustic field of a jet through measurements of <span class="hlt">pressure-gradient</span> correlations on an imaginary conical surface surrounding the jet is discussed. The necessary analytical developments are presented, and their feasibility is checked by using a point source as the sound generator. The distribution of the apparent sources on the cone, equivalent to the point source, is determined in terms of the <span class="hlt">pressure-gradient</span> correlations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890005997','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890005997"><span>The influence of free-stream turbulence on turbulent boundary layers with mild adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hoffmann, Jon A.</p> <p>1988-01-01</p> <p>The influence of near isotropic free-stream turbulence on the shape factors and skin friction coefficients of turbulent bounday layers is presented for the cases of zero and mild adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span>. With free-stream turbulence, improved fluid mixing occurs in boundary layers with adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> relative to the zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> condition, with the same free-stream turbulence intensity and length scale. Stronger boundary layers with lower shape factors occur as a result of a lower ratio of the integral scale of turbulence to the boundary layer thickness, and to vortex stretching of the turbulent eddies in the free stream, both of which act to improve the transmission of momentum from the free stream to the boundary layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890012674','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890012674"><span>The influence of free-stream turbulence on turbulent boundary layers with mild adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hoffmann, J. A.; Kassir, S. M.; Larwood, S. M.</p> <p>1989-01-01</p> <p>The influence of near isotropic free-stream turbulence on the shape factors and skin friction coefficients of turbulent boundary layers is presented for the cases of zero and mild adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span>. With free-stream turbulence, improved fluid mixing occurs in boundary layers with adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> relative to the zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> condition, with the same free-stream turbulence intensity and length scale. Stronger boundary layers with lower shape factors occur as a result of a lower ratio of the integral scale of turbulence to the boundary layer thickness, and to vortex stretching of the turbulent eddies in the free-stream, both of which act to improve the transmission of momentum from the free-stream to the boundary layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26774257','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26774257"><span>Severity assessment of intracranial large artery stenosis by <span class="hlt">pressure</span> <span class="hlt">gradient</span> measurements: A feasibility study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Han, Yun-Fei; Liu, Wen-Hua; Chen, Xiang-Liang; Xiong, Yun-Yun; Yin, Qin-; Xu, Ge-Lin; Zhu, Wu-Sheng; Zhang, Ren-Liang; Ma, Min-Min; Li, Min-; Dai, Qi-Liang; Sun, Wen-; Liu, De-Zhi; Duan, Li-Hui; Liu, Xin-Feng</p> <p>2016-08-01</p> <p>Fractional flow reserve (FFR)-guided revascularization strategy is popular in coronary intervention. However, the feasibility of assessing stenotic severity in intracranial large arteries using <span class="hlt">pressure</span> <span class="hlt">gradient</span> measurements still remains unclear. Between March 2013 and May 2014, 12 consecutive patients with intracranial large artery stenosis (including intracranial internal carotid artery, middle cerebral M1 segment, intracranial vertebral artery, and basilar artery) were enrolled in this study. The trans-stenotic <span class="hlt">pressure</span> <span class="hlt">gradient</span> was measured before and/or after percutaneous transluminal angioplasty and stenting (PTAS), and was then compared with percent diameter stenosis. A Pd /Pa cut-off of ≤0.70 was used to guide stenting of hemodynamically significant stenoses. The device-related and procedure-related serious adverse events and recurrent cerebral ischemic events were recorded. The target vessel could be reached in all cases. No technical complications occurred due to the specific study protocol. Excellent <span class="hlt">pressure</span> signals were obtained in all patients. For seven patients who performed PTAS, the mean pre-procedural <span class="hlt">pressure</span> <span class="hlt">gradient</span> decreased from 59.0 ± 17.2 to 13.3 ± 13.6 mm Hg after the procedure (P < 0.01). Only one patient who refused stenting experienced a TIA event in the ipsilateral MCA territory. No recurrent ischemic event was observed in other patients. Mean trans-stenotic <span class="hlt">pressure</span> <span class="hlt">gradients</span> can be safely and easily measured with a 0.014-inch fluid-filled guide wire in intracranial large arteries. © 2016 Wiley Periodicals, Inc. © 2016 Wiley Periodicals, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28029367','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28029367"><span>On the feasibility to conduct <span class="hlt">gradient</span> liquid chromatography separations in narrow-bore columns at <span class="hlt">pressures</span> up to 2000bar.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>De Pauw, Ruben; Swier, Tim; Degreef, Bart; Desmet, Gert; Broeckhoven, Ken</p> <p>2016-11-18</p> <p>The limits in operating <span class="hlt">pressures</span> are extended for narrow-bore columns in <span class="hlt">gradient</span> elution up to 2000bar. As the required pumps for these <span class="hlt">pressures</span> are incompatible with common chromatographic solvents and are not suitable to apply a mobile phase composition <span class="hlt">gradient</span>, a mobile phase delivery and injection system is described and experimentally validated which allows to use any possible chromatographic solvent in isocratic and <span class="hlt">gradient</span> elution. The mobile phase delivery and injection system also allows to perform multiple separations without the need to depressurize the column. This system consists out of 5 dual on/off valves and two large volume loops in which the <span class="hlt">gradient</span> and equilibration volume of initial mobile phase are loaded by a commercial liquid chromatography pump. The loops are then flushed toward the column at extreme <span class="hlt">pressures</span>. The mobile phase delivery and injection system is first evaluated in isocratic elution and shows a comparable performance to a state-of-the-art commercial flow-through-needle injector but with twice the <span class="hlt">pressure</span> rating. Distortion of the loaded <span class="hlt">gradient</span> by dispersion in the <span class="hlt">gradient</span> storage loop is studied. The effect of the most important parameters (such as flow rate, <span class="hlt">pressure</span> and <span class="hlt">gradient</span> steepness) is experimentally investigated. Different <span class="hlt">gradient</span> steepnesses and volumes can be applied at different flow rates and operating <span class="hlt">pressures</span> with a good repeatability. Due to the isobaric operation of the pumps, the <span class="hlt">gradient</span> is monitored in real-time by a mass flow meter installed at the detector outlet. The chromatograms are then converted from time to volume-base. A separation of a 19-compound sample is performed on a 300×2.1mm column at 1000bar and on a 600×2.1mm column at 2000bar. The peak capacity was found to increase from 141 to 199 and thus scales with L as is predicted by theory. This allows to conclude that the inlet <span class="hlt">pressure</span> for narrow-bore columns in <span class="hlt">gradient</span> elution can be increased up to 2000bar without fundamental</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5479527','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5479527"><span>Hemodynamic and metabolic characteristics associated with development of a right ventricular outflow tract <span class="hlt">pressure</span> <span class="hlt">gradient</span> during upright exercise</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>van Riel, Annelieke C. M. J.; Systrom, David M.; Oliveira, Rudolf K. F.; Landzberg, Michael J.; Mulder, Barbara J. M.; Bouma, Berto J.; Maron, Bradley A.; Shah, Amil M.; Waxman, Aaron B.</p> <p>2017-01-01</p> <p>Background We recently reported a novel observation that many patients with equal resting supine right ventricular(RV) and pulmonary artery(PA) systolic <span class="hlt">pressures</span> develop an RV outflow tract(RVOT) <span class="hlt">pressure</span> <span class="hlt">gradient</span> during upright exercise. The current work details the characteristics of patients who develop such an RVOT <span class="hlt">gradient</span>. Methods We studied 294 patients (59.7±15.5 years-old, 49% male) referred for clinical invasive cardiopulmonary exercise testing, who did not have a resting RVOT <span class="hlt">pressure</span> <span class="hlt">gradient</span> defined by the simultaneously measured peak-to-peak difference between RV and PA systolic <span class="hlt">pressures</span>. Results The magnitude of RVOT <span class="hlt">gradient</span> did not correspond to clinical or hemodynamic findings suggestive of right heart failure; rather, higher <span class="hlt">gradients</span> were associated with favorable exercise findings. The presence of a high peak RVOT <span class="hlt">gradient</span> (90th percentile, ≥33mmHg) was associated with male sex (70 vs. 46%, p = 0.01), younger age (43.6±17.7 vs. 61.8±13.9 years, p<0.001), lower peak right atrial <span class="hlt">pressure</span> (5 [3–7] vs. 8 [4–12]mmHg, p<0.001), higher peak heart rate (159±19 vs. 124±26 beats per minute, p<0.001), and higher peak cardiac index (8.3±2.3 vs. 5.7±1.9 L/min/m2, p<0.001). These associations persisted when treating peak RVOT as a continuous variable and after age and sex adjustment. At peak exercise, patients with a high exercise RVOT <span class="hlt">gradient</span> had both higher RV systolic <span class="hlt">pressure</span> (78±11 vs. 66±17 mmHg, p<0.001) and lower PA systolic <span class="hlt">pressure</span> (34±8 vs. 50±19 mmHg, p<0.001). Conclusions Development of a systolic RV-PA <span class="hlt">pressure</span> <span class="hlt">gradient</span> during upright exercise is not associated with an adverse hemodynamic exercise response and may represent a normal physiologic finding in aerobically fit young people. PMID:28636647</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29753461','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29753461"><span>Hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> after portal vein embolization: An accurate predictor of future liver remnant hypertrophy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mohkam, Kayvan; Rode, Agnès; Darnis, Benjamin; Manichon, Anne-Frédérique; Boussel, Loïc; Ducerf, Christian; Merle, Philippe; Lesurtel, Mickaël; Mabrut, Jean-Yves</p> <p>2018-05-09</p> <p>The impact of portal hemodynamic variations after portal vein embolization on liver regeneration remains unknown. We studied the correlation between the parameters of hepatic venous <span class="hlt">pressure</span> measured before and after portal vein embolization and future hypertrophy of the liver remnant after portal vein embolization. Between 2014 and 2017, we reviewed patients who were eligible for major hepatectomy and who had portal vein embolization. Patients had undergone simultaneous measurement of portal venous <span class="hlt">pressure</span> and hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> before and after portal vein embolization by direct puncture of portal vein and inferior vena cava. We assessed these parameters to predict future liver remnant hypertrophy. Twenty-six patients were included. After portal vein embolization, median portal venous <span class="hlt">pressure</span> (range) increased from 15 (9-24) to 19 (10-27) mm Hg and hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> increased from 5 (0-12) to 8 (0-14) mm Hg. Median future liver remnant volume (range) was 513 (299-933) mL before portal vein embolization versus 724 (499-1279) mL 3 weeks after portal vein embolization, representing a 35% (7.4-83.6) median hypertrophy. Post-portal vein embolization hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> was the most accurate parameter to predict failure of future liver remnant to reach a 30% hypertrophy (c-statistic: 0.882 [95% CI: 0.727-1.000], P < 0.001). A cut-off value of post-portal vein embolization hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> of 8 mm Hg showed a sensitivity of 91% (95% CI: 57%-99%), specificity of 80% (95% CI: 52%-96%), positive predictive value of 77% (95% CI: 46%-95%) and negative predictive value of 92.3% (95% CI: 64.0%-99.8%). On multivariate analysis, post-portal vein embolization hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> and previous chemotherapy were identified as predictors of impaired future liver remnant hypertrophy. Post-portal vein embolization hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> is a simple and reproducible tool which accurately predicts future</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDM28006G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDM28006G"><span>DNS of a non-equilibrium adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> turbulent boundary layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gungor, Taygun R.; Gungor, Ayse G.; Maciel, Yvan; Simens, Mark P.</p> <p>2017-11-01</p> <p>A new direct numerical simulation (DNS) dataset of a non-equilibrium adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> (APG) turbulent boundary layer (TBL) that evolves from a zero-<span class="hlt">pressure-gradient</span> (ZPG) TBL to a TBL which is very close to separation at Reθ is around 8200 is presented. There are two simulations running together in the DNS computational setup. The APG TBL spans Reθ = 1476 - 8276 . Mean velocity results do not satisfy the log law as the defect in the velocity increases. The production and the Reynolds stress peak are observed around y /δ* = 1 after the flow is evolved up to a certain point. The new dataset is compared with other datasets in terms of mean values, Reynolds stresses and turbulent kinetic energy budgets and using this comparison scaling study is performed. Funded by in part by ITU-AYP and NSERC of Canada.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSM13B2386G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM13B2386G"><span>Non-<span class="hlt">ideal</span> energy conversion during asymmetric magnetic reconnection with a moderate guide field</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Genestreti, K. J.; Varsani, A.; Hesse, M.; Torbert, R. B.; Burch, J.; Cassak, P.; Ergun, R.; Phan, T.; Nakamura, R.; Giles, B. L.; Schwartz, S. J.; Wang, S.; Toledo Redondo, S.; Hwang, K. J.; Laignel, B.; Escoubet, C. P.; Fear, R. C.; Khotyaintsev, Y. V.</p> <p>2017-12-01</p> <p>Using data from NASA's Magnetospheric Multiscale (MMS) mission, we investigate the local (in time and space) rate of work done by the non-<span class="hlt">ideal</span> electric field on the plasma during a crossing through the magnetopause reconnection region. The four MMS spacecraft were in a tight tetrahedral formation ( 7 km separation) and observed several ion and electron-scale signatures of asymmetric reconnection, one of which was J.E' (=J.(E+vexB))>0. The data indicate that the magnetic field was expending energy both (1) near the magnetosphere-side separator, where the current was carried by counter-streaming electrons with crescent-shaped velocity distribution functions, and (2) near the magnetic X-point, where the current was carried by accelerated inflowing magnetosheath electrons moving against the guide field. Near the X-point, the current-aligned portion of the non-<span class="hlt">ideal</span> electric field is largely a result of electron <span class="hlt">pressure</span> divergence. We further investigate the <span class="hlt">pressure</span> tensor divergence, separating the components from in and out-of-the-plane <span class="hlt">gradients</span> as well as gyrotropic and non-gyrotropic <span class="hlt">pressures</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1713547P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1713547P"><span>The Phase Rule in a System Subject to a <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Podladchikov, Yuri; Connolly, James; Powell, Roger; Aardvark, Alberto</p> <p>2015-04-01</p> <p>It can be shown by diligent application of Lagrange's method of undetermined multipliers that the phase rule in a system subject to a <span class="hlt">pressure</span> <span class="hlt">gradient</span> is: � + 赑 ≥ ρ. We explore the consequence of this important relationship for natural systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19750020309','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19750020309"><span><span class="hlt">Pressure</span> <span class="hlt">gradient</span> effects on heat transfer to reusable surface insulation tile-array gaps</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Throckmorton, D. A.</p> <p>1975-01-01</p> <p>An experimental investigation was performed to determine the effect of <span class="hlt">pressure</span> <span class="hlt">gradient</span> on the heat transfer within space shuttle reusable surface insulation (RSI) tile-array gaps under thick, turbulent boundary-layer conditions. Heat-transfer and <span class="hlt">pressure</span> measurements were obtained on a curved array of full-scale simulated RSI tiles in a tunnel-wall boundary layer at a nominal free-stream Mach number and free-stream Reynolds numbers. Transverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> of varying degree were induced over the model surface by rotating the curved array with respect to the flow. Definition of the tunnel-wall boundary-layer flow was obtained by measurement of boundary-layer pitot <span class="hlt">pressure</span> profiles, wall <span class="hlt">pressure</span>, and heat transfer. Flat-plate heat-transfer data were correlated and a method was derived for prediction of heat transfer to a smooth curved surface in the highly three-dimensional tunnel-wall boundary-layer flow. <span class="hlt">Pressure</span> on the floor of the RSI tile-array gap followed the trends of the external surface <span class="hlt">pressure</span>. Heat transfer to the surface immediately downstream of a transverse gap is higher than that for a smooth surface at the same location. Heating to the wall of a transverse gap, and immediately downstream of it, at its intersection with a longitudinal gap is significantly greater than that for the simple transverse gap.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930040417&hterms=curvature&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dcurvature','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930040417&hterms=curvature&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dcurvature"><span>Turbulent boundary layers subjected to multiple curvatures and <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bandyopadhyay, Promode R.; Ahmed, Anwar</p> <p>1993-01-01</p> <p>The effects of abruptly applied cycles of curvatures and <span class="hlt">pressure</span> <span class="hlt">gradients</span> on turbulent boundary layers are examined experimentally. Two two-dimensional curved test surfaces are considered: one has a sequence of concave and convex longitudinal surface curvatures and the other has a sequence of convex and concave curvatures. The choice of the curvature sequences were motivated by a desire to study the asymmetric response of turbulent boundary layers to convex and concave curvatures. The relaxation of a boundary layer from the effects of these two opposite sequences has been compared. The effect of the accompaying sequences of <span class="hlt">pressure</span> <span class="hlt">gradient</span> has also been examined but the effect of curvature dominates. The growth of internal layers at the curvature junctions have been studied. Measurements of the Gortler and corner vortex systems have been made. The boundary layer recovering from the sequence of concave to convex curvature has a sustained lower skin friction level than in that recovering from the sequence of convex to concave curvature. The amplification and suppression of turbulence due to the curvature sequences have also been studied.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940028441','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940028441"><span>Modification of the MML turbulence model for adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> flows. M.S. Thesis - Akron Univ., 1993</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Conley, Julianne M.</p> <p>1994-01-01</p> <p>Computational fluid dynamics is being used increasingly to predict flows for aerospace propulsion applications, yet there is still a need for an easy to use, computationally inexpensive turbulence model capable of accurately predicting a wide range of turbulent flows. The Baldwin-Lomax model is the most widely used algebraic model, even though it has known difficulties calculating flows with strong adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> and large regions of separation. The modified mixing length model (MML) was developed specifically to handle the separation which occurs on airfoils and has given significantly better results than the Baldwin-Lomax model. The success of these calculations warrants further evaluation and development of MML. The objective of this work was to evaluate the performance of MML for zero and adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> flows, and modify it as needed. The Proteus Navier-Stokes code was used for this study and all results were compared with experimental data and with calculations made using the Baldwin-Lomax algebraic model, which is currently available in Proteus. The MML model was first evaluated for zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> flow over a flat plate, then modified to produce the proper boundary layer growth. Additional modifications, based on experimental data for three adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> flows, were also implemented. The adapted model, called MMLPG (modified mixing length model for <span class="hlt">pressure</span> <span class="hlt">gradient</span> flows), was then evaluated for a typical propulsion flow problem, flow through a transonic diffuser. Three cases were examined: flow with no shock, a weak shock and a strong shock. The results of these calculations indicate that the objectives of this study have been met. Overall, MMLPG is capable of accurately predicting the adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> flows examined in this study, giving generally better agreement with experimental data than the Baldwin-Lomax model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27350150','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27350150"><span>Inhaled Beta Agonist Bronchodilator Does Not Affect Trans-diaphragmatic <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> but Decreases Lower Esophageal Sphincter Retention <span class="hlt">Pressure</span> in Patients with Chronic Obstructive Pulmonary Disease (COPD) and Gastroesophageal Reflux Disease (GERD).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Del Grande, Leonardo M; Herbella, Fernando A M; Bigatao, Amilcar M; Jardim, Jose R; Patti, Marco G</p> <p>2016-10-01</p> <p>Chronic obstructive pulmonary disease (COPD) patients have a high incidence of gastroesophageal reflux disease (GERD) whose pathophysiology seems to be linked to an increased trans-diaphragmatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> and not to a defective esophagogastric barrier. Inhaled beta agonist bronchodilators are a common therapy used by patients with COPD. This drug knowingly not only leads to a decrease in the lower esophageal sphincter (LES) resting <span class="hlt">pressure</span>, favoring GERD, but also may improve ventilatory parameters, therefore preventing GERD. This study aims to evaluate the effect of inhaled beta agonist bronchodilators on the trans-diaphragmatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> and the esophagogastric barrier. We studied 21 patients (mean age 67 years, 57 % males) with COPD and GERD. All patients underwent high-resolution manometry and esophageal pH monitoring. Abdominal and thoracic <span class="hlt">pressure</span>, trans-diaphragmatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> (abdominal-thoracic <span class="hlt">pressure</span>), and the LES retention <span class="hlt">pressure</span> (LES basal <span class="hlt">pressure</span>-transdiaphragmatic <span class="hlt">gradient</span>) were measured before and 5 min after inhaling beta agonist bronchodilators. The administration of inhaled beta agonist bronchodilators leads to the following: (a) a simultaneous increase in abdominal and thoracic <span class="hlt">pressure</span> not affecting the trans-diaphragmatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> and (b) a decrease in the LES resting <span class="hlt">pressure</span> with a reduction of the LES retention <span class="hlt">pressure</span>. In conclusion, inhaled beta agonist bronchodilators not only increase the thoracic <span class="hlt">pressure</span> but also lead to an increased abdominal <span class="hlt">pressure</span> favoring GERD by affecting the esophagogastric barrier.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040141463&hterms=left&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dleft','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040141463&hterms=left&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dleft"><span>Doppler echo evaluation of pulmonary venous-left atrial <span class="hlt">pressure</span> <span class="hlt">gradients</span>: human and numerical model studies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Firstenberg, M. S.; Greenberg, N. L.; Smedira, N. G.; Prior, D. L.; Scalia, G. M.; Thomas, J. D.; Garcia, M. J.</p> <p>2000-01-01</p> <p>The simplified Bernoulli equation relates fluid convective energy derived from flow velocities to a <span class="hlt">pressure</span> <span class="hlt">gradient</span> and is commonly used in clinical echocardiography to determine <span class="hlt">pressure</span> differences across stenotic orifices. Its application to pulmonary venous flow has not been described in humans. Twelve patients undergoing cardiac surgery had simultaneous high-fidelity pulmonary venous and left atrial <span class="hlt">pressure</span> measurements and pulmonary venous pulsed Doppler echocardiography performed. Convective <span class="hlt">gradients</span> for the systolic (S), diastolic (D), and atrial reversal (AR) phases of pulmonary venous flow were determined using the simplified Bernoulli equation and correlated with measured actual <span class="hlt">pressure</span> differences. A linear relationship was observed between the convective (y) and actual (x) <span class="hlt">pressure</span> differences for the S (y = 0.23x + 0.0074, r = 0.82) and D (y = 0.22x + 0.092, r = 0.81) waves, but not for the AR wave (y = 0. 030x + 0.13, r = 0.10). Numerical modeling resulted in similar slopes for the S (y = 0.200x - 0.127, r = 0.97), D (y = 0.247x - 0. 354, r = 0.99), and AR (y = 0.087x - 0.083, r = 0.96) waves. Consistent with numerical modeling, the convective term strongly correlates with but significantly underestimates actual <span class="hlt">gradient</span> because of large inertial forces.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/10924058','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/10924058"><span>Doppler echo evaluation of pulmonary venous-left atrial <span class="hlt">pressure</span> <span class="hlt">gradients</span>: human and numerical model studies.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Firstenberg, M S; Greenberg, N L; Smedira, N G; Prior, D L; Scalia, G M; Thomas, J D; Garcia, M J</p> <p>2000-08-01</p> <p>The simplified Bernoulli equation relates fluid convective energy derived from flow velocities to a <span class="hlt">pressure</span> <span class="hlt">gradient</span> and is commonly used in clinical echocardiography to determine <span class="hlt">pressure</span> differences across stenotic orifices. Its application to pulmonary venous flow has not been described in humans. Twelve patients undergoing cardiac surgery had simultaneous high-fidelity pulmonary venous and left atrial <span class="hlt">pressure</span> measurements and pulmonary venous pulsed Doppler echocardiography performed. Convective <span class="hlt">gradients</span> for the systolic (S), diastolic (D), and atrial reversal (AR) phases of pulmonary venous flow were determined using the simplified Bernoulli equation and correlated with measured actual <span class="hlt">pressure</span> differences. A linear relationship was observed between the convective (y) and actual (x) <span class="hlt">pressure</span> differences for the S (y = 0.23x + 0.0074, r = 0.82) and D (y = 0.22x + 0.092, r = 0.81) waves, but not for the AR wave (y = 0. 030x + 0.13, r = 0.10). Numerical modeling resulted in similar slopes for the S (y = 0.200x - 0.127, r = 0.97), D (y = 0.247x - 0. 354, r = 0.99), and AR (y = 0.087x - 0.083, r = 0.96) waves. Consistent with numerical modeling, the convective term strongly correlates with but significantly underestimates actual <span class="hlt">gradient</span> because of large inertial forces.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDL26012K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDL26012K"><span>Characterization of Rare Reverse Flow Events in Adverse <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> Turbulent Boundary Layers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kaehler, Christian J.; Bross, Matthew; Fuchs, Thomas</p> <p>2017-11-01</p> <p>Time-resolved tomographic flow fields measured in the viscous sublayer region of a turbulent boundary layer subjected to an adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> (APG) are examined with the aim to resolve and characterize reverse flow events at Reτ = 5000. The fields were measured using a novel high resolution tomographic particle tracking technique. It is shown that this technique is able to fully resolve mean and time dependent features of the complex three-dimensional flow with high accuracy down to very near-wall distances ( 10 μm). From time resolved Lagrangian particle trajectories, statistical information as well as instantaneous topological features of near-wall flow events are deduced. Similar to the zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> case (ZPG), it was found that individual events with reverse flow components still occur relatively rarely under the action of the <span class="hlt">pressure</span> <span class="hlt">gradient</span> investigated here. However, reverse flow events comprised of many individual events, are shown to appear in relatively organized groupings in both spanwise and streamise directions. Furthermore, instantaneous measurements of reverse flow events show that these events are associated with the motion of low-momentum streaks in the near-wall region. This work is supported by the Priority Programme SPP 1881 Turbulent Superstructures and the individual project Grant KA1808/8-2 of the Deutsche Forschungsgemeinschaft.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017OcMod.116....1E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017OcMod.116....1E"><span>High-order accurate finite-volume formulations for the <span class="hlt">pressure</span> <span class="hlt">gradient</span> force in layered ocean models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Engwirda, Darren; Kelley, Maxwell; Marshall, John</p> <p>2017-08-01</p> <p>Discretisation of the horizontal <span class="hlt">pressure</span> <span class="hlt">gradient</span> force in layered ocean models is a challenging task, with non-trivial interactions between the thermodynamics of the fluid and the geometry of the layers often leading to numerical difficulties. We present two new finite-volume schemes for the <span class="hlt">pressure</span> <span class="hlt">gradient</span> operator designed to address these issues. In each case, the horizontal acceleration is computed as an integration of the contact <span class="hlt">pressure</span> force that acts along the perimeter of an associated momentum control-volume. A pair of new schemes are developed by exploring different control-volume geometries. Non-linearities in the underlying equation-of-state definitions and thermodynamic profiles are treated using a high-order accurate numerical integration framework, designed to preserve hydrostatic balance in a non-linear manner. Numerical experiments show that the new methods achieve high levels of consistency, maintaining hydrostatic and thermobaric equilibrium in the presence of strongly-sloping layer geometries, non-linear equations-of-state and non-uniform vertical stratification profiles. These results suggest that the new <span class="hlt">pressure</span> <span class="hlt">gradient</span> formulations may be appropriate for general circulation models that employ hybrid vertical coordinates and/or terrain-following representations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27986288','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27986288"><span>A practical approach for predicting retention time shifts due to <span class="hlt">pressure</span> and temperature <span class="hlt">gradients</span> in ultra-high-<span class="hlt">pressure</span> liquid chromatography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Åsberg, Dennis; Chutkowski, Marcin; Leśko, Marek; Samuelsson, Jörgen; Kaczmarski, Krzysztof; Fornstedt, Torgny</p> <p>2017-01-06</p> <p>Large <span class="hlt">pressure</span> <span class="hlt">gradients</span> are generated in ultra-high-<span class="hlt">pressure</span> liquid chromatography (UHPLC) using sub-2μm particles causing significant temperature <span class="hlt">gradients</span> over the column due to viscous heating. These <span class="hlt">pressure</span> and temperature <span class="hlt">gradients</span> affect retention and ultimately result in important selectivity shifts. In this study, we developed an approach for predicting the retention time shifts due to these <span class="hlt">gradients</span>. The approach is presented as a step-by-step procedure and it is based on empirical linear relationships describing how retention varies as a function of temperature and <span class="hlt">pressure</span> and how the average column temperature increases with the flow rate. It requires only four experiments on standard equipment, is based on straightforward calculations, and is therefore easy to use in method development. The approach was rigorously validated against experimental data obtained with a quality control method for the active pharmaceutical ingredient omeprazole. The accuracy of retention time predictions was very good with relative errors always less than 1% and in many cases around 0.5% (n=32). Selectivity shifts observed between omeprazole and the related impurities when changing the flow rate could also be accurately predicted resulting in good estimates of the resolution between critical peak pairs. The approximations which the presented approach are based on were all justified. The retention factor as a function of <span class="hlt">pressure</span> and temperature was studied in an experimental design while the temperature distribution in the column was obtained by solving the fundamental heat and mass balance equations for the different experimental conditions. We strongly believe that this approach is sufficiently accurate and experimentally feasible for this separation to be a valuable tool when developing a UHPLC method. After further validation with other separation systems, it could become a useful approach in UHPLC method development, especially in the pharmaceutical industry where</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_2");'>2</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li class="active"><span>4</span></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_4 --> <div id="page_5" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li class="active"><span>5</span></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="81"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26688273','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26688273"><span>Perceived social <span class="hlt">pressures</span> and the internalization of the mesomorphic <span class="hlt">ideal</span>: The role of drive for muscularity and autonomy in physically active men.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Edwards, Christian; Tod, David; Molnar, Gyozo; Markland, David</p> <p>2016-03-01</p> <p>We examined if there were both direct and indirect relationships (via the drive for muscularity) between the perceived <span class="hlt">pressure</span> to be muscular and internalization of the mesomorphic <span class="hlt">ideal</span>, and if autonomy moderates these relationships in physically active men. A sample of 330 men, who were undergraduate students studying sport, completed the Behavioral Regulation in Exercise Questionnaire-2, the Mesomorphic <span class="hlt">Ideal</span> Internalization subscale of the revised male version Sociocultural Attitudes Toward Appearance Questionnaire, the Perceived Sociocultural <span class="hlt">Pressure</span> Scale-Modified, and the Drive for Muscularity Scale Attitudes subscale. Perceived <span class="hlt">pressure</span> predicted internalization directly, and indirectly through the drive for muscularity. The direct relationship between <span class="hlt">pressure</span> and internalization was weaker under higher levels of autonomy. The indirect path, via drive for muscularity, was stronger under higher levels of autonomy. These results provide insights into why men vary in the degree to which they internalize <span class="hlt">pressure</span> to develop a mesomorphic <span class="hlt">ideal</span>, supporting further examination of autonomy. Copyright © 2015 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930092289','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930092289"><span>Similar solutions for the compressible laminar boundary layer with heat transfer and <span class="hlt">pressure</span> <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cohen, Clarence B; Reshotko, Eli</p> <p>1956-01-01</p> <p>Stewartson's transformation is applied to the laminar compressible boundary-layer equations and the requirement of similarity is introduced, resulting in a set of ordinary nonlinear differential equations previously quoted by Stewartson, but unsolved. The requirements of the system are Prandtl number of 1.0, linear viscosity-temperature relation across the boundary layer, an isothermal surface, and the particular distributions of free-stream velocity consistent with similar solutions. This system admits axial <span class="hlt">pressure</span> <span class="hlt">gradients</span> of arbitrary magnitude, heat flux normal to the surface, and arbitrary Mach numbers. The system of differential equations is transformed to integral system, with the velocity ratio as the independent variable. For this system, solutions are found by digital computation for <span class="hlt">pressure</span> <span class="hlt">gradients</span> varying from that causing separation to the infinitely favorable <span class="hlt">gradient</span> and for wall temperatures from absolute zero to twice the free-stream stagnation temperature. Some solutions for separated flows are also presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014APS..DFDL27002P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014APS..DFDL27002P"><span>New Models for Velocity/<span class="hlt">Pressure-Gradient</span> Correlations in Turbulent Boundary Layers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Poroseva, Svetlana; Murman, Scott</p> <p>2014-11-01</p> <p>To improve the performance of Reynolds-Averaged Navier-Stokes (RANS) turbulence models, one has to improve the accuracy of models for three physical processes: turbulent diffusion, interaction of turbulent <span class="hlt">pressure</span> and velocity fluctuation fields, and dissipative processes. The accuracy of modeling the turbulent diffusion depends on the order of a statistical closure chosen as a basis for a RANS model. When the Gram-Charlier series expansions for the velocity correlations are used to close the set of RANS equations, no assumption on Gaussian turbulence is invoked and no unknown model coefficients are introduced into the modeled equations. In such a way, this closure procedure reduces the modeling uncertainty of fourth-order RANS (FORANS) closures. Experimental and direct numerical simulation data confirmed the validity of using the Gram-Charlier series expansions in various flows including boundary layers. We will address modeling the velocity/<span class="hlt">pressure-gradient</span> correlations. New linear models will be introduced for the second- and higher-order correlations applicable to two-dimensional incompressible wall-bounded flows. Results of models' validation with DNS data in a channel flow and in a zero-<span class="hlt">pressure</span> <span class="hlt">gradient</span> boundary layer over a flat plate will be demonstrated. A part of the material is based upon work supported by NASA under award NNX12AJ61A.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/9277520','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/9277520"><span>Protein osmotic <span class="hlt">pressure</span> <span class="hlt">gradients</span> and microvascular reflection coefficients.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Drake, R E; Dhother, S; Teague, R A; Gabel, J C</p> <p>1997-08-01</p> <p>Microvascular membranes are heteroporous, so the mean osmotic reflection coefficient for a microvascular membrane (sigma d) is a function of the reflection coefficient for each pore. Investigators have derived equations for sigma d based on the assumption that the protein osmotic <span class="hlt">pressure</span> <span class="hlt">gradient</span> across the membrane (delta II) does not vary from pore to pore. However, for most microvascular membranes, delta II probably does vary from pore to pore. In this study, we derived a new equation for sigma d. According to our equation, pore-to-pore differences in delta II increase the effect of small pores and decrease the effect of large pores on the overall membrane osmotic reflection coefficient. Thus sigma d for a heteroporous membrane may be much higher than previously derived equations indicate. Furthermore, pore-to-pore delta II differences increase the effect of plasma protein osmotic <span class="hlt">pressure</span> to oppose microvascular fluid filtration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3913518','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3913518"><span>Experimental Study on the Flow Regimes and <span class="hlt">Pressure</span> <span class="hlt">Gradients</span> of Air-Oil-Water Three-Phase Flow in Horizontal Pipes</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Al-Hadhrami, Luai M.; Shaahid, S. M.; Tunde, Lukman O.; Al-Sarkhi, A.</p> <p>2014-01-01</p> <p>An experimental investigation has been carried out to study the flow regimes and <span class="hlt">pressure</span> <span class="hlt">gradients</span> of air-oil-water three-phase flows in 2.25 ID horizontal pipe at different flow conditions. The effects of water cuts, liquid and gas velocities on flow patterns and <span class="hlt">pressure</span> <span class="hlt">gradients</span> have been studied. The experiments have been conducted at 20°C using low viscosity Safrasol D80 oil, tap water and air. Superficial water and oil velocities were varied from 0.3 m/s to 3 m/s and air velocity varied from 0.29 m/s to 52.5 m/s to cover wide range of flow patterns. The experiments were performed for 10% to 90% water cuts. The flow patterns were observed and recorded using high speed video camera while the <span class="hlt">pressure</span> drops were measured using <span class="hlt">pressure</span> transducers and U-tube manometers. The flow patterns show strong dependence on water fraction, gas velocities, and liquid velocities. The observed flow patterns are stratified (smooth and wavy), elongated bubble, slug, dispersed bubble, and annular flow patterns. The <span class="hlt">pressure</span> <span class="hlt">gradients</span> have been found to increase with the increase in gas flow rates. Also, for a given superficial gas velocity, the <span class="hlt">pressure</span> <span class="hlt">gradients</span> increased with the increase in the superficial liquid velocity. The <span class="hlt">pressure</span> <span class="hlt">gradient</span> first increases and then decreases with increasing water cut. In general, phase inversion was observed with increase in the water cut. The experimental results have been compared with the existing unified Model and a good agreement has been noticed. PMID:24523645</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24523645','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24523645"><span>Experimental study on the flow regimes and <span class="hlt">pressure</span> <span class="hlt">gradients</span> of air-oil-water three-phase flow in horizontal pipes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Al-Hadhrami, Luai M; Shaahid, S M; Tunde, Lukman O; Al-Sarkhi, A</p> <p>2014-01-01</p> <p>An experimental investigation has been carried out to study the flow regimes and <span class="hlt">pressure</span> <span class="hlt">gradients</span> of air-oil-water three-phase flows in 2.25 ID horizontal pipe at different flow conditions. The effects of water cuts, liquid and gas velocities on flow patterns and <span class="hlt">pressure</span> <span class="hlt">gradients</span> have been studied. The experiments have been conducted at 20 °C using low viscosity Safrasol D80 oil, tap water and air. Superficial water and oil velocities were varied from 0.3 m/s to 3 m/s and air velocity varied from 0.29 m/s to 52.5 m/s to cover wide range of flow patterns. The experiments were performed for 10% to 90% water cuts. The flow patterns were observed and recorded using high speed video camera while the <span class="hlt">pressure</span> drops were measured using <span class="hlt">pressure</span> transducers and U-tube manometers. The flow patterns show strong dependence on water fraction, gas velocities, and liquid velocities. The observed flow patterns are stratified (smooth and wavy), elongated bubble, slug, dispersed bubble, and annular flow patterns. The <span class="hlt">pressure</span> <span class="hlt">gradients</span> have been found to increase with the increase in gas flow rates. Also, for a given superficial gas velocity, the <span class="hlt">pressure</span> <span class="hlt">gradients</span> increased with the increase in the superficial liquid velocity. The <span class="hlt">pressure</span> <span class="hlt">gradient</span> first increases and then decreases with increasing water cut. In general, phase inversion was observed with increase in the water cut. The experimental results have been compared with the existing unified Model and a good agreement has been noticed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19810018494','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19810018494"><span>Radio jet refraction in galactic atmospheres with static <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Henriksen, R. N.; Vallee, J. P.; Bridle, A. H.</p> <p>1981-01-01</p> <p>A theory of double radio sources which have a 'Z' or 'S' morphology is proposed, based on the refraction of radio jets in the extended atmosphere of an elliptical galaxy. The model describes a collimated jet of supersonic material bending self-consistently under the influence of external static <span class="hlt">pressure</span> <span class="hlt">gradients</span>. Gravity and magnetic fields are neglected in the simplest case except insofar as they determine the static <span class="hlt">pressure</span> distribution. The calculation is a straightforward extension of a method used to calculate a ram-<span class="hlt">pressure</span> model for twin radio trails ('C' morphology). It may also be described as a continuous-jet version of a buoyancy model proposed in 1973. The model has the added virtue of invoking a galactic atmosphere similar to those already indicated by X-ray measurements of some other radio galaxies and by models for the collimation of other radio jets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24370000','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24370000"><span>Very high <span class="hlt">pressure</span> liquid chromatography using core-shell particles: quantitative analysis of fast <span class="hlt">gradient</span> separations without post-run times.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Stankovich, Joseph J; Gritti, Fabrice; Stevenson, Paul G; Beaver, Lois A; Guiochon, Georges</p> <p>2014-01-17</p> <p>Five methods for controlling the mobile phase flow rate for <span class="hlt">gradient</span> elution analyses using very high <span class="hlt">pressure</span> liquid chromatography (VHPLC) were tested to determine thermal stability of the column during rapid <span class="hlt">gradient</span> separations. To obtain rapid separations, instruments are operated at high flow rates and high inlet <span class="hlt">pressure</span> leading to uneven thermal effects across columns and additional time needed to restore thermal equilibrium between successive analyses. The purpose of this study is to investigate means to minimize thermal instability and obtain reliable results by measuring the reproducibility of the results of six replicate <span class="hlt">gradient</span> separations of a nine component RPLC standard mixture under various experimental conditions with no post-run times. <span class="hlt">Gradient</span> separations under different conditions were performed: constant flow rates, two sets of constant <span class="hlt">pressure</span> operation, programmed flow constant <span class="hlt">pressure</span> operation, and conditions which theoretically should yield a constant net heat loss at the column's wall. The results show that using constant flow rates, programmed flow constant <span class="hlt">pressures</span>, and constant heat loss at the column's wall all provide reproducible separations. However, performing separations using a high constant <span class="hlt">pressure</span> with programmed flow reduces the analysis time by 16% compared to constant flow rate methods. For the constant flow rate, programmed flow constant <span class="hlt">pressure</span>, and constant wall heat experiments no equilibration time (post-run time) was required to obtain highly reproducible data. Copyright © 2013 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/8149707','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/8149707"><span>Assessment of coronary artery stenosis <span class="hlt">pressure</span> <span class="hlt">gradient</span> by quantitative coronary arteriography in patients with coronary artery disease.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Atar, D; Ramanujam, P S; Saunamäki, K; Haunsø, S</p> <p>1994-01-01</p> <p>The aim of the study described here was to correlate coronary artery (CA) stenosis <span class="hlt">pressure</span> <span class="hlt">gradients</span> calculated by quantitative coronary arteriography (QCA) to invasively measured transstenotic <span class="hlt">pressure</span> drops in patients with anginal symptoms and with known or suspected coronary artery disease. Furthermore, the known mathematical models are improved by introducing (1) <span class="hlt">pressure</span> catheter-corrected minimal stenosis area, (2) modification of flow assumptions, and (3) stenosis exit angle. Included in the study were 45 patients with 61 stenoses. The visually estimated CA lesion severity in these non-complex stenoses was in the equivocal range of 40-70%. All measurements were performed after intracoronary administration of nifedipine and nitroglycerin. Stenosis dimensions were assessed from magnified cinefilms, using hand-held calipers. Highly significant overall correlation was found between measured and calculated <span class="hlt">pressure</span> <span class="hlt">gradients</span> with correction for the impact of the intracoronary catheter (P < 0.00001, r = 0.84). In particular, a substantial number of stenoses with haemodynamically-insignificant <span class="hlt">pressure</span> <span class="hlt">gradients</span> were identified by hydrodynamic calculations. In conclusion, the great majority of the coronary artery stenoses could be classified reliably by QCA as being haemodynamically insignificant or significant, respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29761086','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29761086"><span>Aortic-Brachial Pulse Wave Velocity Ratio: A Measure of Arterial Stiffness <span class="hlt">Gradient</span> Not Affected by Mean Arterial <span class="hlt">Pressure</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fortier, Catherine; Desjardins, Marie-Pier; Agharazii, Mohsen</p> <p>2018-03-01</p> <p>Aortic stiffness, measured by carotid-femoral pulse wave velocity (cf-PWV), is used for the prediction of cardiovascular risk. This mini-review describes the nonlinear relationship between cf-PWV and operational blood <span class="hlt">pressure</span>, presents the proposed methods to adjust for this relationship, and discusses a potential place for aortic-brachial PWV ratio (a measure of arterial stiffness <span class="hlt">gradient</span>) as a blood <span class="hlt">pressure</span>-independent measure of vascular aging. PWV is inherently dependent on the operational blood <span class="hlt">pressure</span>. In cross-sectional studies, PWV adjustment for mean arterial <span class="hlt">pressure</span> (MAP) is preferred, but still remains a nonoptimal approach, as the relationship between PWV and blood <span class="hlt">pressure</span> is nonlinear and varies considerably among individuals due to heterogeneity in genetic background, vascular tone, and vascular remodeling. Extrapolations from the blood <span class="hlt">pressure</span>-independent stiffness parameter β (β 0 ) have led to the creation of stiffness index β, which can be used for local stiffness. A similar approach has been used for cardio-ankle PWV to generate a blood <span class="hlt">pressure</span>-independent cardio-ankle vascular index (CAVI). It was recently demonstrated that stiffness index β and CAVI remain slightly blood <span class="hlt">pressure</span>-dependent, and a more appropriate formula has been proposed to make the proper adjustments. On the other hand, the negative impact of aortic stiffness on clinical outcomes is thought to be mediated through attenuation or reversal of the arterial stiffness <span class="hlt">gradient</span>, which can also be influenced by a reduction in peripheral medium-sized muscular arteries in conditions that predispose to accelerate vascular aging. Arterial stiffness <span class="hlt">gradient</span>, assessed by aortic-brachial PWV ratio, is emerging to be at least as good as cf-PWV for risk prediction, but has the advantage of not being affected by operating MAP. The negative impacts of aortic stiffness on clinical outcomes are proposed to be mediated through attenuation or reversal of arterial stiffness <span class="hlt">gradient</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994MsT.........17M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994MsT.........17M"><span>Compressible turbulence measurements in a supersonic boundary layer including favorable <span class="hlt">pressure</span> <span class="hlt">gradient</span> effects</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Miller, Raymond S.</p> <p>1994-12-01</p> <p>The effect of a favorable <span class="hlt">pressure</span> <span class="hlt">gradient</span> on the turbulent flow structure in a Mach 2.9 boundary layer (Re/m approximately equal to 1.5 x 10(exp 7)) is investigated experimentally. Conventional flow and hot film measurements of turbulent fluctuation properties have been made upstream of and along an expansion ramp. Upstream measurements were taken in a zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> boundary layer 44 cm from the nozzle throat in a 6.35 cm square test section. Measurements are obtained in the boundary layer, above the expansion ramp, 71.5 cm from the nozzle throat. Mean flow and turbulent flow characteristics are measured in all three dimensions. Comparisons are made between data obtained using single and multiple-overheat cross-wire anemometry as well as conventional mean flow probes. Conventional flow measurements were taken using a Pitot probe and a 10 degree cone static probe. Flow visualization was conducted via imaging techniques (Schlieren and shadowgraph photographs). Results suggest that compressibility effects, as seen through the density fluctuations in the Reynolds shear stress, are roughly 10% relative to the mean velocity and are large relative to the velocity fluctuations. This is also observed in the total Reynolds shear stress; compressibility accounts for 50-75% of the total shear. This is particularly true in the favorable <span class="hlt">pressure</span> <span class="hlt">gradient</span> region, where though the peak fluctuation intensities are diminished, the streamwise component of the mean flow is larger, hence the contribution of the compressibility term is significant in the Reynolds shear.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140002798','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140002798"><span>Vandenberg Air Force Base <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> Wind Study</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shafer, Jaclyn A.</p> <p>2013-01-01</p> <p>Warning category winds can adversely impact day-to-day space lift operations at Vandenberg Air Force Base (VAFB) in California. NASA's Launch Services Program and other programs at VAFB use wind forecasts issued by the 30 Operational Support Squadron Weather Flight (30 OSSWF) to determine if they need to limit activities or protect property such as a launch vehicle. The 30 OSSWF tasked the AMU to develop an automated Excel graphical user interface that includes <span class="hlt">pressure</span> <span class="hlt">gradient</span> thresholds between specific observing stations under different synoptic regimes to aid forecasters when issuing wind warnings. This required the AMU to determine if relationships between the variables existed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NucFu..58d6006S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NucFu..58d6006S"><span>On the physics of the <span class="hlt">pressure</span> and temperature <span class="hlt">gradients</span> in the edge of tokamak plasmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stacey, Weston M.</p> <p>2018-04-01</p> <p>An extended plasma fluid theory including atomic physics, radiation, electromagnetic and themodynamic forces, external sources of particles, momentum and energy, and kinetic ion orbit loss is employed to derive theoretical expressions that display the role of the various factors involved in the determination of the <span class="hlt">pressure</span> and temperature <span class="hlt">gradients</span> in the edge of tokamak plasmas. Calculations for current experiments are presented to illustrate the magnitudes of various effects including strong radiative and atomic physics edge cooling effects and strong reduction in ion particle and energy fluxes due to ion orbit loss in the plasma edge. An important new insight is the strong relation between rotation and the edge <span class="hlt">pressure</span> <span class="hlt">gradient</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DFDG32008A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DFDG32008A"><span>Experimental Measurements of a High Reynolds Num- ber Adverse <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> Turbulent Boundary Layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Atkinson, Callum; Amili, Omid; Stanislas, Michel; Cuvier, Christophe; Foucaut, Jean-Marc; Srinath, Sricharan; Laval, Jean-Philippe; Kaehler, Christian; Hain, Rainer; Scharnowski, Sven; Schroeder, Andreas; Geisler, Reinhard; Agocs, Janos; Roese, Anni; Willert, Christian; Klinner, Joachim; Soria, Julio</p> <p>2016-11-01</p> <p>The study of adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> turbulent boundary layers is complicated by the need to characterise both the local <span class="hlt">pressure</span> <span class="hlt">gradient</span> and it's upstream flow history. It is therefore necessary to measure a significant streamwise domain at a resolution sufficient to resolve the small scales features. To achieve this collaborative particle image velocimetry (PIV) measurements were performed in the large boundary layer wind-tunnel at the Laboratoire de Mecanique de Lille, including: planar measurements spanning a streamwise domain of 3.5m using 16 cameras covering 15 δ spanwise wall-normal stereo-PIV measurements, high-speed micro-PIV of the near wall region and wall shear stress; and streamwise wall-normal PIV in the viscous sub layer. Details of the measurements and preliminary results will be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930015352','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930015352"><span>Experimental Study of a Three-Dimensional Shear-Driven Turbulent Boundary Layer with Streamwise Adverse <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Driver, David M.; Johnston, James P.</p> <p>1990-01-01</p> <p>The effects of a strong adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> on a three-dimensional turbulent boundary layer are studied in an axisymmetric spinning cylinder geometry. Velocity measurements made with a three-component laser Doppler velocimeter include all three mean flow components, all six Reynolds stress components, and all ten triple-product correlations. Reynolds stress diminishes as the flow becomes three-dimensional. Lower levels of shear stress were seen to persist under adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> conditions. This low level of stress was seen to roughly correlate with the magnitude of cross-flow (relative to free stream flow) for this experiment as well as most of the other experiments in the literature. Variations in <span class="hlt">pressure</span> <span class="hlt">gradient</span> do not appear to alter this correlation. For this reason, it is hypothesized that a three-dimensional boundary layer is more prone to separate than a two-dimensional boundary layer, although it could not be directly shown here. None of the computations performed with either a Prandtl mixing length, k-epsilon, or a Launder-Reece-Rodi full Reynolds-stress model were able to predict the reduction in Reynolds stress.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29651628','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29651628"><span>Intracranial and Intraocular <span class="hlt">Pressure</span> at the Lamina Cribrosa: <span class="hlt">Gradient</span> Effects.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jóhannesson, Gauti; Eklund, Anders; Lindén, Christina</p> <p>2018-04-12</p> <p>A <span class="hlt">pressure</span> difference between the intraocular and intracranial compartments at the site of the lamina cribrosa has been hypothesized to have a pathophysiological role in several optic nerve head diseases. This paper reviews the current literature on the translamina cribrosa <span class="hlt">pressure</span> difference (TLCPD), the associated <span class="hlt">pressure</span> <span class="hlt">gradient</span>, and its potential pathophysiological role, as well as the methodology to assess TLCPD. For normal-tension glaucoma (NTG), initial studies indicated low intracranial <span class="hlt">pressure</span> (ICP) while recent findings indicate that a reduced ICP is not mandatory. Data from studies on the elevated TLCPD as a pathophysiological factor of NTG are equivocal. From the identification of potential postural effects on the cerebrospinal fluid (CSF) communication between the intracranial and retrolaminar space, we hypothesize that the missing link could be a dysfunction of an occlusion mechanism of the optic nerve sheath around the optic nerve. In upright posture, this could cause an elevated TLCPD even with normal ICP and we suggest that this should be investigated as a pathophysiological component in NTG patients.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28703367','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28703367"><span>Temporal relationship between instantaneous <span class="hlt">pressure</span> <span class="hlt">gradients</span> and peak-to-peak systolic ejection <span class="hlt">gradient</span> in congenital aortic stenosis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Boe, Brian A; Norris, Mark D; Zampi, Jeffrey D; Rocchini, Albert P; Ensing, Gregory J</p> <p>2017-12-01</p> <p>We sought to identify a time during cardiac ejection when the instantaneous <span class="hlt">pressure</span> <span class="hlt">gradient</span> (IPG) correlated best, and near unity, with peak-to-peak systolic ejection <span class="hlt">gradient</span> (PPSG) in patients with congenital aortic stenosis. Noninvasive echocardiographic measurement of IPG has limited correlation with cardiac catheterization measured PPSG across the spectrum of disease severity of congenital aortic stenosis. A major contributor is the observation that these measures are inherently different with a variable relationship dependent on the degree of stenosis. Hemodynamic data from cardiac catheterizations utilizing simultaneous <span class="hlt">pressure</span> measurements from the left ventricle (LV) and ascending aorta (AAo) in patients with congenital valvar aortic stenosis was retrospectively reviewed over the past 5 years. The cardiac cycle was standardized for all patients using the percentage of total LV ejection time (ET). Instantaneous <span class="hlt">gradient</span> at 5% intervals of ET were compared to PPSG using linear regression and Bland-Altman analysis. A total of 22 patients underwent catheterization at a median age of 13.7 years (interquartile range [IQR] 10.3-18.0) and median weight of 51.1 kg (IQR 34.2-71.6). The PPSG was 46.5 ± 12.6 mm Hg (mean ± SD) and correlated suboptimally with the maximum and mean IPG. The midsystolic IPG (occurring at 50% of ET) had the strongest correlation with the PPSG ( PPSG = 0.97(IPG50%)-1.12, R 2  = 0.88), while the IPG at 55% of ET was closest to unity ( PPSG = 0.997(IPG55%)-1.17, R 2  = 0.87). The commonly measured maximum and mean IPG are suboptimal estimates of the PPSG in congenital aortic stenosis. Using catheter-based data, IPG at 50%-55% of ejection correlates well with PPSG. This may allow for a more accurate estimation of PPSG via noninvasive assessment of IPG. © 2017 Wiley Periodicals, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22129011','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22129011"><span>Ice particles trapped by temperature <span class="hlt">gradients</span> at mbar <span class="hlt">pressure</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kelling, Thorben; Wurm, Gerhard; Dürmann, Christoph</p> <p>2011-11-01</p> <p>In laboratory experiments we observe that ice particles (≤100 μm) entrained in a low <span class="hlt">pressure</span> atmosphere (~1 mbar) get trapped by temperature <span class="hlt">gradients</span> between three reservoirs at different temperature. Confining elements are a peltier element at 250 K (bottom), a liquid nitrogen reservoir at 77 K (top), and the surrounding vacuum chamber at 293 K. Particle levitation and trapping is modeled by an interplay of thermophoresis, photophoresis, and gravity. A number of ice particles are trapped simultaneously in close spatial distance to each other at least up to minutes and are accessible for further experiments. © 2011 American Institute of Physics</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011RScI...82k5105K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011RScI...82k5105K"><span>Ice particles trapped by temperature <span class="hlt">gradients</span> at mbar <span class="hlt">pressure</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kelling, Thorben; Wurm, Gerhard; Dürmann, Christoph</p> <p>2011-11-01</p> <p>In laboratory experiments we observe that ice particles (⩽100 μm) entrained in a low <span class="hlt">pressure</span> atmosphere (˜1 mbar) get trapped by temperature <span class="hlt">gradients</span> between three reservoirs at different temperature. Confining elements are a peltier element at 250 K (bottom), a liquid nitrogen reservoir at 77 K (top), and the surrounding vacuum chamber at 293 K. Particle levitation and trapping is modeled by an interplay of thermophoresis, photophoresis, and gravity. A number of ice particles are trapped simultaneously in close spatial distance to each other at least up to minutes and are accessible for further experiments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhyS...91a5601Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhyS...91a5601Z"><span>Nonlinear Alfvén wave propagating in <span class="hlt">ideal</span> MHD plasmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zheng, Jugao; Chen, Yinhua; Yu, Mingyang</p> <p>2016-01-01</p> <p>The behavior of nonlinear Alfvén waves propagating in <span class="hlt">ideal</span> MHD plasmas is investigated numerically. It is found that in a one-dimensional weakly nonlinear system an Alfvén wave train can excite two longitudinal disturbances, namely an acoustic wave and a ponderomotively driven disturbance, which behave differently for β \\gt 1 and β \\lt 1, where β is the ratio of plasma-to-magnetic <span class="hlt">pressures</span>. In a strongly nonlinear system, the Alfvén wave train is modulated and can steepen to form shocks, leading to significant dissipation due to appearance of current sheets at magnetic-<span class="hlt">pressure</span> minima. For periodic boundary condition, we find that the Alfvén wave transfers its energy to the plasma and heats it during the shock formation. In two-dimensional systems, fast magneto-acoustic wave generation due to Alfvén wave phase mixing is considered. It is found that the process depends on the amplitude and frequency of the Alfvén waves, as well as their speed <span class="hlt">gradients</span> and the <span class="hlt">pressure</span> of the background plasma.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li class="active"><span>5</span></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_5 --> <div id="page_6" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li class="active"><span>6</span></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="101"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27165918','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27165918"><span>Automatic Calculation of Hydrostatic <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> in Patients with Head Injury: A Pilot Study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Moss, Laura; Shaw, Martin; Piper, Ian; Arvind, D K; Hawthorne, Christopher</p> <p>2016-01-01</p> <p>The non-surgical management of patients with traumatic brain injury is the treatment and prevention of secondary insults, such as low cerebral perfusion <span class="hlt">pressure</span> (CPP). Most clinical <span class="hlt">pressure</span> monitoring systems measure <span class="hlt">pressure</span> relative to atmospheric <span class="hlt">pressure</span>. If a patient is managed with their head tilted up, relative to their arterial <span class="hlt">pressure</span> transducer, then a hydrostatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> (HPG) can act against arterial <span class="hlt">pressure</span> and cause significant errors in calculated CPP.To correct for HPG, the arterial <span class="hlt">pressure</span> transducer should be placed level with the intracranial <span class="hlt">pressure</span> transducer. However, this is not always achieved. In this chapter, we describe a pilot study investigating the application of speckled computing (or "specks") for the automatic monitoring of the patient's head tilt and subsequent automatic calculation of HPG. In future applications this will allow us to automatically correct CPP to take into account any HPG.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19960015858','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19960015858"><span>A Study of the Development of Steady and Periodic Unsteady Turbulent Wakes Through Curved Channels at Positive, Zero, and Negative Streamwise <span class="hlt">Pressure</span> <span class="hlt">Gradients</span>, Part 1</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schobeiri, M. T.; John, J.</p> <p>1996-01-01</p> <p>The turbomachinery wake flow development is largely influenced by streamline curvature and streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The objective of this investigation is to study the development of the wake under the influence of streamline curvature and streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The experimental investigation is carried out in two phases. The first phase involves the study of the wake behind a stationary circular cylinder (steady wake) in curved channels at positive, zero, and negative streamwise <span class="hlt">pressure</span> <span class="hlt">gradients</span>. The mean velocity and Reynolds stress components are measured using a X-hot-film probe. The measured quantities obtained in probe coordinates are transformed to a curvilinear coordinate system along the wake centerline and are presented in similarity coordinates. The results of the steady wakes suggest strong asymmetry in velocity and Reynolds stress components. However, the velocity defect profiles in similarity coordinates are almost symmetrical and follow the same distribution as the zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> straight wake. The results of Reynolds stress distributions show higher values on the inner side of the wake than the outer side. Other quantities, including the decay of maximum velocity defect, growth of wake width, and wake integral parameters, are also presented for the three different <span class="hlt">pressure</span> <span class="hlt">gradient</span> cases of steady wake. The decay rate of velocity defect is fastest for the negative streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span> case and slowest for the positive <span class="hlt">pressure</span> <span class="hlt">gradient</span> case. Conversely, the growth of the wake width is fastest for the positive streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span> case and slowest for the negative streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The second phase studies the development of periodic unsteady wakes generated by the circular cylinders of the rotating wake generator in a curved channel at zero streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span>. Instantaneous velocity components of the periodic unsteady wakes, measured with a stationary X-hot-film probe, are analyzed by the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10240E..0HW','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10240E..0HW"><span>Accelerating <span class="hlt">gradient</span> improvement using shape-tailor laser front in radiation <span class="hlt">pressure</span> acceleration progress</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, W. P.; Shen, B. F.; Xu, Z. Z.</p> <p>2017-05-01</p> <p>The accelerating <span class="hlt">gradient</span> of a proton beam is crucial for stable radiation <span class="hlt">pressure</span> acceleration (RPA) because the multi-dimensional instabilities increase γ times slower in the relativistic region. In this paper, a shape-tailored laser is proposed to significantly accelerate the ions in a controllable high accelerating <span class="hlt">gradient</span>. In this method, the fastest ions initially rest in the middle of the foil are controlled to catch the compressed electron layer at the end of the hole-boring stage, thus the light-sail stage can start as soon as possible. Then the compressed electron layer is accelerated tightly together with the fastest ions by the shaped laser intensity, which further increases the accelerating <span class="hlt">gradient</span> in the light-sail stage. Such tailored pulse may be beneficial for the RPA driven by the 10-fs 10 petawatt laser in the future.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20020024643','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20020024643"><span>Flow Control Device Evaluation for an Internal Flow with an Adverse <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jenkins, Luther N.; Gorton, Susan Althoff; Anders, Scott G.</p> <p>2002-01-01</p> <p>The effectiveness of several active and passive devices to control flow in an adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> with secondary flows present was evaluated in the 15 Inch Low Speed Tunnel at NASA Langley Research Center. In this study, passive micro vortex generators, micro bumps, and piezoelectric synthetic jets were evaluated for their flow control characteristics using surface static <span class="hlt">pressures</span>, flow visualization, and 3D Stereo Digital Particle Image Velocimetry. Data also were acquired for synthetic jet actuators in a zero flow environment. It was found that the micro vortex generator is very effective in controlling the flow environment for an adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span>, even in the presence of secondary vortical flow. The mechanism by which the control is effected is a re-energization of the boundary layer through flow mixing. The piezoelectric synthetic jet actuators must have sufficient velocity output to produce strong longitudinal vortices if they are to be effective for flow control. The output of these devices in a laboratory or zero flow environment will be different than the output in a flow environment. In this investigation, the output was higher in the flow environment, but the stroke cycle in the flow did not indicate a positive inflow into the synthetic jet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5258845','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5258845"><span>Internalization of Appearance <span class="hlt">Ideals</span> Mediates the Relationship between Appearance-Related <span class="hlt">Pressures</span> from Peers and Emotional Eating among Adolescent Boys and Girls</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Thompson, Katherine A.; Kelly, Nichole R.; Schvey, Natasha A.; Brady, Sheila M.; Courville, Amber B.; Tanofsky-Kraff, Marian; Yanovski, Susan Z.; Yanovski, Jack A.; Shomaker, Lauren B.</p> <p>2016-01-01</p> <p>Appearance-related <span class="hlt">pressures</span> have been associated with binge eating in previous studies. Yet, it is unclear if these <span class="hlt">pressures</span> are associated with emotional eating or if specific sources of <span class="hlt">pressure</span> are differentially associated with emotional eating. We studied the associations between multiple sources of appearance-related <span class="hlt">pressures</span>, including <span class="hlt">pressure</span> to be thin and <span class="hlt">pressure</span> to increase muscularity, and emotional eating in 300 adolescents (Mage = 15.3, SD = 1.4, 60% female). Controlling for age, race, puberty, body mass index (BMI) z-score, and sex, both <span class="hlt">pressure</span> to be thin and <span class="hlt">pressure</span> to be more muscular from same-sex peers were positively associated with emotional eating in response to feeling angry/frustrated and unsettled (ps<.05). <span class="hlt">Pressure</span> from same-sex peers to be more muscular also was associated with eating when depressed (p<.05), and muscularity <span class="hlt">pressure</span> from opposite-sex peers related to eating in response to anger/frustration (p<.05). All associations were fully mediated by internalization of appearance <span class="hlt">ideals</span> according to Western cultural standards (ps<.001). Associations of <span class="hlt">pressures</span> from mothers and fathers with emotional eating were non-significant. Results considering sex as a moderator of the associations between appearance-related <span class="hlt">pressures</span> and emotional eating were non-significant. Findings illustrate that both <span class="hlt">pressure</span> to be thin and muscular from peers are related to more frequent emotional eating among both boys and girls, and these associations are explained through internalization of appearance-related <span class="hlt">ideals</span>. PMID:28038437</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28038437','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28038437"><span>Internalization of appearance <span class="hlt">ideals</span> mediates the relationship between appearance-related <span class="hlt">pressures</span> from peers and emotional eating among adolescent boys and girls.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Thompson, Katherine A; Kelly, Nichole R; Schvey, Natasha A; Brady, Sheila M; Courville, Amber B; Tanofsky-Kraff, Marian; Yanovski, Susan Z; Yanovski, Jack A; Shomaker, Lauren B</p> <p>2017-01-01</p> <p>Appearance-related <span class="hlt">pressures</span> have been associated with binge eating in previous studies. Yet, it is unclear if these <span class="hlt">pressures</span> are associated with emotional eating or if specific sources of <span class="hlt">pressure</span> are differentially associated with emotional eating. We studied the associations between multiple sources of appearance-related <span class="hlt">pressures</span>, including <span class="hlt">pressure</span> to be thin and <span class="hlt">pressure</span> to increase muscularity, and emotional eating in 300 adolescents (M age =15.3, SD=1.4, 60% female). Controlling for age, race, puberty, body mass index (BMI) z-score, and sex, both <span class="hlt">pressure</span> to be thin and <span class="hlt">pressure</span> to be more muscular from same-sex peers were positively associated with emotional eating in response to feeling angry/frustrated and unsettled (ps<0.05). <span class="hlt">Pressure</span> from same-sex peers to be more muscular also was associated with eating when depressed (p<0.05), and muscularity <span class="hlt">pressure</span> from opposite-sex peers related to eating in response to anger/frustration (p<0.05). All associations were fully mediated by internalization of appearance <span class="hlt">ideals</span> according to Western cultural standards (ps<0.001). Associations of <span class="hlt">pressures</span> from mothers and fathers with emotional eating were non-significant. Results considering sex as a moderator of the associations between appearance-related <span class="hlt">pressures</span> and emotional eating were non-significant. Findings illustrate that both <span class="hlt">pressure</span> to be thin and muscular from peers are related to more frequent emotional eating among both boys and girls, and these associations are explained through internalization of appearance-related <span class="hlt">ideals</span>. Copyright © 2016 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25753157','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25753157"><span>MRI measurements of intracranial <span class="hlt">pressure</span> in the upright posture: The effect of the hydrostatic <span class="hlt">pressure</span> <span class="hlt">gradient</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Alperin, Noam; Lee, Sang H; Bagci, Ahmet M</p> <p>2015-10-01</p> <p>To add the hydrostatic component of the cerebrospinal fluid (CSF) <span class="hlt">pressure</span> to magnetic resonance imaging (MRI)-derived intracranial <span class="hlt">pressure</span> (ICP) measurements in the upright posture for derivation of <span class="hlt">pressure</span> value in a central cranial location often used in invasive ICP measurements. Additional analyses were performed using data previously collected from 10 healthy subjects scanned in supine and sitting positions with a 0.5T vertical gap MRI scanner (GE Medical). Pulsatile blood and CSF flows to and from the brain were quantified using cine phase-contrast. Intracranial compliance and <span class="hlt">pressure</span> were calculated using a previously described method. The vertical distance between the location of the CSF flow measurement and a central cranial location was measured manually in the mid-sagittal T1 -weighted image obtained in the upright posture. The hydrostatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> of a CSF column with similar height was then added to the MR-ICP value. After adjustment for the hydrostatic component, the mean ICP value was reduced by 7.6 mmHg. Mean ICP referenced to the central cranial level was -3.4 ± 1.7 mmHg compared to the unadjusted value of +4.3 ± 1.8 mmHg. In the upright posture, the hydrostatic <span class="hlt">pressure</span> component needs to be added to the MRI-derived ICP values for compatibility with invasive ICP at a central cranial location. © 2015 Wiley Periodicals, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950014614','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950014614"><span>Wake measurements in a strong adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hoffenberg, R.; Sullivan, John P.; Schneider, S. P.</p> <p>1994-01-01</p> <p>The behavior of wakes in adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> is critical to the performance of high-lift systems for transport aircraft. Wake deceleration is known to lead to sudden thickening and the onset of reversed flow; this 'wake bursting' phenomenon can occur while surface flows remain attached. Although 'wake bursting' is known to be important for high-lift systems, no detailed measurements of 'burst' wakes have ever been reported. Wake bursting has been successfully achieved in the wake of a flat plate as it decelerated in a two-dimensional diffuser, whose sidewalls were forced to remain attached by use of slot blowing. Pilot probe surveys, L.D.V. measurements, and flow visualization have been used to investigate the physics of this decelerated wake, through the onset of reversed flow.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26940013','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26940013"><span>Cardiomyopathy in children: Can we rely on echocardiographic tricuspid regurgitation <span class="hlt">gradient</span> estimates of right ventricular and pulmonary arterial <span class="hlt">pressure</span>?</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lee, Simon; Lytrivi, Irene D; Roytman, Zhanna; Ko, Hyun-Sook Helen; Vinograd, Cheryl; Srivastava, Shubhika</p> <p>2016-10-01</p> <p>Introduction Agreement between echocardiography and right heart catheterisation-derived right ventricular systolic <span class="hlt">pressure</span> is modest in the adult heart failure population, but is unknown in the paediatric cardiomyopathy population. All patients at a single centre from 2001 to 2012 with a diagnosis of cardiomyopathy who underwent echocardiography and catheterisation within 30 days were included in this study. The correlation between tricuspid regurgitation <span class="hlt">gradient</span> and catheterisation-derived right ventricular systolic <span class="hlt">pressure</span> and mean pulmonary artery <span class="hlt">pressure</span> was determined. Agreement between echocardiography and catheterisation-derived right ventricular systolic <span class="hlt">pressure</span> was assessed using Bland-Altman plots. Analysis was repeated for patients who underwent both procedures within 7 days. Haemodynamic data from those with poor agreement and good agreement between echocardiography and catheterisation were compared. A total of 37 patients who underwent 48 catheterisation procedures were included in our study. The median age was 11.8 (0.1-20.6 years) with 22 males (58% total). There was a modest correlation (r=0.65) between echocardiography and catheterisation-derived right ventricular systolic <span class="hlt">pressure</span>, but agreement was poor. Agreement between tricuspid regurgitation <span class="hlt">gradient</span> and right ventricular systolic <span class="hlt">pressure</span> showed wide 95% limits of agreement. There was a modest correlation between the tricuspid regurgitation <span class="hlt">gradient</span> and mean pulmonary artery <span class="hlt">pressure</span> (r=0.6). Shorter time interval between the two studies did not improve agreement. Those with poor agreement between echocardiography and catheterisation had higher right heart <span class="hlt">pressures</span>, but this difference became insignificant after accounting for right atrial <span class="hlt">pressure</span>. Transthoracic echocardiography estimation of right ventricular systolic <span class="hlt">pressure</span> shows modest correlation with right heart <span class="hlt">pressures</span>, but has limited agreement and may underestimate the degree of pulmonary hypertension in paediatric</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoRL..44.8017C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoRL..44.8017C"><span>On the violation of <span class="hlt">gradient</span> wind balance at the top of tropical cyclones</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cohen, Yair; Harnik, Nili; Heifetz, Eyal; Nolan, David S.; Tao, Dandan; Zhang, Fuqing</p> <p>2017-08-01</p> <p>The existence of physical solutions for the <span class="hlt">gradient</span> wind balance is examined at the top of 12 simulated tropical cyclones. The <span class="hlt">pressure</span> field at the top of these storms, which depends on the vertically integrated effect of the warm core and the near surface low, is found to violate the <span class="hlt">gradient</span> wind balance—termed here as a state of nonbalance. Using a toy model, it is shown that slight changes in the relative location and relative widths of the warm core drastically increase the isobaric curvature at the upper level <span class="hlt">pressure</span> maps leading to nonbalance. While <span class="hlt">idealized</span> storms return to balance within several days, simulations of real-world tropical cyclones retain a considerable degree of nonbalance throughout the model integration. Comparing mean and maximum values of different storms shows that peak nonbalance correlates with either peak intensity or intensification, implying the possible importance of nonbalance at upper levels for the near surface winds.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19830054819&hterms=employment+work&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Demployment%2Bwork','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19830054819&hterms=employment+work&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Demployment%2Bwork"><span>A comparison of methods for computing the sigma-coordinate <span class="hlt">pressure</span> <span class="hlt">gradient</span> force for flow over sloped terrain in a hybrid theta-sigma model</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Johnson, D. R.; Uccellini, L. W.</p> <p>1983-01-01</p> <p>In connection with the employment of the sigma coordinates introduced by Phillips (1957), problems can arise regarding an accurate finite-difference computation of the <span class="hlt">pressure</span> <span class="hlt">gradient</span> force. Over steeply sloped terrain, the calculation of the sigma-coordinate <span class="hlt">pressure</span> <span class="hlt">gradient</span> force involves computing the difference between two large terms of opposite sign which results in large truncation error. To reduce the truncation error, several finite-difference methods have been designed and implemented. The present investigation has the objective to provide another method of computing the sigma-coordinate <span class="hlt">pressure</span> <span class="hlt">gradient</span> force. Phillips' method is applied for the elimination of a hydrostatic component to a flux formulation. The new technique is compared with four other methods for computing the <span class="hlt">pressure</span> <span class="hlt">gradient</span> force. The work is motivated by the desire to use an isentropic and sigma-coordinate hybrid model for experiments designed to study flow near mountainous terrain.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870033194&hterms=coulomb+law&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dcoulomb%2Blaw','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870033194&hterms=coulomb+law&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dcoulomb%2Blaw"><span>Beam-induced <span class="hlt">pressure</span> <span class="hlt">gradients</span> in the early phase of proton-heated solar flares</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tamres, David H.; Canfield, Richard C.; Mcclymont, A. N.</p> <p>1986-01-01</p> <p>The <span class="hlt">pressure</span> <span class="hlt">gradient</span> induced in a coronal loop by proton beam momentum deposition is calculated and compared with the thermal <span class="hlt">pressure</span> <span class="hlt">gradient</span> arising from nonuniform deposition of beam energy; it is assumed that the transfer of momentum and energy from beam to target occurs via the Coulomb interaciton. Results are presented for both a low mean energy and a high mean energy proton beam injected at the loop apex and characterized by a power-law energy spectrum. The present treatment takes account of the breakdown of the cold target approximation for the low-energy proton beam in the corona, where the thermal speed of target electrons exceeds the beam speed. It is found that proton beam momentum deposition plays a potentially significant role in flare dynamics only in the low mean energy case and only in the corona, where it may dominate the acceleration of target material for as long as several tens of seconds. This conclusion suggest that the presence of low-energy nonthermal protons may be inferred from velocity-sensitive coronal observations in the early impulsive phase.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5316482','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5316482"><span>Broadening of Analyte Streams due to a Transverse <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> in Free-Flow Isoelectric Focusing</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Dutta, Debashis</p> <p>2017-01-01</p> <p><span class="hlt">Pressure</span>-driven cross-flows can arise in free-flow isoelectric focusing systems (FFIEF) due to a non-uniform electroosmotic flow velocity along the channel width induced by the pH <span class="hlt">gradient</span> in this direction. In addition, variations in the channel cross-section as well as unwanted differences in hydrostatic heads at the buffer/sample inlet ports can also lead to such <span class="hlt">pressure-gradients</span> which besides altering the equilibrium position of the sample zones have a tendency to substantially broaden their widths deteriorating the separations. In this situation, a thorough assessment of stream broadening due to transverse <span class="hlt">pressure-gradients</span> in FFIEF devices is necessary in order to establish accurate design rules for the assay. The present article describes a mathematical framework to estimate the noted zone dispersion in FFIEF separations based on the method-of-moments approach under laminar flow conditions. A closed-form expression has been derived for the spatial variance of the analyte streams at their equilibrium positions as a function of the various operating parameters governing the assay performance. This expression predicts the normalized stream variance under the chosen conditions to be determined by two dimensionless Péclet numbers evaluated based on the transverse <span class="hlt">pressure</span>-driven and electrophoretic solute velocities in the separation chamber, respectively. Moreover, the analysis shows that while the stream width can be expected to increase with an increase in the value of the first Péclet number, the opposite trend will be followed with respect to the latter. The noted results have been validated using Monte Carlo simulations that also establish a time/length scale over which the predicted equilibrium stream width is attained in the system. PMID:28081900</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730006564','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730006564"><span>The turbulent boundary layer on a porous plate: An experimental study of the heat transfer behavior with adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Blackwell, B. F.; Kays, W. M.; Moffat, R. J.</p> <p>1972-01-01</p> <p>An experimental investigation of the heat transfer behavior of the near equilibrium transpired turbulent boundary layer with adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> has been carried out. Stanton numbers were measured by an energy balance on electrically heated plates that form the bottom wall of the wind tunnel. Two adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> were studied. Two types of transpiration boundary conditions were investigated. The concept of an equilibrium thermal boundary layer was introduced. It was found that Stanton number as a function of enthalpy thickness Reynolds number is essentially unaffected by adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> with no transpiration. Shear stress, heat flux, and turbulent Prandtl number profiles were computed from mean temperature and velocity profiles. It was concluded that the turbulent Prandtl number is greater than unity in near the wall and decreases continuously to approximately 0.5 at the free stream.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24787565','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24787565"><span>Analysis of the intraocular jet flows and <span class="hlt">pressure</span> <span class="hlt">gradients</span> induced by air and fluid infusion: mechanism of focal chorioretinal damage.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kim, Yong Joon; Jo, Sungkil; Moon, Daruchi; Joo, Youngcheol; Choi, Kyung Seek</p> <p>2014-05-01</p> <p>To comprehend the mechanism of focal chorioretinal damage by analysis of the <span class="hlt">pressure</span> distribution and dynamic <span class="hlt">pressure</span> induced by infused air during fluid-air exchange. A precise simulation featuring a model eye and a fluid circuit was designed to analyze fluid-air exchange. The <span class="hlt">pressure</span> distribution, flow velocity, and dynamic <span class="hlt">pressure</span> induced by infusion of air into an air-filled eye were analyzed using an approach based on fluid dynamics. The size of the port and the infusion <span class="hlt">pressure</span> were varied during simulated iterations. We simulated infusion of an air-filled eye with balanced salt solution (BSS) to better understand the mechanism of chorioretinal damage induced by infused air. Infused air was projected straight toward a point on the retina contralateral to the infusion port (the "vulnerable point"). The highest <span class="hlt">pressure</span> was evident at the vulnerable point, and the lowest <span class="hlt">pressure</span> was recorded on most retinal areas. Simulations using greater infusion <span class="hlt">pressure</span> and a port of larger size were associated with elevations in dynamic <span class="hlt">pressure</span> and the <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The <span class="hlt">pressure</span> <span class="hlt">gradients</span> were 2.8 and 5.1 mm Hg, respectively, when infusion <span class="hlt">pressures</span> of 30 and 50 mm Hg were delivered through a 20-gauge port. The <span class="hlt">pressure</span> <span class="hlt">gradient</span> associated with BSS infusion was greater than that created by air, but lasted for only a moment. Our simulation explains the mechanism of focal chorioretinal damage in numerical terms. Infused air induces a prolonged increase in focal <span class="hlt">pressure</span> on the vulnerable point, and this may be responsible for visual field defects arising after fluid-air exchange. Copyright 2014 The Association for Research in Vision and Ophthalmology, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011APS..DFD.M7003H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011APS..DFD.M7003H"><span>Zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> boundary layer at extreme Reynolds numbers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hultmark, Marcus; Vallikivi, Margit; Smits, Alexander</p> <p>2011-11-01</p> <p>Experiments were conducted in a zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> flat plate boundary layer using the Princeton/ONR High Reynolds number Test Facility (HRTF). The HRTF uses highly compressed air, up to 220 atmospheres, to produce Reynolds numbers up to Reθ =225,000 . This corresponds to a δ+ =65,000 which is one of the highest Reynolds numbers ever measured in a laboratory. When using <span class="hlt">pressure</span> to achieve high Reynolds numbers the size of the measurement probes become critical, thus the need for very small sensors is acute. The streamwise component of velocity was investigated using a nanoscale thermal anemometer (NSTAP) as well as a 200 μm pitot tube. The NSTAP has a spatial resolution as well as a temporal resolution one order of magnitude better than conventional measurement techniques. The data was compared to recent data from a high Reynolds number turbulent pipe flow and it was shown that the two flows are more similar than previous data suggests. Supported under NR Grant N00014-09-1-0263 (program manager Ron Joslin) and NSF Grant CBET-1064257(program manager Henning Winter).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/20999347-vertical-two-phase-flow-regimes-pressure-gradients-under-influence-sds-surfactant','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/20999347-vertical-two-phase-flow-regimes-pressure-gradients-under-influence-sds-surfactant"><span>Vertical two-phase flow regimes and <span class="hlt">pressure</span> <span class="hlt">gradients</span> under the influence of SDS surfactant</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Duangprasert, Tanabordee; Sirivat, Anuvat; Siemanond, Kitipat</p> <p>2008-01-15</p> <p>Two-phase gas/liquid flows in vertical pipes have been systematically investigated. Water and SDS surfactant solutions at various concentrations were used as the working fluids. In particular, we focus our work on the influence of surfactant addition on the flow regimes, the corresponding <span class="hlt">pressure</span> <span class="hlt">gradients</span>, and the bubble sizes and velocity. Adding the surfactant lowers the air critical Reynolds numbers for the bubble-slug flow and the slug flow transitions. The <span class="hlt">pressure</span> <span class="hlt">gradients</span> of SDS solutions are lower than those of pure water especially in the slug flow and the slug-churn flow regimes, implying turbulent drag reduction. At low Re{sub air}, themore » bubble sizes of the surfactant solution are lower than those of pure water due to the increase in viscosity. With increasing and at high Re{sub air}, the bubble sizes of the SDS solution become greater than those of pure water which is attributed to the effect of surface tension. (author)« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16621262','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16621262"><span>Determination of performance of non-<span class="hlt">ideal</span> aluminized explosives.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Keshavarz, Mohammad Hossein; Mofrad, Reza Teimuri; Poor, Karim Esmail; Shokrollahi, Arash; Zali, Abbas; Yousefi, Mohammad Hassan</p> <p>2006-09-01</p> <p>Non-<span class="hlt">ideal</span> explosives can have Chapman-Jouguet (C-J) detonation <span class="hlt">pressure</span> significantly different from those expected from existing thermodynamic computer codes, which usually allows finding the parameters of <span class="hlt">ideal</span> detonation of individual high explosives with good accuracy. A simple method is introduced by which detonation <span class="hlt">pressure</span> of non-<span class="hlt">ideal</span> aluminized explosives with general formula C(a)H(b)N(c)O(d)Al(e) can be predicted only from a, b, c, d and e at any loading density without using any assumed detonation products and experimental data. Calculated detonation <span class="hlt">pressures</span> show good agreement with experimental values with respect to computed results obtained by complicated computer code. It is shown here how loading density and atomic composition can be integrated into an empirical formula for predicting detonation <span class="hlt">pressure</span> of proposed aluminized explosives.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24209296','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24209296"><span>Fast <span class="hlt">gradient</span> separation by very high <span class="hlt">pressure</span> liquid chromatography: reproducibility of analytical data and influence of delay between successive runs.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Stankovicha, Joseph J; Gritti, Fabrice; Beaver, Lois Ann; Stevensona, Paul G; Guiochon, Georges</p> <p>2013-11-29</p> <p>Five methods were used to implement fast <span class="hlt">gradient</span> separations: constant flow rate, constant column-wall temperature, constant inlet <span class="hlt">pressure</span> at moderate and high <span class="hlt">pressures</span> (controlled by a <span class="hlt">pressure</span> controller),and programmed flow constant <span class="hlt">pressure</span>. For programmed flow constant <span class="hlt">pressure</span>, the flow rates and <span class="hlt">gradient</span> compositions are controlled using input into the method instead of the <span class="hlt">pressure</span> controller. Minor fluctuations in the inlet <span class="hlt">pressure</span> do not affect the mobile phase flow rate in programmed flow. There producibilities of the retention times, the response factors, and the eluted band width of six successive separations of the same sample (9 components) were measured with different equilibration times between 0 and 15 min. The influence of the length of the equilibration time on these reproducibilities is discussed. The results show that the average column temperature may increase from one separation to the next and that this contributes to fluctuation of the results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040087555&hterms=Gradient&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DGradient','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040087555&hterms=Gradient&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DGradient"><span>Improvement in diastolic intraventricular <span class="hlt">pressure</span> <span class="hlt">gradients</span> in patients with HOCM after ethanol septal reduction</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rovner, Aleksandr; Smith, Rebecca; Greenberg, Neil L.; Tuzcu, E. Murat; Smedira, Nicholas; Lever, Harry M.; Thomas, James D.; Garcia, Mario J.</p> <p>2003-01-01</p> <p>We sought to validate measurement of intraventricular <span class="hlt">pressure</span> <span class="hlt">gradients</span> (IVPG) and analyze their change in patients with hypertrophic obstructive cardiomyopathy (HOCM) after ethanol septal reduction (ESR). Quantitative analysis of color M-mode Doppler (CMM) images may be used to estimate diastolic IVPG noninvasively. Noninvasive IVPG measurement was validated in 10 patients undergoing surgical myectomy. Echocardiograms were then analyzed in 19 patients at baseline and after ESR. Pulsed Doppler data through the mitral valve and pulmonary venous flow were obtained. CMM was used to obtain the flow propagation velocity (Vp) and to calculate IVPG off-line. Left atrial <span class="hlt">pressure</span> was estimated with the use of previously validated Doppler equations. Data were compared before and after ESR. CMM-derived IVPG correlated well with invasive measurements obtained before and after surgical myectomy [r = 0.8, P < 0.01, Delta(CMM - invasive IVPG) = 0.09 +/- 0.45 mmHg]. ESR resulted in a decrease of resting LVOT systolic <span class="hlt">gradient</span> from 62 +/- 10 to 29 +/- 5 mmHg (P < 0.001). There was a significant increase in the Vp and IVPG (from 48 +/- 5to 74 +/- 7 cm/s and from 1.5 +/- 0.2 to 2.6 +/- 0.3 mmHg, respectively, P < 0.001 for both). Estimated left atrial <span class="hlt">pressure</span> decreased from 16.2 +/- 1.1 to 11.5 +/- 0.9 mmHg (P < 0.001). The increase in IVPG correlated with the reduction in the LVOT <span class="hlt">gradient</span> (r = 0.6, P < 0.01). Reduction of LVOT obstruction after ESR is associated with an improvement in diastolic suction force. Noninvasive measurements of IVPG may be used as an indicator of diastolic function improvement in HOCM.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li class="active"><span>6</span></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_6 --> <div id="page_7" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="121"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19810012482','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19810012482"><span>The influence of a high <span class="hlt">pressure</span> <span class="hlt">gradient</span> on unsteady velocity perturbations in the case of a turbulent supersonic flow</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dussauge, J. P.; Debieve, J. F.</p> <p>1980-01-01</p> <p>The amplification or reduction of unsteady velocity perturbations under the influence of strong flow acceleration or deceleration was studied. Supersonic flows with large velocity, <span class="hlt">pressure</span> <span class="hlt">gradients</span>, and the conditions in which the velocity fluctuations depend on the action of the average <span class="hlt">gradients</span> of <span class="hlt">pressure</span> and velocity rather than turbulence, are described. Results are analyzed statistically and interpreted as a return to laminar process. It is shown that this return to laminar implies negative values in the turbulence production terms for kinetic energy. A simple geometrical representation of the Reynolds stress production is given.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22972665','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22972665"><span><span class="hlt">Idealness</span> and similarity in goal-derived categories: a computational examination.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Voorspoels, Wouter; Storms, Gert; Vanpaemel, Wolf</p> <p>2013-02-01</p> <p>The finding that the typicality <span class="hlt">gradient</span> in goal-derived categories is mainly driven by <span class="hlt">ideals</span> rather than by exemplar similarity has stood uncontested for nearly three decades. Due to the rather rigid earlier implementations of similarity, a key question has remained--that is, whether a more flexible approach to similarity would alter the conclusions. In the present study, we evaluated whether a similarity-based approach that allows for dimensional weighting could account for findings in goal-derived categories. To this end, we compared a computational model of exemplar similarity (the generalized context model; Nosofsky, Journal of Experimental Psychology. General 115:39-57, 1986) and a computational model of <span class="hlt">ideal</span> representation (the <span class="hlt">ideal</span>-dimension model; Voorspoels, Vanpaemel, & Storms, Psychonomic Bulletin & Review 18:1006-114, 2011) in their accounts of exemplar typicality in ten goal-derived categories. In terms of both goodness-of-fit and generalizability, we found strong evidence for an <span class="hlt">ideal</span> approach in nearly all categories. We conclude that focusing on a limited set of features is necessary but not sufficient to account for the observed typicality <span class="hlt">gradient</span>. A second aspect of <span class="hlt">ideal</span> representations--that is, that extreme rather than common, central-tendency values drive typicality--seems to be crucial.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27457561','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27457561"><span>Repeatability of <span class="hlt">gradient</span> ultrahigh <span class="hlt">pressure</span> liquid chromatography-tandem mass spectrometry methods in instrument-controlled thermal environments.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Grinias, James P; Wong, Jenny-Marie T; Kennedy, Robert T</p> <p>2016-08-26</p> <p>The impact of viscous friction on eluent temperature and column efficiency in liquid chromatography is of renewed interest as the need for <span class="hlt">pressures</span> exceeding 1000bar to use with columns packed with sub-2μm particles has grown. One way the development of axial and radial temperature <span class="hlt">gradients</span> that arise due to viscous friction can be affected is by the thermal environment the column is placed in. In this study, a new column oven integrated into an ultrahigh <span class="hlt">pressure</span> liquid chromatograph that enables both still-air and forced-air operating modes is investigated to find the magnitude of the effect of the axial thermal <span class="hlt">gradient</span> that forms in 2.1×100mm columns packed with sub-2μm particles in these modes. Temperature increases of nearly 30K were observed when the generated power of the column exceeded 25W/m. The impact of the heating due to viscous friction on the repeatability of peak capacity, elution time, and peak area ratio to an internal standard for a <span class="hlt">gradient</span> UHPLC-MS/MS method to analyze neurotransmitters was found to be limited. This result indicates that high speed UHPLC-MS/MS <span class="hlt">gradient</span> methods under conditions of high viscous friction may be possible without the negative effects typically observed with isocratic separations under similar conditions. Copyright © 2016 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24739801','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24739801"><span>Can we identify response markers to antihypertensive drugs? First results from the <span class="hlt">IDEAL</span> Trial.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gueyffier, F; Subtil, F; Bejan-Angoulvant, T; Zerbib, Y; Baguet, J P; Boivin, J M; Mercier, A; Leftheriotis, G; Gagnol, J P; Fauvel, J P; Giraud, C; Bricca, G; Maucort-Boulch, D; Erpeldinger, S</p> <p>2015-01-01</p> <p>Current antihypertensive strategies do not take into account that individual characteristics may influence the magnitude of blood <span class="hlt">pressure</span> (BP) reduction. Guidelines promote trial-and-error approaches with many different drugs. We conducted the Identification of the Determinants of the Efficacy of Arterial blood <span class="hlt">pressure</span> Lowering drugs (<span class="hlt">IDEAL</span>) Trial to identify factors associated with BP responses to perindopril and indapamide. <span class="hlt">IDEAL</span> was a cross-over, double-blind, placebo-controlled trial, involving four 4-week periods: indapamide, perindopril and two placebo. Eligible patients were untreated, hypertensive and aged 25-70 years. The main outcome was systolic BP (SBP) response to drugs. The 112 participants with good compliance had a mean age of 52. One in every three participants was a woman. In middle-aged women, the SBP reduction from drugs was -11.5 mm Hg (indapamide) and -8.3 mm Hg (perindopril). In men, the response was significantly smaller: -4.8 mm Hg (indapamide) and -4.3 (perindopril) (P for sex differences 0.001 and 0.015, respectively). SBP response to perindopril decreased by 2 mm Hg every 10 years of age in both sexes (P=0.01). The response to indapamide increased by 3 mm Hg every 10 years of age <span class="hlt">gradient</span> in women (P=0.02). Age and sex were important determinants of BP response for antihypertensive drugs in the <span class="hlt">IDEAL</span> population. This should be taken into account when choosing drugs a priori.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16448061','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16448061"><span>Pseudolinear <span class="hlt">gradient</span> ultrahigh-<span class="hlt">pressure</span> liquid chromatography using an injection valve assembly.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Xiang, Yanqiao; Liu, Yansheng; Stearns, Stanley D; Plistil, Alex; Brisbin, Martin P; Lee, Milton L</p> <p>2006-02-01</p> <p>The use of ultrahigh <span class="hlt">pressures</span> in liquid chromatography (UHPLC) imposes stringent requirements on hardware such as pumps, valves, injectors, connecting tubing, and columns. One of the most difficult components of the UHPLC system to develop has been the sample injector. Static-split injection, which can be performed at <span class="hlt">pressures</span> up to 6900 bar (100,000 psi), consumes a large sample volume and is very irreproducible. A <span class="hlt">pressure</span>-balanced injection valve provided better reproducibility, shorter injection time, reduced sample consumption, and greater ease of use; however, it could only withstand <span class="hlt">pressures</span> up to approximately 1000 bar (15,000 psi). In this study, a new injection valve assembly that can operate at <span class="hlt">pressures</span> as high as 2070 bar (30,000 psi) was evaluated for UHPLC. This assembly contains six miniature electronically controlled needle valves to provide accurate and precise volumes for introduction into the capillary LC column. It was found that sample volumes as small as several tenths of a nanoliter can be injected, which are comparable to the results obtained from the static-split injector. The reproducibilities of retention time, efficiency, and peak area were investigated, and the results showed that the relative standard deviations of these parameters were small enough for quantitative analyses. Separation experiments using the UHPLC system with this new injection valve assembly showed that this new injector is suitable for both isocratic and <span class="hlt">gradient</span> operation modes. A newly designed capillary connector was used at a <span class="hlt">pressure</span> as high as 2070 bar (30,000 psi).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930092247','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930092247"><span>Analysis and calculation by integral methods of laminar compressible boundary-layer with heat transfer and with and without <span class="hlt">pressure</span> <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Morduchow, Morris</p> <p>1955-01-01</p> <p>A survey of integral methods in laminar-boundary-layer analysis is first given. A simple and sufficiently accurate method for practical purposes of calculating the properties (including stability) of the laminar compressible boundary layer in an axial <span class="hlt">pressure</span> <span class="hlt">gradient</span> with heat transfer at the wall is presented. For flow over a flat plate, the method is applicable for an arbitrarily prescribed distribution of temperature along the surface and for any given constant Prandtl number close to unity. For flow in a <span class="hlt">pressure</span> <span class="hlt">gradient</span>, the method is based on a Prandtl number of unity and a uniform wall temperature. A simple and accurate method of determining the separation point in a compressible flow with an adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> over a surface at a given uniform wall temperature is developed. The analysis is based on an extension of the Karman-Pohlhausen method to the momentum and the thermal energy equations in conjunction with fourth- and especially higher degree velocity and stagnation-enthalpy profiles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930092249','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930092249"><span>Characteristics of turbulence in boundary layer with zero <span class="hlt">pressure</span> <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Klebanoff, P S</p> <p>1955-01-01</p> <p>The results of an experimental investigation of a turbulent boundary layer with zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> are presented. Measurements with the hot-wire anemometer were made of turbulent energy and turbulent shear stress, probability density and flattening factor of u-fluctuation (fluctuation in x-direction), spectra of turbulent energy and shear stress, and turbulent dissipation. The importance of the region near the wall and the inadequacy of the concept of local isotropy are demonstrated. Attention is given to the energy balance and the intermittent character of the outer region of the boundary layer. Also several interesting features of the spectral distribution of the turbulent motions are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28864110','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28864110"><span>Accurate prediction of retention in hydrophilic interaction chromatography by back calculation of high <span class="hlt">pressure</span> liquid chromatography <span class="hlt">gradient</span> profiles.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Nu; Boswell, Paul G</p> <p>2017-10-20</p> <p><span class="hlt">Gradient</span> retention times are difficult to project from the underlying retention factor (k) vs. solvent composition (φ) relationships. A major reason for this difficulty is that <span class="hlt">gradients</span> produced by HPLC pumps are imperfect - <span class="hlt">gradient</span> delay, <span class="hlt">gradient</span> dispersion, and solvent mis-proportioning are all difficult to account for in calculations. However, we recently showed that a <span class="hlt">gradient</span> "back-calculation" methodology can measure these imperfections and take them into account. In RPLC, when the back-calculation methodology was used, error in projected <span class="hlt">gradient</span> retention times is as low as could be expected based on repeatability in the k vs. φ relationships. HILIC, however, presents a new challenge: the selectivity of HILIC columns drift strongly over time. Retention is repeatable in short time, but selectivity frequently drifts over the course of weeks. In this study, we set out to understand if the issue of selectivity drift can be avoid by doing our experiments quickly, and if there any other factors that make it difficult to predict <span class="hlt">gradient</span> retention times from isocratic k vs. φ relationships when <span class="hlt">gradient</span> imperfections are taken into account with the back-calculation methodology. While in past reports, the accuracy of retention projections was >5%, the back-calculation methodology brought our error down to ∼1%. This result was 6-43 times more accurate than projections made using <span class="hlt">ideal</span> <span class="hlt">gradients</span> and 3-5 times more accurate than the same retention projections made using offset <span class="hlt">gradients</span> (i.e., <span class="hlt">gradients</span> that only took <span class="hlt">gradient</span> delay into account). Still, the error remained higher in our HILIC projections than in RPLC. Based on the shape of the back-calculated <span class="hlt">gradients</span>, we suspect the higher error is a result of prominent <span class="hlt">gradient</span> distortion caused by strong, preferential water uptake from the mobile phase into the stationary phase during the <span class="hlt">gradient</span> - a factor our model did not properly take into account. It appears that, at least with the stationary phase</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PSST...27c5008Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PSST...27c5008Y"><span>Magnetical asymmetry effect in capacitively coupled plasmas: effects of the magnetic field <span class="hlt">gradient</span>, <span class="hlt">pressure</span>, and gap length</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Shali; Chang, Lijie; Zhang, Ya; Jiang, Wei</p> <p>2018-03-01</p> <p>By applying the asymmetric magnetic field to a discharge, the dc self-bias and asymmetric plasma response can be generated even in a geometrically and electrically symmetric system. This is called magnetical asymmetric effect (MAE), which can be a new method to control the ion energy and flux independently (Yang et al 2017 Plasma Process. Polym. 14 1700087). In the present work, the effects of magnetic field <span class="hlt">gradient</span>, gas <span class="hlt">pressure</span> and gap length on MAE are investigated by using a one-dimensional implicit particle-in-cell/Monte Carlo collision simulation. It found that by appropriately increasing the magnetic field <span class="hlt">gradient</span> and the gap length, the range of the self-bias voltage will be enlarged, which can be used as the effective approach to control the ion bombarding energy at the electrodes since the ion energy is determined by the voltage drop across the sheath. It also found that the ion flux asymmetry will disappear at high <span class="hlt">pressure</span> when the magnetic field <span class="hlt">gradient</span> is relative low, due to the frequent electron-neutral collisions can disrupt electron gyromotion and thus the MAE is greatly reduced.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040112441&hterms=adrenergic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dadrenergic','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040112441&hterms=adrenergic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dadrenergic"><span>Estimation of diastolic intraventricular <span class="hlt">pressure</span> <span class="hlt">gradients</span> by Doppler M-mode echocardiography</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Greenberg, N. L.; Vandervoort, P. M.; Firstenberg, M. S.; Garcia, M. J.; Thomas, J. D.</p> <p>2001-01-01</p> <p>Previous studies have shown that small intraventricular <span class="hlt">pressure</span> <span class="hlt">gradients</span> (IVPG) are important for efficient filling of the left ventricle (LV) and as a sensitive marker for ischemia. Unfortunately, there has previously been no way of measuring these noninvasively, severely limiting their research and clinical utility. Color Doppler M-mode (CMM) echocardiography provides a spatiotemporal velocity distribution along the inflow tract throughout diastole, which we hypothesized would allow direct estimation of IVPG by using the Euler equation. Digital CMM images, obtained simultaneously with intracardiac <span class="hlt">pressure</span> waveforms in six dogs, were processed by numerical differentiation for the Euler equation, then integrated to estimate IVPG and the total (left atrial to left ventricular apex) <span class="hlt">pressure</span> drop. CMM-derived estimates agreed well with invasive measurements (IVPG: y = 0.87x + 0.22, r = 0.96, P < 0.001, standard error of the estimate = 0.35 mmHg). Quantitative processing of CMM data allows accurate estimation of IVPG and tracking of changes induced by beta-adrenergic stimulation. This novel approach provides unique information on LV filling dynamics in an entirely noninvasive way that has previously not been available for assessment of diastolic filling and function.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1985asme.confU....M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1985asme.confU....M"><span>The influence of the radial <span class="hlt">pressure</span> <span class="hlt">gradient</span> on the blade root loss in an annular subsonic nozzle cascade</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Meng, D.; Weng, Z.; Xiang, Y.</p> <p>1985-09-01</p> <p>This paper presents a method for predicting the blade root loss in an annular nozzle cascade in which consideration is given to the influence of the radial <span class="hlt">pressure</span> <span class="hlt">gradient</span> (RPG) on it. The variation of blade root losses under different RPG is obtained experimentally, and finite element method is used to calculate the <span class="hlt">pressure</span> distribution in the blade passage.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010018435','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010018435"><span>Measurement of the Turbulence Kinetic Energy Budget of a Turbulent Planar Wake Flow in <span class="hlt">Pressure</span> <span class="hlt">Gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Liu, Xiao-Feng; Thomas, Flint O.; Nelson, Robert C.</p> <p>2001-01-01</p> <p>Turbulence kinetic energy (TKE) is a very important quantity for turbulence modeling and the budget of this quantity in its transport equation can provide insight into the flow physics. Turbulence kinetic energy budget measurements were conducted for a symmetric turbulent wake flow subjected to constant zero, favorable and adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> in year-three of research effort. The purpose of this study is to clarify the flow physics issues underlying the demonstrated influence of <span class="hlt">pressure</span> <span class="hlt">gradient</span> on wake development and provide experimental support for turbulence modeling. To ensure the reliability of these notoriously difficult measurements, the experimental procedure was carefully designed on the basis of an uncertainty analysis. Four different approaches, based on an isotropic turbulence assumption, a locally axisymmetric homogeneous turbulence assumption, a semi-isotropy assumption and a forced balance of the TKE equation, were applied for the estimate of the dissipation term. The <span class="hlt">pressure</span> transport term is obtained from a forced balance of the turbulence kinetic energy equation. This report will present the results of the turbulence kinetic energy budget measurement and discuss their implication on the development of strained turbulent wakes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19750006922','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19750006922"><span>An experimental investigation of heat transfer to reusable surface insulation tile array gaps in a turbulent boundary layer with <span class="hlt">pressure</span> <span class="hlt">gradient</span>. M.S. Thesis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Throckmorton, D. A.</p> <p>1975-01-01</p> <p>An experimental investigation was performed to determine the effect of <span class="hlt">pressure</span> <span class="hlt">gradient</span> on the heat transfer to space shuttle reusable surface insulation (RSI) tile array gaps under thick, turbulent boundary layer conditions. Heat transfer and <span class="hlt">pressure</span> measurements were obtained on a curved array of full-scale simulated RSI tiles in a tunnel wall boundary layer at a nominal freestream Mach number of 10.3 and freestream unit Reynolds numbers of 1.6, 3.3, and and 6.1 million per meter. Transverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> were induced over the model surface by rotating the curved array with respect to the flow. Definition of the tunnel wall boundary layer flow was obtained by measurement of boundary layer pitot <span class="hlt">pressure</span> profiles, and flat plate wall <span class="hlt">pressure</span> and heat transfer. Flat plate wall heat transfer data were correlated and a method was derived for prediction of smooth, curved array heat transfer in the highly three-dimensional tunnel wall boundary layer flow and simulation of full-scale space shuttle vehicle <span class="hlt">pressure</span> <span class="hlt">gradient</span> levels was assessed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19720007523','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19720007523"><span>Calculation of turbulent boundary layers with heat transfer and <span class="hlt">pressure</span> <span class="hlt">gradient</span> utilizing a compressibility transformation. Part 3: Computer program manual</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schneider, J.; Boccio, J.</p> <p>1972-01-01</p> <p>A computer program is described capable of determining the properties of a compressible turbulent boundary layer with <span class="hlt">pressure</span> <span class="hlt">gradient</span> and heat transfer. The program treats the two-dimensional problem assuming perfect gas and Crocco integral energy solution. A compressibility transformation is applied to the equation for the conservation of mass and momentum, which relates this flow to a low speed constant property flow with simultaneous mass transfer and <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The resulting system of describing equations consists of eight ordinary differential equations which are solved numerically. For Part 1, see N72-12226; for Part 2, see N72-15264.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25703162','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25703162"><span>Identification of <span class="hlt">ideal</span> resuscitation <span class="hlt">pressure</span> with concurrent traumatic brain injury in a rat model of hemorrhagic shock.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hu, Yi; Wu, Yue; Tian, Kunlun; Lan, Dan; Chen, Xiangyun; Xue, Mingying; Liu, Liangming; Li, Tao</p> <p>2015-05-01</p> <p>Traumatic brain injury (TBI) is often associated with uncontrolled hemorrhagic shock (UHS), which contributes significantly to the mortality of severe trauma. Studies have demonstrated that permissive hypotension resuscitation improves the survival for uncontrolled hemorrhage. What the <span class="hlt">ideal</span> target mean arterial <span class="hlt">pressure</span> (MAP) is for TBI with UHS remains unclear. With the rat model of TBI in combination with UHS, we investigated the effects of a series of target resuscitation <span class="hlt">pressures</span> (MAP from 50-90 mm Hg) on animal survival, brain perfusion, and organ function before hemorrhage controlled. Rats in 50-, 60-, and 70-mm Hg target MAP groups had less blood loss and less fluid requirement, a better vital organ including mitochondrial function and better cerebral blood flow, and animal survival (8, 6, and 7 of 10, respectively) than 80- and 90-mm Hg groups. The 70-mm Hg group had a better cerebral blood flow and cerebral mitochondrial function than in 50- and 60-mm Hg groups. In contrast, 80- and 90-mm Hg groups resulted in an excessive hemodilution, a decreased blood flow, an increased brain water content, and more severe cerebral edema. A 50-mm Hg target MAP is not suitable for the resuscitation of TBI combined with UHS. A 70 mm Hg of MAP is the <span class="hlt">ideal</span> target resuscitation <span class="hlt">pressure</span> for this trauma, which can keep sufficient perfusion to the brain and keep good organ function including cerebral mitochondrial function. Copyright © 2015 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19820031072&hterms=refraction&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Drefraction','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19820031072&hterms=refraction&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Drefraction"><span>Radio jet refraction in galactic atmospheres with static <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Henriksen, R. N.; Vallee, J. P.; Bridle, A. H.</p> <p>1981-01-01</p> <p>A theory based on the refraction of radio jets in the extended atmosphere of an elliptical galaxy, is proposed for double radio sources with a Z or S morphology. The model describes a collimated jet of supersonic material that bends self-consistently under the influence of external static <span class="hlt">pressure</span> <span class="hlt">gradients</span>, and may alternatively be seen as a continuous-jet version of the buoyancy model proposed by Gull (1973). Emphasis is placed on (1) S-shaped radio sources identified with isolated galaxies, such as 3C 293, whose radio structures should be free of distortions resulting from motion relative to a cluster medium, and (2) small-scale, galaxy-dominated rather than environment-dominated S-shaped sources such as the inner jet structure of Fornax A.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15518624','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15518624"><span>Development of exercise-induced arm-leg blood <span class="hlt">pressure</span> <span class="hlt">gradient</span> and abnormal arterial compliance in patients with repaired coarctation of the aorta.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Markham, Larry W; Knecht, Sandra K; Daniels, Stephen R; Mays, Wayne A; Khoury, Philip R; Knilans, Timothy K</p> <p>2004-11-01</p> <p>Often, the lack of systemic arterial hypertension and the lack of a resting arm-leg blood <span class="hlt">pressure</span> <span class="hlt">gradient</span> are used to assess the adequacy of the anatomic result after intervention for coarctation of the aorta (CoA). Some patients with no arm-leg <span class="hlt">gradient</span> at rest may develop a <span class="hlt">gradient</span> with exercise, leading caregivers to question the success of the repair. It is not clear what the prevalence is of patients who have undergone a successful intervention for CoA and have no arm-leg <span class="hlt">gradient</span> at rest but develop a significant <span class="hlt">gradient</span> with exercise and which factors may predict the development of an arm-leg <span class="hlt">gradient</span> with exercise. This study evaluates the prevalence and predictors of an exercise-induced arm-leg <span class="hlt">gradient</span> in subjects who have undergone an apparently successful intervention for CoA.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1236848','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1236848"><span>Modeling of Propagation of Interacting Cracks Under Hydraulic <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Huang, Hai; Mattson, Earl Douglas; Podgorney, Robert Karl</p> <p></p> <p>A robust and reliable numerical model for fracture initiation and propagation, which includes the interactions among propagating fractures and the coupling between deformation, fracturing and fluid flow in fracture apertures and in the permeable rock matrix, would be an important tool for developing a better understanding of fracturing behaviors of crystalline brittle rocks driven by thermal and (or) hydraulic <span class="hlt">pressure</span> <span class="hlt">gradients</span>. In this paper, we present a physics-based hydraulic fracturing simulator based on coupling a quasi-static discrete element model (DEM) for deformation and fracturing with conjugate lattice network flow model for fluid flow in both fractures and porous matrix. Fracturingmore » is represented explicitly by removing broken bonds from the network to represent microcracks. Initiation of new microfractures and growth and coalescence of the microcracks leads to the formation of macroscopic fractures when external and/or internal loads are applied. The coupled DEM-network flow model reproduces realistic growth pattern of hydraulic fractures. In particular, simulation results of perforated horizontal wellbore clearly demonstrate that elastic interactions among multiple propagating fractures, fluid viscosity, strong coupling between fluid <span class="hlt">pressure</span> fluctuations within fractures and fracturing, and lower length scale heterogeneities, collectively lead to complicated fracturing patterns.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980227970','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980227970"><span>Charts and Tables for Estimating the Stability of the Compressible Laminar Boundary Layer with Heat Transfer and Arbitrary <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tetervin, Neal</p> <p>1959-01-01</p> <p>The minimum critical Reynolds numbers for the similar solutions of the compressible laminar boundary layer computed by Cohen and Reshotko and also for the Falkner and Skan solutions as recomputed by Smith have been calculated by Lin's rapid approximate method for two-dimensional disturbances. These results enable the stability of the compressible laminar boundary layer with heat transfer and <span class="hlt">pressure</span> <span class="hlt">gradient</span> to be easily estimated after the behavior of the boundary layer has been computed by the approximate method of Cohen and Reshotko. The previously reported unusual result (NACA Technical Note 4037) that a highly cooled stagnation point flow is more unstable than a highly cooled flat-plate flow is again encountered. Moreover, this result is found to be part of the more general result that a favorable <span class="hlt">pressure</span> <span class="hlt">gradient</span> is destabilizing for very cool walls when the Mach number is less than that for complete stability. The minimum critical Reynolds numbers for these wall temperature ratios are, however, all larger than any value of the laminar-boundary-layer Reynolds number likely to be encountered. For Mach numbers greater than those for which complete stability occurs a favorable <span class="hlt">pressure</span> <span class="hlt">gradient</span> is stabilizing, even for very cool walls.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3991613','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3991613"><span>The Influence of Body Position on Cerebrospinal Fluid <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> and Movement in Cats with Normal and Impaired Craniospinal Communication</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Radoš, Milan; Erceg, Gorislav; Petošić, Antonio; Jurjević, Ivana</p> <p>2014-01-01</p> <p>Intracranial hypertension is a severe therapeutic problem, as there is insufficient knowledge about the physiology of cerebrospinal fluid (CSF) <span class="hlt">pressure</span>. In this paper a new CSF <span class="hlt">pressure</span> regulation hypothesis is proposed. According to this hypothesis, the CSF <span class="hlt">pressure</span> depends on the laws of fluid mechanics and on the anatomical characteristics inside the cranial and spinal space, and not, as is today generally believed, on CSF secretion, circulation and absorption. The volume and <span class="hlt">pressure</span> changes in the newly developed CSF model, which by its anatomical dimensions and basic biophysical features imitates the craniospinal system in cats, are compared to those obtained on cats with and without the blockade of craniospinal communication in different body positions. During verticalization, a long-lasting occurrence of negative CSF <span class="hlt">pressure</span> inside the cranium in animals with normal cranio-spinal communication was observed. CSF <span class="hlt">pressure</span> <span class="hlt">gradients</span> change depending on the body position, but those <span class="hlt">gradients</span> do not enable unidirectional CSF circulation from the hypothetical site of secretion to the site of absorption in any of them. Thus, our results indicate the existence of new physiological/pathophysiological correlations between intracranial fluids, which opens up the possibility of new therapeutic approaches to intracranial hypertension. PMID:24748150</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_7 --> <div id="page_8" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="141"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24748150','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24748150"><span>The influence of body position on cerebrospinal fluid <span class="hlt">pressure</span> <span class="hlt">gradient</span> and movement in cats with normal and impaired craniospinal communication.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Klarica, Marijan; Radoš, Milan; Erceg, Gorislav; Petošić, Antonio; Jurjević, Ivana; Orešković, Darko</p> <p>2014-01-01</p> <p>Intracranial hypertension is a severe therapeutic problem, as there is insufficient knowledge about the physiology of cerebrospinal fluid (CSF) <span class="hlt">pressure</span>. In this paper a new CSF <span class="hlt">pressure</span> regulation hypothesis is proposed. According to this hypothesis, the CSF <span class="hlt">pressure</span> depends on the laws of fluid mechanics and on the anatomical characteristics inside the cranial and spinal space, and not, as is today generally believed, on CSF secretion, circulation and absorption. The volume and <span class="hlt">pressure</span> changes in the newly developed CSF model, which by its anatomical dimensions and basic biophysical features imitates the craniospinal system in cats, are compared to those obtained on cats with and without the blockade of craniospinal communication in different body positions. During verticalization, a long-lasting occurrence of negative CSF <span class="hlt">pressure</span> inside the cranium in animals with normal cranio-spinal communication was observed. CSF <span class="hlt">pressure</span> <span class="hlt">gradients</span> change depending on the body position, but those <span class="hlt">gradients</span> do not enable unidirectional CSF circulation from the hypothetical site of secretion to the site of absorption in any of them. Thus, our results indicate the existence of new physiological/pathophysiological correlations between intracranial fluids, which opens up the possibility of new therapeutic approaches to intracranial hypertension.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22972446','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22972446"><span>Preretinal partial <span class="hlt">pressure</span> of oxygen <span class="hlt">gradients</span> before and after experimental pars plana vitrectomy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Petropoulos, Ioannis K; Pournaras, Jean-Antoine C; Stangos, Alexandros N; Pournaras, Constantin J</p> <p>2013-01-01</p> <p>To evaluate preretinal partial <span class="hlt">pressure</span> of oxygen (PO2) <span class="hlt">gradients</span> before and after experimental pars plana vitrectomy. Arteriolar, venous, and intervascular preretinal PO2 <span class="hlt">gradients</span> were recorded in 7 minipigs during slow withdrawal of oxygen-sensitive microelectrodes (10-μm tip diameter) from the vitreoretinal interface to 2 mm into the vitreous cavity. Recordings were repeated after pars plana vitrectomy and balanced salt solution (BSS) intraocular perfusion. Arteriolar, venous, and intervascular preretinal PO2 at the vitreoretinal interface were 62.3 ± 13.8, 22.5 ± 3.3, and 17.0 ± 7.5 mmHg, respectively, before vitrectomy; 97.7 ± 19.9, 40.0 ± 21.9, and 56.3 ± 28.4 mmHg, respectively, immediately after vitrectomy; and 59.0 ± 27.4, 25.2 ± 3.0, and 21.5 ± 4.5 mmHg, respectively, 2½ hours after interruption of BSS perfusion. PO2 2 mm from the vitreoretinal interface was 28.4 ± 3.6 mmHg before vitrectomy; 151.8 ± 4.5 mmHg immediately after vitrectomy; and 34.8 ± 4.1 mmHg 2½ hours after interruption of BSS perfusion. PO2 <span class="hlt">gradients</span> were still present after vitrectomy, with the same patterns as before vitrectomy. Preretinal PO2 <span class="hlt">gradients</span> are not eliminated after pars plana vitrectomy. During BSS perfusion, vitreous cavity PO2 is very high. Interruption of BSS perfusion evokes progressive equilibration of vitreous cavity PO2 with concomitant progressive return of preretinal PO2 <span class="hlt">gradients</span> to their previtrectomy patterns. This indicates that preretinal diffusion of oxygen is not altered after vitrectomy. The beneficial effect of vitrectomy in ischemic retinal diseases or macular edema may be related to other mechanisms, such as increased oxygen convection currents or removal of growth factors and cytokines secreted in the vitreous.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5402700','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5402700"><span>Elimination of Trans-coarctation <span class="hlt">Pressure</span> <span class="hlt">Gradients</span> Has No Impact on Left Ventricular Function or Aortic Shear Stress Post Intervention in Patients with Mild Coarctation</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Keshavarz-Motamed, Zahra; Nezami, Farhad Rikhtegar; Partida, Ramon A.; Nakamura, Kenta; Staziaki, Pedro Vinícius; Ben-Assa, Eyal; Ghoshhajra, Brian; Bhatt, Ami B.; Edelman, Elazer R.</p> <p>2017-01-01</p> <p>OBJECTIVES To investigate the impact of transcatheter intervention on left ventricular (LV) function and aortic hemodynamics in patients with mild coarctation of the aorta (COA). BACKGROUND The optimal method and timing of transcatheter intervention for COA remains unclear, especially when the severity of COA is mild (peak-to-peak trans-coarctation <span class="hlt">pressure</span> <span class="hlt">gradient</span>, PKdP < 20 mmHg). Debate rages regarding the risk/benefit ratio of intervention vs. long-term effects of persistent minimal <span class="hlt">gradient</span> in this heterogeneous population with differing blood <span class="hlt">pressures</span>, ventricular function and peripheral perfusion. METHODS We developed a unique computational fluid dynamics and lumped parameter modeling framework based on patient-specific hemodynamic input parameters and validated it against patient-specific clinical outcomes (pre- and post-intervention). We used clinically measured hemodynamic metrics and imaging of the aorta and the LV in thirty-four patients with mild COA to make these correlations. RESULTS Despite dramatic reduction in trans-coarctation <span class="hlt">pressure</span> <span class="hlt">gradient</span> (catheter and Doppler echocardiography <span class="hlt">pressure</span> <span class="hlt">gradients</span> reduced 75% and 47.3%,), there was only modest effect on aortic flow and no significant impact on aortic shear stress (maximum time-averaged wall shear stress in descending aorta was reduced 5.1%). In no patient did transcatheter intervention improve LV function (e.g., stroke work and normalized stroke work were reduced by only 4.48% and 3.9%). CONCLUSIONS Transcatheter intervention which successfully relieves mild COA <span class="hlt">pressure</span> <span class="hlt">gradients</span> does not translate to decrease myocardial strain. The effects of intervention were determined to the greatest degree by ventricular-vascular coupling hemodynamics, and provide a novel valuable mechanism to evaluate patients with COA which may influence clinical practice. PMID:27659574</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDG17002W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDG17002W"><span>Effects of surface roughness on an adverse-<span class="hlt">pressure-gradient</span> separating turbulent boundary layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wu, Wen; Piomelli, Ugo; Turbulence Simulation; Modelling Laboratory Team</p> <p>2017-11-01</p> <p>Separating turbulent boundary layers over smooth and rough flat plates are investigated by large-eddy simulations. A suction-blowing velocity distribution is imposed at the top boundary to produce an adverse-to-favourable <span class="hlt">pressure</span> <span class="hlt">gradient</span> and a closed separation bubble. Sandgrain roughness in the fully-rough regime is modelled by an immersed boundary method. In the rough-wall case, streamline detachment occurs earlier and the separation region is substantially larger due to the momentum deficit caused by the roughness. The adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> decreases the form drag and causes a thin reversed-flow region below the roughness crest, so that Cf = 0 does not coincide with the detachment of the flow from the surface. The wake regions behind roughness elements affect the intermittency of the near-wall flow, so that upstream of the detachment point the flow can be reversed half of the time, but its average is positive. The separated shear layer exhibits higher turbulent kinetic energy (TKE); the growth of the TKE there begins earlier relative to the separation point, and the peak TKE occurs close to the separation point. The momentum deficit caused by the roughness, again, plays a critical role in these changes. The authors acknowledge the support from Hydro-Québec and the NSERC Collaborative Research & Development program (CRDPJ 418786-11). The simulations were performed at CAC Queen't site. UP also thanks the support of Canada Research Chair Program.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25502599','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25502599"><span>Characterization of the startup transient electrokinetic flow in rectangular channels of arbitrary dimensions, zeta potential distribution, and time-varying <span class="hlt">pressure</span> <span class="hlt">gradient</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Miller, Andrew; Villegas, Arturo; Diez, F Javier</p> <p>2015-03-01</p> <p>The solution to the startup transient EOF in an arbitrary rectangular microchannel is derived analytically and validated experimentally. This full 2D transient solution describes the evolution of the flow through five distinct periods until reaching a final steady state. The derived analytical velocity solution is validated experimentally for different channel sizes and aspect ratios under time-varying <span class="hlt">pressure</span> <span class="hlt">gradients</span>. The experiments used a time resolved micro particle image velocimetry technique to calculate the startup transient velocity profiles. The measurements captured the effect of time-varying <span class="hlt">pressure</span> <span class="hlt">gradient</span> fields derived in the analytical solutions. This is tested by using small reservoirs at both ends of the channel which allowed a time-varying <span class="hlt">pressure</span> <span class="hlt">gradient</span> to develop with a time scale on the order of the transient EOF. Results showed that under these common conditions, the effect of the <span class="hlt">pressure</span> build up in the reservoirs on the temporal development of the transient startup EOF in the channels cannot be neglected. The measurements also captured the analytical predictions for channel walls made of different materials (i.e., zeta potentials). This was tested in channels that had three PDMS and one quartz wall, resulting in a flow with an asymmetric velocity profile due to variations in the zeta potential between the walls. © 2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhCS1001a2001A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS1001a2001A"><span>Reynolds stress structures in a self-similar adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> turbulent boundary layer at the verge of separation.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Atkinson, C.; Sekimoto, A.; Jiménez, J.; Soria, J.</p> <p>2018-04-01</p> <p>Mean Reynolds stress profiles and instantaneous Reynolds stress structures are investigated in a self-similar adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> turbulent boundary layer (APG-TBL) at the verge of separation using data from direct numerical simulations. The use of a self-similar APG-TBL provides a flow domain in which the flow gradually approaches a constant non-dimensional <span class="hlt">pressure</span> <span class="hlt">gradient</span>, resulting in a flow in which the relative contribution of each term in the governing equations is independent of streamwise position over a domain larger than two boundary layer thickness. This allows the flow structures to undergo a development that is less dependent on the upstream flow history when compared to more rapidly decelerated boundary layers. This APG-TBL maintains an almost constant shape factor of H = 2.3 to 2.35 over a momentum thickness based Reynolds number range of Re δ 2 = 8420 to 12400. In the APG-TBL the production of turbulent kinetic energy is still mostly due to the correlation of streamwise and wall-normal fluctuations, 〈uv〉, however the contribution form the other components of the Reynolds stress tensor are no longer negligible. Statistical properties associated with the scale and location of sweeps and ejections in this APG-TBL are compared with those of a zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> turbulent boundary layer developing from the same inlet profile, resulting in momentum thickness based range of Re δ 2 = 3400 to 3770. In the APG-TBL the peak in both the mean Reynolds stress and the production of turbulent kinetic energy move from the near wall region out to a point consistent with the displacement thickness height. This is associated with a narrower distribution of the Reynolds stress and a 1.6 times higher relative number of wall-detached negative uv structures. These structures occupy 5 times less of the boundary layer volume and show a similar reduction in their streamwise extent with respect to the boundary layer thickness. A significantly lower percentage</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvE..96c3114S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvE..96c3114S"><span>Luminescence from cavitation bubbles deformed in uniform <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Supponen, Outi; Obreschkow, Danail; Kobel, Philippe; Farhat, Mohamed</p> <p>2017-09-01</p> <p>Presented here are observations that demonstrate how the deformation of millimetric cavitation bubbles by a uniform <span class="hlt">pressure</span> <span class="hlt">gradient</span> quenches single-collapse luminescence. Our innovative measurement system captures a broad luminescence spectrum (wavelength range, 300-900 nm) from the individual collapses of laser-induced bubbles in water. By varying the bubble size, driving <span class="hlt">pressure</span>, and perceived gravity level aboard parabolic flights, we probed the limit from aspherical to highly spherical bubble collapses. Luminescence was detected for bubbles of maximum radii within the previously uncovered range, R0=1.5 -6 mm, for laser-induced bubbles. The relative luminescence energy was found to rapidly decrease as a function of the bubble asymmetry quantified by the anisotropy parameter ζ , which is the dimensionless equivalent of the Kelvin impulse. As established previously, ζ also dictates the characteristic parameters of bubble-driven microjets. The threshold of ζ beyond which no luminescence is observed in our experiment closely coincides with the threshold where the microjets visibly pierce the bubble and drive a vapor jet during the rebound. The individual fitted blackbody temperatures range between Tlum=7000 and Tlum=11 500 K but do not show any clear trend as a function of ζ . Time-resolved measurements using a high-speed photodetector disclose multiple luminescence events at each bubble collapse. The averaged full width at half-maximum of the pulse is found to scale with R0 and to range between 10 and 20 ns.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790054016&hterms=1043&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3D%2526%25231043','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790054016&hterms=1043&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3D%2526%25231043"><span>Gap heating with <span class="hlt">pressure</span> <span class="hlt">gradients</span>. [for Shuttle Orbiter thermal protection system tiles</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Scott, C. D.; Maraia, R. J.</p> <p>1979-01-01</p> <p>The heating rate distribution and temperature response on the gap walls of insulating tiles is analyzed to determine significant phenomena and parameters in flows where there is an external surface <span class="hlt">pressure</span> <span class="hlt">gradient</span>. Convective heating due to gap flow, modeled as fully developed pipe flow, is coupled with a two-dimensional thermal model of the tiles that includes conduction and radiative heat transfer. To account for geometry and important environmental parameters, scale factors are obtained by curve-fitting measured temperatures to analytical solutions. These scale factors are then used to predict the time-dependent gap heat flux and temperature response of tile gaps on the Space Shuttle Orbiter during entry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29049384','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29049384"><span><span class="hlt">Ideal</span> cardiovascular health predicts lower risk of abnormal liver enzymes levels in the Chilean National Health Survey (2009-2010).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>García-Hermoso, Antonio; Hackney, Anthony C; Ramírez-Vélez, Robinson</p> <p>2017-01-01</p> <p>High levels of gamma glutamyltransferase (gamma-GT) and alanine aminotransferase (ALT), as well as fatty liver index (FLI) has been associated with higher cardiovascular disease risk factors in adults. The aim of this study was to examine the relationship between gamma-GT, ALT, and fatty liver index FLI levels across a <span class="hlt">gradient</span> number of <span class="hlt">ideal</span> cardiovascular health metrics in a representative sample of adults from the Chilean National Health Survey 2009-2010. Data from 1,023 men and 1,449 women (≥ 15 years) from the Chilean Health Survey 2009-2010 were analyzed. <span class="hlt">Ideal</span> cardiovascular health was defined as meeting <span class="hlt">ideal</span> levels of the following components: four behaviours (smoking, body mass index, physical activity and diet adherence) and three factors (total cholesterol, blood <span class="hlt">pressure</span> and fasting glucose). Adults were grouped into three categories according to their number of <span class="hlt">ideal</span> cardiovascular health metrics: <span class="hlt">ideal</span> (5-7 metrics), intermediate (3-4 metrics), and poor (0-2 metrics). Blood levels of gamma-GT and ALT were measured and the FLI was calculated. A higher number of <span class="hlt">ideal</span> cardiovascular health index metric was associated with lower gamma-GT, ALT and FLI (p from trend analysis <0.001). Also, adults meeting at least 3-4 metrics were predicted less likely to have prevalence of abnormal levels of gamma-GT and FLI (p<0.001) compared to adults who met only 0-2 metrics. These findings reinforce the usefulness of the <span class="hlt">ideal</span> cardiovascular health metrics proposed by the American Heart Association as a tool to identify target subjects and promote cardiovascular health in South-American adults.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25506260','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25506260"><span>Changes in intracranial <span class="hlt">pressure</span> <span class="hlt">gradients</span> between the cerebral hemispheres in patients with intracerebral hematomas in one cerebral hemisphere.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Qiu, Wusi; Jiang, Qizhou; Xiao, Guoming; Wang, Weiming; Shen, Hong</p> <p>2014-01-01</p> <p>Intracranial-<span class="hlt">pressure</span> (ICP) monitoring is useful for patients with increased ICP following hemorrhagic stroke. In this study, the changes in <span class="hlt">pressure</span> <span class="hlt">gradients</span> between the two cerebral hemispheres were investigated after hemorrhagic stroke of one side, and after a craniotomy. Twenty-four patients with acute cerebral hemorrhages and intracerebral hematomas who exhibited mass effect and midline shift to the contralateral side on computed tomography were selected for this study. After admission, both sides of the cranium were drilled, and optical fiber sensors were implanted to monitor the brain parenchyma <span class="hlt">pressure</span> (BPP) in both cerebral hemispheres. All patients underwent surgical hematoma evacuations. The preoperative and postoperative BPP data from both cerebral hemispheres were collected at various time points and compared pairwise. There were statistically significant differences (P < 0.01) in the preoperative BPP values between the two hemispheres at three different time points. Differences in the BPP values between the two hemispheres at the time of surgery, and 24 and 48 h after surgery, were not statistically significant (P > 0.05). The posteroperative BPPs of both hemispheres were statistically significantly lower than preoperative recordings. BPP sensors should be applied to the injured cerebral hemisphere, because this becomes the source of increased ICP. Hematoma evacuation surgery effectively decreases ICP and eliminates <span class="hlt">pressure</span> <span class="hlt">gradients</span> between the two cerebral hemispheres, consequently enabling brain shift correction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27185055','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27185055"><span>Intrinsic advantages of packed capillaries over narrow-bore columns in very high-<span class="hlt">pressure</span> <span class="hlt">gradient</span> liquid chromatography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gritti, Fabrice; McDonald, Thomas; Gilar, Martin</p> <p>2016-06-17</p> <p>250μm×100mm fused silica glass capillaries were packed with 1.8μm high-strength silica (HSS) fully porous particles. They were prepared without bulky stainless steel endfittings and metal frits, which both generate significant sample dispersion. The isocratic efficiencies and <span class="hlt">gradient</span> peak capacities of these prototype capillary columns were measured for small molecules (n-alkanophenones) using a home-made ultra-low dispersive micro-HPLC instrument. Their resolution power was compared to that of standard 2.1mm×100mm very high-<span class="hlt">pressure</span> liquid chromatography (vHPLC) narrow-bore columns packed with the same particles. The results show that, for the same column efficiency (25000 plates) and <span class="hlt">gradient</span> steepness (0.04min(-1)), the peak capacity of the 250μm i.d. capillary columns is systematically 15-20% higher than that of the 2.1mm i.d. narrow-bore columns. A validated model of <span class="hlt">gradient</span> chromatography enabled one to predict accurately the observed peak capacities of the capillary columns for non-linear solvation strength retention behavior and under isothermal conditions. Thermodynamics applied to the eluent quantified the temperature difference for the thermal <span class="hlt">gradients</span> in both capillary and narrow-bore columns. Experimental data revealed that the <span class="hlt">gradient</span> peak capacity is more affected by viscous heating than the column efficiency. Unlike across 2.1mm i.d. columns, the changes in eluent composition across the 250μm i.d. columns during the <span class="hlt">gradient</span> is rapidly relaxed by transverse dispersion. The combination of (1) the absence of viscous heating and (2) the high uniformity of the eluent composition across the diameter of capillary columns explains the intrinsic advantage of capillary over narrow-bore columns in <span class="hlt">gradient</span> vHPLC. Copyright © 2016 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24296292','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24296292"><span>Very high <span class="hlt">pressure</span> liquid chromatography using fully porous particles: quantitative analysis of fast <span class="hlt">gradient</span> separations without post-run times.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Stankovich, Joseph J; Gritti, Fabrice; Stevenson, Paul G; Beaver, Lois Ann; Guiochon, Georges</p> <p>2014-01-10</p> <p>Using a column packed with fully porous particles, four methods for controlling the flow rates at which <span class="hlt">gradient</span> elution runs are conducted in very high <span class="hlt">pressure</span> liquid chromatography (VHPLC) were tested to determine whether reproducible thermal conditions could be achieved, such that subsequent analyses would proceed at nearly the same initial temperature. In VHPLC high flow rates are achieved, producing fast analyses but requiring high inlet <span class="hlt">pressures</span>. The combination of high flow rates and high inlet <span class="hlt">pressures</span> generates local heat, leading to temperature changes in the column. Usually in this case a post-run time is input into the analytical method to allow the return of the column temperature to its initial state. An alternative strategy involves operating the column without a post-run equilibration period and maintaining constant temperature variations for subsequent analysis after conducting one or a few separations to bring the column to a reproducible starting temperature. A liquid chromatography instrument equipped with a <span class="hlt">pressure</span> controller was used to perform constant <span class="hlt">pressure</span> and constant flow rate VHPLC separations. Six replicate <span class="hlt">gradient</span> separations of a nine component mixture consisting of acetophenone, propiophenone, butyrophenone, valerophenone, hexanophenone, heptanophenone, octanophenone, benzophenone, and acetanilide dissolved in water/acetonitrile (65:35, v/v) were performed under various experimental conditions: constant flow rate, two sets of constant <span class="hlt">pressure</span>, and constant <span class="hlt">pressure</span> operation with a programmed flow rate. The relative standard deviations of the response factors for all the analytes are lower than 5% across the methods. Programming the flow rate to maintain a fairly constant <span class="hlt">pressure</span> instead of using instrument controlled constant <span class="hlt">pressure</span> improves the reproducibility of the retention times by a factor of 5, when plotting the chromatograms in time. Copyright © 2013 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70034727','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70034727"><span><span class="hlt">Pressure-gradient</span>-driven nearshore circulation on a beach influenced by a large inlet-tidal shoal system</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Shi, F.; Hanes, D.M.; Kirby, J.T.; Erikson, L.; Barnard, P.; Eshleman, J.</p> <p>2011-01-01</p> <p>The nearshore circulation induced by a focused pattern of surface gravity waves is studied at a beach adjacent to a major inlet with a large ebb tidal shoal. Using a coupled wave and wave-averaged nearshore circulation model, it is found that the nearshore circulation is significantly affected by the heterogeneous wave patterns caused by wave refraction over the ebb tidal shoal. The model is used to predict waves and currents during field experiments conducted near the mouth of San Francisco Bay and nearby Ocean Beach. The field measurements indicate strong spatial variations in current magnitude and direction and in wave height and direction along Ocean Beach and across the ebb tidal shoal. Numerical simulations suggest that wave refraction over the ebb tidal shoal causes wave focusing toward a narrow region at Ocean Beach. Due to the resulting spatial variation in nearshore wave height, wave-induced setup exhibits a strong alongshore nonuniformity, resulting in a dramatic change in the <span class="hlt">pressure</span> field compared to a simulation with only tidal forcing. The analysis of momentum balances inside the surf zone shows that, under wave conditions with intensive wave focusing, the alongshore <span class="hlt">pressure</span> <span class="hlt">gradient</span> associated with alongshore nonuniform wave setup can be a dominant force driving circulation, inducing heterogeneous alongshore currents. <span class="hlt">Pressure-gradient</span>- forced alongshore currents can exhibit flow reversals and flow convergence or divergence, in contrast to the uniform alongshore currents typically caused by tides or homogeneous waves.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29764373','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29764373"><span>A subclinical high tricuspid regurgitation <span class="hlt">pressure</span> <span class="hlt">gradient</span> independent of the mean pulmonary artery <span class="hlt">pressure</span> is a risk factor for the survival after living donor liver transplantation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Saragai, Yosuke; Takaki, Akinobu; Umeda, Yuzo; Matsusaki, Takashi; Yasunaka, Tetsuya; Oyama, Atsushi; Kaku, Ryuji; Nakamura, Kazufumi; Yoshida, Ryuichi; Nobuoka, Daisuke; Kuise, Takashi; Takagi, Kosei; Adachi, Takuya; Wada, Nozomu; Takeuchi, Yasuto; Koike, Kazuko; Ikeda, Fusao; Onishi, Hideki; Shiraha, Hidenori; Nakamura, Shinichiro; Morimatsu, Hiroshi; Ito, Hiroshi; Fujiwara, Toshiyoshi; Yagi, Takahito; Okada, Hiroyuki</p> <p>2018-05-15</p> <p>Portopulmonary hypertension (POPH) is characterized by pulmonary vasoconstriction, while hepatopulmonary syndrome (HPS) is characterized by vasodilation. Definite POPH is a risk factor for the survival after orthotopic liver transplantation (OLT), as the congestive <span class="hlt">pressure</span> affects the grafted liver, while subclinical pulmonary hypertension (PH) has been acknowledged as a non-risk factor for deceased donor OLT. Given that PH measurement requires cardiac catheterization, the tricuspid regurgitation <span class="hlt">pressure</span> <span class="hlt">gradient</span> (TRPG) measured by echocardiography is used to screen for PH and congestive <span class="hlt">pressure</span> to the liver. We investigated the impact of a subclinical high TRPG on the survival of small grafted living donor liver transplantation (LDLT). We retrospectively analyzed 84 LDLT candidates. Patients exhibiting a TRPG ≥25 mmHg on echocardiography were categorized as potentially having liver congestion (subclinical high TRPG; n = 34). The mean pulmonary artery <span class="hlt">pressure</span> (mPAP) measured after general anesthesia with FIO 2 0.6 (mPAP-FIO 2 0.6) was also assessed. Patients exhibiting pO 2  < 80 mmHg and an alveolar-arterial oxygen <span class="hlt">gradient</span> (AaDO 2 ) ≥ 15 mmHg were categorized as potentially having HPS (subclinical HPS; n = 29). The clinical course after LDLT was investigated according to subclinical high TRPG. A subclinical high TRPG (p = 0.012) and older donor age (p = 0.008) were correlated with a poor 40-month survival. Although a higher mPAP-FIO 2 0.6 was expected to correlate with a worse survival, a high mPAP-FIO 2 0.6 with a low TRPG was associated with high frequency complicating subclinical HPS and a good survival, suggesting a reduction in the PH <span class="hlt">pressure</span> via pulmonary shunt. In cirrhosis patients, mPAP-FIO 2 0.6 may not accurately reflect the congestive <span class="hlt">pressure</span> to the liver, as the <span class="hlt">pressure</span> might escape via pulmonary shunt. A subclinical high TRPG is an important marker for predicting a worse survival after LDLT, possibly reflecting</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3880383','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3880383"><span>A <span class="hlt">pressure-gradient</span> mechanism for vortex shedding in constricted channels</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Boghosian, M. E.; Cassel, K. W.</p> <p>2013-01-01</p> <p>Numerical simulations of the unsteady, two-dimensional, incompressible Navier–Stokes equations are performed for a Newtonian fluid in a channel having a symmetric constriction modeled by a two-parameter Gaussian distribution on both channel walls. The Reynolds number based on inlet half-channel height and mean inlet velocity ranges from 1 to 3000. Constriction ratios based on the half-channel height of 0.25, 0.5, and 0.75 are considered. The results show that both the Reynolds number and constriction geometry have a significant effect on the behavior of the post-constriction flow field. The Navier–Stokes solutions are observed to experience a number of bifurcations: steady attached flow, steady separated flow (symmetric and asymmetric), and unsteady vortex shedding downstream of the constriction depending on the Reynolds number and constriction ratio. A sequence of events is described showing how a sustained spatially growing flow instability, reminiscent of a convective instability, leads to the vortex shedding phenomenon via a proposed streamwise <span class="hlt">pressure-gradient</span> mechanism. PMID:24399860</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6548360-assessment-stenosis-severity-correlation-angiography-t1-scintigraphy-intracoronary-pressure-gradients','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6548360-assessment-stenosis-severity-correlation-angiography-t1-scintigraphy-intracoronary-pressure-gradients"><span>Assessment of stenosis severity: Correlation of angiography, T1-201 scintigraphy, and intracoronary <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Bateman, T.; Raymond, M.; Czer, L.</p> <p>1984-01-01</p> <p>To clarify the relationship between angiographic and hemodynamic stenosis severity and the appearance during stress-redistribution myocardial T1-201 scintigraphy (Ex-T1) of a visual (V) or quantitative (Q) perfusion defect (PD) or washout (WO) abnormality, 24 pts with CAD underwent intracoronary <span class="hlt">pressure</span> <span class="hlt">gradient</span> study at bypass surgery (CABG). All had pre-CABG Ex-T1 without interval deterioration. The mean diastolic <span class="hlt">pressure</span> <span class="hlt">gradient</span> (MDG) measured at reproducible hyperemic flow rates was determined for 34 stenoses (13 LAD, 7 LCX, 14 RCA) and compared with the results of Ex-T1 in subtended myocardial regions (LAD=anterior; LCX=posterolateral; RCA=inferior). Fourteen stenoses (50-99% diameter narrowing) were unassociated with VPD despitemore » maximal exercise: MDG was 9 +- 5mmHg, with MDG/mean aortic diastolic <span class="hlt">pressure</span> (ADP) ratio of 0.12 +- 0.07. QPD and QWO analysis detected 8 of these. Thirteen stenoses (90-100% severity) led to reversible VPD: MDG was 36 +- 11 mm Hg, MDG/ADP ratio was 0.52 +- 0.17, and Q analysis was abnormal in 12/13. Seven stenoses (90-100% severity) subtended infarcted myocardium: MDG was 42 +- 21 mm Hg, MDG/ADP ratio was 0.52 +- 0.18, and V and Q analyses were abnormal in all. From this study, the authors derive the following conclusion: 1) Ex-T1 correlates better with hemodynamic severity of stenoses than does angiography; 2) V abnormalities identify stenoses of major angiographic and hemodynamic severity, while Q analysis detects some (57% in this study) stenoses of lesser severity; and 3) stenoses causing reversible Ex-T1 abnormalities present similar hemodynamic impediments to those causing myocardial infarcts.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20628534','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20628534"><span>Reported Effects of Masculine <span class="hlt">Ideals</span> on Gay Men.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sánchez, Francisco J; Greenberg, Stefanie T; Liu, William Ming; Vilain, Eric</p> <p>2009-01-01</p> <p>This exploratory study used consensual qualitative research methodology (Hill et al., 2005) to analyze what gay men associate with masculinity and femininity, how they feel masculine <span class="hlt">ideals</span> affect their self-image, and how masculine <span class="hlt">ideals</span> affect their same-sex relationships. Written responses were collected from 547 self-identified gay men in the U.S. via an Internet-based survey. Findings supported previous reports that perceptions of gender roles among gay men appear based on masculine and feminine stereotypes. Additionally, more adverse versus positive effects on self-image and same-sex romantic relationships were reported including difficulty being emotional and affectionate, <span class="hlt">pressure</span> to be physically attractive, and <span class="hlt">pressure</span> to appear masculine in order to be accepted by society and to be seen as desirable by other gay men. While research on gay men's experience with masculinity continues, psychologists should consider the possible influence of traditional masculine <span class="hlt">ideals</span> when conceptualizing their gay male clients.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2902177','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2902177"><span>Reported Effects of Masculine <span class="hlt">Ideals</span> on Gay Men</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Sánchez, Francisco J.; Greenberg, Stefanie T.; Liu, William Ming; Vilain, Eric</p> <p>2010-01-01</p> <p>This exploratory study used consensual qualitative research methodology (Hill et al., 2005) to analyze what gay men associate with masculinity and femininity, how they feel masculine <span class="hlt">ideals</span> affect their self-image, and how masculine <span class="hlt">ideals</span> affect their same-sex relationships. Written responses were collected from 547 self-identified gay men in the U.S. via an Internet-based survey. Findings supported previous reports that perceptions of gender roles among gay men appear based on masculine and feminine stereotypes. Additionally, more adverse versus positive effects on self-image and same-sex romantic relationships were reported including difficulty being emotional and affectionate, <span class="hlt">pressure</span> to be physically attractive, and <span class="hlt">pressure</span> to appear masculine in order to be accepted by society and to be seen as desirable by other gay men. While research on gay men’s experience with masculinity continues, psychologists should consider the possible influence of traditional masculine <span class="hlt">ideals</span> when conceptualizing their gay male clients. PMID:20628534</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730012553','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730012553"><span>The behavior of a compressible turbulent boundary layer in a shock-wave-induced adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span>. Ph.D. Thesis - Washington Univ., Seattle, Aug. 1972</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rose, W. C.</p> <p>1973-01-01</p> <p>The results of an experimental investigation of the mean- and fluctuating-flow properties of a compressible turbulent boundary layer in a shock-wave-induced adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> are presented. The turbulent boundary layer developed on the wall of an axially symmetric nozzle and test section whose nominal free-stream Mach number and boundary-layer thickness Reynolds number were 4 and 100,000, respectively. The adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> was induced by an externally generated conical shock wave. Mean and time-averaged fluctuating-flow data, including the complete experimental Reynolds stress tensor and experimental turbulent mass- and heat-transfer rates are presented for the boundary layer and external flow, upstream, within and downstream of the <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The mean-flow data include distributions of total temperature throughout the region of interest. The turbulent mixing properties of the flow were determined experimentally with a hot-wire anemometer. The calibration of the wires and the interpretation of the data are discussed. From the results of the investigation, it is concluded that the shock-wave - boundary-layer interaction significantly alters the turbulent mixing characteristics of the boundary layer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22617069','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22617069"><span>[Diagnostic importance of the alveolar-arterial oxygen <span class="hlt">gradient</span>].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Weinans, Marije A E; Drost-de Klerck, Amanda M; ter Maaten, Jan C</p> <p>2012-01-01</p> <p>The alveolar-arterial (A-a) oxygen <span class="hlt">gradient</span> is the difference between the partial <span class="hlt">pressure</span> of oxygen in the alveoli and the partial <span class="hlt">pressure</span> of arterial oxygen and can be elevated in the case of pulmonary disease. We describe a 41-year-old patient with pneumonia who presented with abdominal pain, in whom calculation of the A-a <span class="hlt">gradient</span> could have led to earlier diagnosis. The A-a oxygen <span class="hlt">gradient</span> is mainly of diagnostic importance and the presented nomogram allows easy and quick interpretation. This might lead to a more frequent use of the A-a oxygen <span class="hlt">gradient</span> in the future.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_8 --> <div id="page_9" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="161"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900014354','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900014354"><span>Aerodynamic <span class="hlt">pressure</span> and heating-rate distributions in tile gaps around chine regions with <span class="hlt">pressure</span> <span class="hlt">gradients</span> at a Mach number of 6.6</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hunt, L. Roane; Notestine, Kristopher K.</p> <p>1990-01-01</p> <p>Surface and gap <span class="hlt">pressures</span> and heating-rate distributions were obtained for simulated Thermal Protection System (TPS) tile arrays on the curved surface test apparatus of the Langley 8-Foot High Temperature Tunnel at Mach 6.6. The results indicated that the chine gap <span class="hlt">pressures</span> varied inversely with gap width because larger gap widths allowed greater venting from the gap to the lower model side <span class="hlt">pressures</span>. Lower gap <span class="hlt">pressures</span> caused greater flow ingress from the surface and increased gap heating. Generally, gap heating was greater in the longitudinal gaps than in the circumferential gaps. Gap heating decreased with increasing gap depth. Circumferential gap heating at the mid-depth was generally less than about 10 percent of the external surface value. Gap heating was most severe at local T-gap junctions and tile-to-tile forward-facing steps that caused the greatest heating from flow impingement. The use of flow stoppers at discrete locations reduced heating from flow impingement. The use of flow stoppers at discrete locations reduced heating in most gaps but increased heating in others. Limited use of flow stoppers or gap filler in longitudinal gaps could reduce gap heating in open circumferential gaps in regions of high surface <span class="hlt">pressure</span> <span class="hlt">gradients</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3635164','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3635164"><span>Investigating Individual- and Area-Level Socioeconomic <span class="hlt">Gradients</span> of Pulse <span class="hlt">Pressure</span> among Normotensive and Hypertensive Participants</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Matricciani, Lisa A.; Paquet, Catherine; Howard, Natasha J.; Adams, Robert; Coffee, Neil T.; Taylor, Anne W.; Daniel, Mark</p> <p>2013-01-01</p> <p>Socioeconomic status is a strong predictor of cardiovascular disease. Pulse <span class="hlt">pressure</span>, the difference between systolic and diastolic blood <span class="hlt">pressure</span>, has been identified as an important predictor of cardiovascular risk even after accounting for absolute measures of blood <span class="hlt">pressure</span>. However, little is known about the social determinants of pulse <span class="hlt">pressure</span>. The aim of this study was to examine individual- and area-level socioeconomic <span class="hlt">gradients</span> of pulse <span class="hlt">pressure</span> in a sample of 2,789 Australian adults. Using data from the North West Adelaide Health Study we estimated the association between pulse <span class="hlt">pressure</span> and three indices of socioeconomic status (education, income and employment status) at the area and individual level for hypertensive and normotensive participants, using Generalized Estimating Equations. In normotensive individuals, area-level education (estimate: −0.106; 95% CI: −0.172, −0.041) and individual-level income (estimate: −1.204; 95% CI: −2.357, −0.050) and employment status (estimate: −1.971; 95% CI: −2.894, −1.048) were significant predictors of pulse <span class="hlt">pressure</span>, even after accounting for the use of medication and lifestyle behaviors. In hypertensive individuals, only individual-level measures of socioeconomic status were significant predictors of pulse <span class="hlt">pressure</span> (education estimate: −2.618; 95% CI: −4.878, −0.357; income estimate: −1.683, 95% CI: −3.743, 0.377; employment estimate: −2.023; 95% CI: −3.721, −0.326). Further research is needed to better understand how individual- and area-level socioeconomic status influences pulse <span class="hlt">pressure</span> in normotensive and hypertensive individuals. PMID:23380912</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4437633','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4437633"><span>Ex-Vivo Lymphatic Perfusion System for Independently Controlling <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> and Transmural <span class="hlt">Pressure</span> in Isolated Vessels</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kornuta, Jeffrey A.; Dixon, J. Brandon</p> <p>2015-01-01</p> <p>In addition to external forces, collecting lymphatic vessels intrinsically contract to transport lymph from the extremities to the venous circulation. As a result, the lymphatic endothelium is routinely exposed to a wide range of dynamic mechanical forces, primarily fluid shear stress and circumferential stress, which have both been shown to affect lymphatic pumping activity. Although various ex-vivo perfusion systems exist to study this innate pumping activity in response to mechanical stimuli, none are capable of independently controlling the two primary mechanical forces affecting lymphatic contractility: transaxial <span class="hlt">pressure</span> <span class="hlt">gradient</span>, ΔP, which governs fluid shear stress; and average transmural <span class="hlt">pressure</span>, Pavg, which governs circumferential stress. Hence, the authors describe a novel ex-vivo lymphatic perfusion system (ELPS) capable of independently controlling these two outputs using a linear, explicit model predictive control (MPC) algorithm. The ELPS is capable of reproducing arbitrary waveforms within the frequency range observed in the lymphatics in vivo, including a time-varying ΔP with a constant Pavg, time-varying ΔP and Pavg, and a constant ΔP with a time-varying Pavg. In addition, due to its implementation of syringes to actuate the working fluid, a post-hoc method of estimating both the flow rate through the vessel and fluid wall shear stress over multiple, long (5 sec) time windows is also described. PMID:24809724</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28606683','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28606683"><span>Prevalence of <span class="hlt">ideal</span> cardiovascular health in European adolescents: The HELENA study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Henriksson, Pontus; Henriksson, Hanna; Gracia-Marco, Luis; Labayen, Idoia; Ortega, Francisco B; Huybrechts, Inge; España-Romero, Vanesa; Manios, Yannis; Widhalm, Kurt; Dallongeville, Jean; González-Gross, Marcela; Marcos, Ascensión; Moreno, Luis A; Castillo, Manuel J; Ruiz, Jonatan R</p> <p>2017-08-01</p> <p>The <span class="hlt">ideal</span> cardiovascular health (iCVH) construct consists of 4 health behaviours and 3 health factors and is strongly related to later cardiovascular disease. However, the prevalence of iCVH in European adolescents is currently unknown. The Healthy Lifestyle in Europe by Nutrition in Adolescence (HELENA) study is a cross-sectional, multicentre study conducted in 9 European countries during 2006-2007 and included 3528 adolescents (1683 boys and 1845 girls) between 12.5 and 17.5years of age. Status (<span class="hlt">ideal</span> vs. non-<span class="hlt">ideal</span>) for the health behaviours (smoking status, body mass index, physical activity and diet) and health factors (total cholesterol, blood <span class="hlt">pressure</span> and fasting glucose) were determined. Overall, the prevalence of <span class="hlt">ideal</span> health behaviours was low; non-smoking (60.9% <span class="hlt">ideal</span>), body mass index (76.8%), physical activity (62.1%), and diet (1.7%). The prevalence of <span class="hlt">ideal</span> health factors was; total cholesterol (65.8%), blood <span class="hlt">pressure</span> (62.0%) and plasma glucose (88.8%). The low prevalence of iCVH behaviours, especially diet and physical activity, identified in European adolescents is likely to influence later cardiovascular health which strongly motivates efforts to increase <span class="hlt">ideal</span> health behaviours in this population. Copyright © 2017 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25138664','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25138664"><span>The role of jet eccentricity in generating disproportionately elevated transaortic <span class="hlt">pressure</span> <span class="hlt">gradients</span> in patients with aortic stenosis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Abbas, Amr E; Franey, Laura M; Lester, Steven; Raff, Gilbert; Gallagher, Michael J; Hanzel, George; Safian, Robert D; Pibarot, Philippe</p> <p>2015-02-01</p> <p>In patients with aortic stenosis (AS) and eccentric transaortic flow, greater <span class="hlt">pressure</span> loss occurs as the jet collides with the aortic wall together with delayed and diminished <span class="hlt">pressure</span> recovery. This leads to the elevated transaortic valve <span class="hlt">pressure</span> <span class="hlt">gradients</span> noted on both Doppler and cardiac catheterization. Such situations may present a diagnostic dilemma where traditional measures of stenosis severity indicate severe AS, while imaging modalities of the aortic valve geometric aortic valve area (GOA) suggest less than severe stenosis. In this study, we present a series of cases exemplifying this clinical dilemma and demonstrate how color M-mode, 2D and 3D transthoracic (TTE) and transesophageal (TEE) echocardiography, cardiac computed tomography angiography (CTA), and magnetic resonance imaging (MRI), may be used to resolve such discrepancies. © 2014, Wiley Periodicals, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27743249','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27743249"><span>The association between the pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> at the cranio-cervical junction derived from phase-contrast magnetic resonance imaging and invasively measured pulsatile intracranial <span class="hlt">pressure</span> in symptomatic patients with Chiari malformation type 1.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Frič, Radek; Lindstrøm, Erika Kristina; Ringstad, Geir Andre; Mardal, Kent-André; Eide, Per Kristian</p> <p>2016-12-01</p> <p>In symptomatic Chiari malformation type 1 (CMI), impaired intracranial compliance (ICC) is associated with an increased cranio-spinal pulsatile <span class="hlt">pressure</span> <span class="hlt">gradient</span>. Phase-contrast magnetic resonance imaging (MRI) represents a non-invasive modality for the assessment of the pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> at the cranio-cervical junction (CCJ). We wished to explore how the MRI-derived pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> (MRI-dP) compares with invasively measured pulsatile intracranial <span class="hlt">pressure</span> (ICP) in CMI, and with healthy controls. From phase-contrast MRI of CMI patients and healthy controls, we computed cerebrospinal fluid (CSF) flow velocities and MRI-dP at the CCJ. We assessed bidirectional flow and compared the flow between the anterior and the posterior subarachnoid space at the CCJ. We computed total intracranial volume (ICV), ventricular CSF volume (VV), and posterior cranial fossa volume (PCFV). We analyzed the static and pulsatile ICP scores from overnight monitoring in CMI patients. Five CMI patients and four healthy subjects were included. The CMI group had a significantly larger extent of tonsillar ectopia, smaller PCFV, and a smaller area of CSF in the FM. The pulsatile ICP (mean ICP wave amplitude, MWA) was abnormally increased in 4/5 CMI patients and correlated positively with MRI-dP. However, the MRI-dP as well as the CSF flow velocities did not differ significantly between CMI and healthy subjects. Moreover, bidirectional flow was observed in both CMI as well as healthy subjects, with no significant difference. In symptomatic CMI patients, we found a significant association between the pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> at the CCJ derived from phase-contrast MRI and the pulsatile ICP (MWA) measured invasively. However, the MRI-dP was close to identical in CMI patients and healthy subjects. Moreover, the CSF flow velocities at the CCJ and the occurrence of bidirectional flow were not different in CMI patients and healthy individuals. Further studies are required to determine the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19840015581','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840015581"><span>Investigation of the effects of <span class="hlt">pressure</span> <span class="hlt">gradient</span>, temperature and wall temperature ratio on the stagnation point heat transfer for circular cylinders and gas turbine vanes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nagamatsu, H. T.; Duffy, R. E.</p> <p>1984-01-01</p> <p>Low and high <span class="hlt">pressure</span> shock tubes were designed and constructed for the purpose of obtaining heat transfer data over a temperature range of 390 to 2500 K, <span class="hlt">pressures</span> of 0.3 to 42 atm, and Mach numbers of 0.15 to 1.5 with and without <span class="hlt">pressure</span> <span class="hlt">gradient</span>. A square test section with adjustable top and bottom walls was constructed to produce the favorable and adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> over the flat plate with heat gages. A water cooled gas turbine nozzle cascade which is attached to the high <span class="hlt">pressure</span> shock tube was obtained to measuse the heat flux over <span class="hlt">pressure</span> and suction surfaces. Thin-film platinum heat gages with a response time of a few microseconds were developed and used to measure the heat flux for laminar, transition, and turbulent boundary layers. The laminar boundary heat flux on the shock tube wall agreed with Mirel's flat plate theory. Stagnation point heat transfer for circular cylinders at low temperature compared with the theoretical prediction, but for a gas temperature of 922 K the heat fluxes were higher than the predicted values. Preliminary flat plate heat transfer data were measured for laminar, transition, and turbulent boundary layers with and without <span class="hlt">pressure</span> <span class="hlt">gradients</span> for free-stream temperatures of 350 to 2575 K and flow Mach numbers of 0.11 to 1.9. The experimental heat flux data were correlated with the laminar and turbulent theories and the agreement was good at low temperatures which was not the case for higher temperatures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5648121','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5648121"><span><span class="hlt">Ideal</span> cardiovascular health predicts lower risk of abnormal liver enzymes levels in the Chilean National Health Survey (2009–2010)</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Hackney, Anthony C.</p> <p>2017-01-01</p> <p>High levels of gamma glutamyltransferase (gamma-GT) and alanine aminotransferase (ALT), as well as fatty liver index (FLI) has been associated with higher cardiovascular disease risk factors in adults. The aim of this study was to examine the relationship between gamma-GT, ALT, and fatty liver index FLI levels across a <span class="hlt">gradient</span> number of <span class="hlt">ideal</span> cardiovascular health metrics in a representative sample of adults from the Chilean National Health Survey 2009–2010. Data from 1,023 men and 1,449 women (≥ 15 years) from the Chilean Health Survey 2009–2010 were analyzed. <span class="hlt">Ideal</span> cardiovascular health was defined as meeting <span class="hlt">ideal</span> levels of the following components: four behaviours (smoking, body mass index, physical activity and diet adherence) and three factors (total cholesterol, blood <span class="hlt">pressure</span> and fasting glucose). Adults were grouped into three categories according to their number of <span class="hlt">ideal</span> cardiovascular health metrics: <span class="hlt">ideal</span> (5–7 metrics), intermediate (3–4 metrics), and poor (0–2 metrics). Blood levels of gamma-GT and ALT were measured and the FLI was calculated. A higher number of <span class="hlt">ideal</span> cardiovascular health index metric was associated with lower gamma-GT, ALT and FLI (p from trend analysis <0.001). Also, adults meeting at least 3–4 metrics were predicted less likely to have prevalence of abnormal levels of gamma-GT and FLI (p<0.001) compared to adults who met only 0–2 metrics. These findings reinforce the usefulness of the <span class="hlt">ideal</span> cardiovascular health metrics proposed by the American Heart Association as a tool to identify target subjects and promote cardiovascular health in South-American adults. PMID:29049384</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16657786','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16657786"><span>Water potential <span class="hlt">gradient</span> in a tall sequoiadendron.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tobiessen, P</p> <p>1971-09-01</p> <p>With an elevator installed in a 90-meter tall Sequoiadendron to collect the samples, xylem <span class="hlt">pressure</span> potential measurements were made approximately every 15 meters along 60 meters of the tree's height. The measured <span class="hlt">gradient</span> was about -0.8 bar per 10 meters of height, i.e., less than the hydrostatic <span class="hlt">gradient</span>. Correction of the xylem <span class="hlt">pressure</span> potential data by calibration against a thermocouple psychrometer confirmed this result. Similar <span class="hlt">gradients</span> are described in the literature in tall conifers at times of low transpiration, although a different sampling technique was used. If the data in the present study and those supporting it are typical, they imply a re-evaluation of either the use of the <span class="hlt">pressure</span> chamber to estimate water potential or the present theories describing water transport in tall trees.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=396854','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=396854"><span>Water Potential <span class="hlt">Gradient</span> in a Tall Sequoiadendron</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Tobiessen, Peter; Rundel, Philip W.; Stecker, R. E.</p> <p>1971-01-01</p> <p>With an elevator installed in a 90-meter tall Sequoiadendron to collect the samples, xylem <span class="hlt">pressure</span> potential measurements were made approximately every 15 meters along 60 meters of the tree's height. The measured <span class="hlt">gradient</span> was about −0.8 bar per 10 meters of height, i.e., less than the hydrostatic <span class="hlt">gradient</span>. Correction of the xylem <span class="hlt">pressure</span> potential data by calibration against a thermocouple psychrometer confirmed this result. Similar <span class="hlt">gradients</span> are described in the literature in tall conifers at times of low transpiration, although a different sampling technique was used. If the data in the present study and those supporting it are typical, they imply a re-evaluation of either the use of the <span class="hlt">pressure</span> chamber to estimate water potential or the present theories describing water transport in tall trees. PMID:16657786</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19740025322','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19740025322"><span>Boundary-layer transition on a plate subjected to simultaneous spanwise and chordwise <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Boldman, D. R.; Brinich, P. F.</p> <p>1974-01-01</p> <p>The boundary-layer transition on a short plate was studied by means of the china-clay visual technique. The plate model was mounted in a wind tunnel so that it was subjected to small simultaneous spanwise and chordwise <span class="hlt">pressure</span> <span class="hlt">gradients</span>. Results of the experimental study, which was performed at three subsonic velocities, indicated that the transition pattern was appreciably curved in the spanwise direction but quite smooth and well behaved. Reasonable comparisons between predictions of transition and experiment were obtained from two finite-difference two-dimensional boundary-layer calculation methods which incorporated transition models based on the concept of a transition intermittency factor.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhDT.......146A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhDT.......146A"><span>Design and development of second order MEMS sound <span class="hlt">pressure</span> <span class="hlt">gradient</span> sensor</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Albahri, Shehab</p> <p></p> <p>The design and development of a second order MEMS sound <span class="hlt">pressure</span> <span class="hlt">gradient</span> sensor is presented in this dissertation. Inspired by the directional hearing ability of the parasitoid fly, Ormia ochracea, a novel first order directional microphone that mimics the mechanical structure of the fly's ears and detects the sound <span class="hlt">pressure</span> <span class="hlt">gradient</span> has been developed. While the first order directional microphones can be very beneficial in a large number of applications, there is great potential for remarkable improvements in performance through the use of second order systems. The second order directional microphone is able to provide a theoretical improvement in Sound to Noise ratio (SNR) of 9.5dB, compared to the first-order system that has its maximum SNR of 6dB. Although second order microphone is more sensitive to sound angle of incidence, the nature of the design and fabrication process imposes different factors that could lead to deterioration in its performance. The first Ormia ochracea second order directional microphone was designed in 2004 and fabricated in 2006 at Binghamton University. The results of the tested parts indicate that the Ormia ochracea second order directional microphone performs mostly as an Omni directional microphone. In this work, the previous design is reexamined and analyzed to explain the unexpected results. A more sophisticated tool implementing a finite element package ANSYS is used to examine the previous design response. This new tool is used to study different factors that used to be ignored in the previous design, mainly; response mismatch and fabrication uncertainty. A continuous model using Hamilton's principle is introduced to verify the results using the new method. Both models agree well, and propose a new way for optimizing the second order directional microphone using geometrical manipulation. In this work we also introduce a new fabrication process flow to increase the fabrication yield. The newly suggested method uses the shell</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22778438','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22778438"><span>Redox systematics of a magma ocean with variable <span class="hlt">pressure</span>-temperature <span class="hlt">gradients</span> and composition.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Righter, K; Ghiorso, M S</p> <p>2012-07-24</p> <p>Oxygen fugacity in metal-bearing systems controls some fundamental aspects of the geochemistry of the early Earth, such as the FeO and siderophile trace element content of the mantle, volatile species that influence atmospheric composition, and conditions for organic compounds synthesis. Redox and metal-silicate equilibria in the early Earth are sensitive to oxygen fugacity (fO(2)), yet are poorly constrained in modeling and experimentation. High <span class="hlt">pressure</span> and temperature experimentation and modeling in metal-silicate systems usually employs an approximation approach for estimating fO(2) that is based on the ratio of Fe and FeO [called "ΔIW (ratio)" hereafter]. We present a new approach that utilizes free energy and activity modeling of the equilibrium: Fe + SiO(2) + O(2) = Fe(2)SiO(4) to calculate absolute fO(2) and relative to the iron-wüstite (IW) buffer at <span class="hlt">pressure</span> and temperature [ΔIW (P,T)]. This equilibrium is considered across a wide range of <span class="hlt">pressures</span> and temperatures, including up to the liquidus temperature of peridotite (4,000 K at 50 GPa). Application of ΔIW (ratio) to metal-silicate experiments can be three or four orders of magnitude different from ΔIW (P,T) values calculated using free energy and activity modeling. We will also use this approach to consider the variation in oxygen fugacity in a magma ocean scenario for various thermal structures for the early Earth: hot liquidus <span class="hlt">gradient</span>, 100 °C below the liquidus, hot and cool adiabatic <span class="hlt">gradients</span>, and a cool subsolidus adiabat. The results are used to assess the effect of increasing P and T, changing silicate composition during accretion, and related to current models for accretion and core formation in the Earth. The fO(2) in a deep magma ocean scenario may become lower relative to the IW buffer at hotter and deeper conditions, which could include metal entrainment scenarios. Therefore, fO(2) may evolve from high to low fO(2) during Earth (and other differentiated bodies) accretion. Any</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3409746','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3409746"><span>Redox systematics of a magma ocean with variable <span class="hlt">pressure</span>-temperature <span class="hlt">gradients</span> and composition</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Righter, K.; Ghiorso, M. S.</p> <p>2012-01-01</p> <p>Oxygen fugacity in metal-bearing systems controls some fundamental aspects of the geochemistry of the early Earth, such as the FeO and siderophile trace element content of the mantle, volatile species that influence atmospheric composition, and conditions for organic compounds synthesis. Redox and metal-silicate equilibria in the early Earth are sensitive to oxygen fugacity (fO2), yet are poorly constrained in modeling and experimentation. High <span class="hlt">pressure</span> and temperature experimentation and modeling in metal-silicate systems usually employs an approximation approach for estimating fO2 that is based on the ratio of Fe and FeO [called “ΔIW (ratio)” hereafter]. We present a new approach that utilizes free energy and activity modeling of the equilibrium: Fe + SiO2 + O2 = Fe2SiO4 to calculate absolute fO2 and relative to the iron-wüstite (IW) buffer at <span class="hlt">pressure</span> and temperature [ΔIW (P,T)]. This equilibrium is considered across a wide range of <span class="hlt">pressures</span> and temperatures, including up to the liquidus temperature of peridotite (4,000 K at 50 GPa). Application of ΔIW (ratio) to metal-silicate experiments can be three or four orders of magnitude different from ΔIW (P,T) values calculated using free energy and activity modeling. We will also use this approach to consider the variation in oxygen fugacity in a magma ocean scenario for various thermal structures for the early Earth: hot liquidus <span class="hlt">gradient</span>, 100 °C below the liquidus, hot and cool adiabatic <span class="hlt">gradients</span>, and a cool subsolidus adiabat. The results are used to assess the effect of increasing P and T, changing silicate composition during accretion, and related to current models for accretion and core formation in the Earth. The fO2 in a deep magma ocean scenario may become lower relative to the IW buffer at hotter and deeper conditions, which could include metal entrainment scenarios. Therefore, fO2 may evolve from high to low fO2 during Earth (and other differentiated bodies) accretion. Any modeling of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150023002','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150023002"><span>Implicit Large-Eddy Simulations of Zero-<span class="hlt">Pressure</span> <span class="hlt">Gradient</span>, Turbulent Boundary Layer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sekhar, Susheel; Mansour, Nagi N.</p> <p>2015-01-01</p> <p>A set of direct simulations of zero-<span class="hlt">pressure</span> <span class="hlt">gradient</span>, turbulent boundary layer flows are conducted using various span widths (62-630 wall units), to document their influence on the generated turbulence. The FDL3DI code that solves compressible Navier-Stokes equations using high-order compact-difference scheme and filter, with the standard recycling/rescaling method of turbulence generation, is used. Results are analyzed at two different Re values (500 and 1,400), and compared with spectral DNS data. They show that a minimum span width is required for the mere initiation of numerical turbulence. Narrower domains ((is) less than 100 w.u.) result in relaminarization. Wider spans ((is) greater than 600 w.u.) are required for the turbulent statistics to match reference DNS. The upper-wall boundary condition for this setup spawns marginal deviations in the mean velocity and Reynolds stress profiles, particularly in the buffer region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/20034237-temperature-gradient-effects-vapor-diffusion-partially-saturated-porous-media','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/20034237-temperature-gradient-effects-vapor-diffusion-partially-saturated-porous-media"><span>Temperature <span class="hlt">gradient</span> effects on vapor diffusion in partially-saturated porous media</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Webb, S.W.</p> <p>1999-07-01</p> <p>Vapor diffusion in porous media in the presence of its own liquid may be enhanced due to pore-scale processes, such as condensation and evaporation across isolated liquid islands. Webb and Ho (1997) developed one-and two-dimensional mechanistic pore-scale models of these processes in an <span class="hlt">ideal</span> porous medium. For isothermal and isobaric boundary conditions with a concentration <span class="hlt">gradient</span>, the vapor diffusion rate was significantly enhanced by these liquid island processes compared to a dry porous media. The influence of a temperature <span class="hlt">gradient</span> on the enhanced vapor diffusion rate is considered in this paper. The two-dimensional pore network model which is used inmore » the present study is shown. For partially-saturated conditions, a liquid island is introduced into the top center pore. Boundary conditions on the left and right sides of the model are specified to give the desired concentration and temperature <span class="hlt">gradients</span>. Vapor condenses on one side of the liquid island and evaporates off the other side due to local vapor <span class="hlt">pressure</span> lowering caused by the interface curvature, even without a temperature <span class="hlt">gradient</span>. Rather than acting as an impediment to vapor diffusion, the liquid island actually enhances the vapor diffusion rate. The enhancement of the vapor diffusion rate can be significant depending on the liquid saturation. Vapor diffusion is enhanced by up to 40% for this single liquid island compared to a dry porous medium; enhancement factors of up to an order of magnitude have been calculated for other conditions by Webb and Ho (1997). The dominant effect on the enhancement factor is the concentration <span class="hlt">gradient</span>; the influence of the temperature <span class="hlt">gradient</span> is smaller. The significance of these results, which need to be confirmed by experiments, is that the dominant model of enhanced vapor diffusion (EVD) by Philip and deVries (1957) predicts that temperature <span class="hlt">gradients</span> must exist for EVD to occur. If there is no temperature <span class="hlt">gradient</span>, there is no enhancement. The present</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090042611','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090042611"><span>Optimal Disturbances in Boundary Layers Subject to Streamwise <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tumin, Anatoli; Ashpis, David E.</p> <p>2003-01-01</p> <p>Laminar-turbulent transition in shear flows is still an enigma in the area of fluid mechanics. The conventional explanation of the phenomenon is based on the instability of the shear flow with respect to infinitesimal disturbances. The conventional hydrodynamic stability theory deals with the analysis of normal modes that might be unstable. The latter circumstance is accompanied by an exponential growth of the disturbances that might lead to laminar-turbulent transition. Nevertheless, in many cases, the transition scenario bypasses the exponential growth stage associated with the normal modes. This type of transition is called bypass transition. An understanding of the phenomenon has eluded us to this day. One possibility is that bypass transition is associated with so-called algebraic (non-modal) growth of disturbances in shear flows. In the present work, an analysis of the optimal disturbances/streamwise vortices associated with the transient growth mechanism is performed for boundary layers in the presence of a streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The theory will provide the optimal spacing of the control elements in the spanwise direction and their placement in the streamwise direction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790025267','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790025267"><span>Survey and bibliography on attainment of laminar flow control in air using <span class="hlt">pressure</span> <span class="hlt">gradient</span> and suction, volume 1</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bushnell, D. M.; Tuttle, M. H.</p> <p>1979-01-01</p> <p>A survey was conducted and a bibliography compiled on attainment of laminar flow in air through the use of favorable <span class="hlt">pressure</span> <span class="hlt">gradient</span> and suction. This report contains the survey, summaries of data for both ground and flight experiments, and abstracts of referenced reports. Much early information is also included which may be of some immediate use as background material for LFC applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19097201','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19097201"><span>Turboprop <span class="hlt">IDEAL</span>: a motion-resistant fat-water separation technique.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Huo, Donglai; Li, Zhiqiang; Aboussouan, Eric; Karis, John P; Pipe, James G</p> <p>2009-01-01</p> <p>Suppression of the fat signal in MRI is very important for many clinical applications. Multi-point water-fat separation methods, such as <span class="hlt">IDEAL</span> (Iterative Decomposition of water and fat with Echo Asymmetry and Least-squares estimation), can robustly separate water and fat signal, but inevitably increase scan time, making separated images more easily affected by patient motions. PROPELLER (Periodically Rotated Overlapping ParallEL Lines with Enhanced Reconstruction) and Turboprop techniques offer an effective approach to correct for motion artifacts. By combining these techniques together, we demonstrate that the new TP-<span class="hlt">IDEAL</span> method can provide reliable water-fat separation with robust motion correction. The Turboprop sequence was modified to acquire source images, and motion correction algorithms were adjusted to assure the registration between different echo images. Theoretical calculations were performed to predict the optimal shift and spacing of the <span class="hlt">gradient</span> echoes. Phantom images were acquired, and results were compared with regular FSE-<span class="hlt">IDEAL</span>. Both T1- and T2-weighted images of the human brain were used to demonstrate the effectiveness of motion correction. TP-<span class="hlt">IDEAL</span> images were also acquired for pelvis, knee, and foot, showing great potential of this technique for general clinical applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Gradient+AND+physics&pg=2&id=EJ333486','ERIC'); return false;" href="https://eric.ed.gov/?q=Gradient+AND+physics&pg=2&id=EJ333486"><span>A Note on Diffusive Mass Transport.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Haynes, Henry W., Jr.</p> <p>1986-01-01</p> <p>Current chemical engineering textbooks teach that the driving force for diffusive mass transport in <span class="hlt">ideal</span> solutions is the <span class="hlt">gradient</span> in mole fraction. This is only true for <span class="hlt">ideal</span> solution liquids. Therefore, it is shown that the appropriate driving force for use with <span class="hlt">ideal</span> gases is the <span class="hlt">gradient</span> in partial <span class="hlt">pressure</span>. (JN)</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_9 --> <div id="page_10" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="181"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29439881','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29439881"><span>Prospective assessment of the frequency of low <span class="hlt">gradient</span> severe aortic stenosis with preserved left ventricular ejection fraction: Critical impact of aortic flow misalignment and <span class="hlt">pressure</span> recovery phenomenon.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ringle, Anne; Castel, Anne-Laure; Le Goffic, Caroline; Delelis, François; Binda, Camille; Bohbot, Yohan; Ennezat, Pierre Vladimir; Guerbaai, Raphaëlle A; Levy, Franck; Vincentelli, André; Graux, Pierre; Tribouilloy, Christophe; Maréchaux, Sylvestre</p> <p>2018-02-10</p> <p>The frequency of paradoxical low-<span class="hlt">gradient</span> severe aortic stenosis (AS) varies widely across studies. The impact of misalignment of aortic flow and <span class="hlt">pressure</span> recovery phenomenon on the frequency of low-<span class="hlt">gradient</span> severe AS with preserved left ventricular ejection fraction (LVEF) has not been evaluated in prospective studies. To investigate prospectively the impact of aortic flow misalignment by Doppler and lack of <span class="hlt">pressure</span> recovery phenomenon correction on the frequency of low-<span class="hlt">gradient</span> (LG) severe aortic stenosis (AS) with preserved LVEF. Aortic jet velocities and mean <span class="hlt">pressure</span> <span class="hlt">gradient</span> (MPG) were obtained by interrogating all windows in 68 consecutive patients with normal LVEF and severe AS (aortic valve area [AVA] ≤1cm 2 ) on the basis of the apical imaging window alone (two-dimensional [2D] apical approach). Patients were classified as having LG or high-<span class="hlt">gradient</span> (HG) AS according to MPG <40mmHg or ≥40mmHg, and normal flow (NF) or low flow (LF) according to stroke volume index >35mL/m 2 or ≤35mL/m 2 , on the basis of the 2D apical approach, the multiview approach (multiple windows evaluation) and AVA corrected for <span class="hlt">pressure</span> recovery. The proportion of LG severe AS was 57% using the 2D apical approach alone. After the multiview approach and correction for <span class="hlt">pressure</span> recovery, the proportion of LG severe AS decreased from 57% to 13% (LF-LG severe AS decreased from 23% to 3%; NF-LG severe AS decreased from 34% to 10%). As a result, 25% of patients were reclassified as having HG severe AS (AVA ≤1cm 2 and MPG ≥40mmHg) and 19% as having moderate AS. Hence, 77% of patients initially diagnosed with LG severe AS did not have "true" LG severe AS when the multiview approach and the <span class="hlt">pressure</span> recovery phenomenon correction were used. Aortic flow misevaluation, resulting from lack of use of multiple windows evaluation and <span class="hlt">pressure</span> recovery phenomenon correction, accounts for a large proportion of incorrectly graded AS and considerable overestimation of the frequency of LG</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25932974','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25932974"><span>Body satisfaction, thin-<span class="hlt">ideal</span> internalization, and perceived <span class="hlt">pressure</span> to be thin among Canadian women: The role of acculturation and religiosity.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chaker, Zina; Chang, Felicia M; Hakim-Larson, Julie</p> <p>2015-06-01</p> <p>In an online study, 143 Canadian women of various religious backgrounds completed measures of acculturation, religiosity, body satisfaction, internalization of the thin <span class="hlt">ideal</span>, perceived <span class="hlt">pressure</span> from media, and manner of dress. Heritage acculturation correlated with appearance satisfaction, but not weight satisfaction. After accounting for BMI and social desirability, higher heritage acculturation and lower mainstream acculturation were associated with lower perceived <span class="hlt">pressure</span> from media. Thus, heritage acculturation across religious denominations may serve as a buffer against appearance dissatisfaction and perceived media <span class="hlt">pressure</span>. Manner of dress among the Muslim subgroup and its relation to religiosity and acculturation were also assessed. Muslim women who dressed in greater accordance with Islamic principles reported lower heritage acculturation and greater religiosity. Thus, Muslim women's manner of dress was related to their religiosity and the extent to which they embraced cultural values. These findings are discussed in terms of the possible distinctions between heritage acculturation and religiosity. Copyright © 2015 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3778006','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3778006"><span>Selective <span class="hlt">Pressure</span> along a Latitudinal <span class="hlt">Gradient</span> Affects Subindividual Variation in Plants</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Sobral, Mar; Guitián, José; Guitián, Pablo; Larrinaga, Asier R.</p> <p>2013-01-01</p> <p>Individual plants produce repeated structures such as leaves, flowers or fruits, which, although belonging to the same genotype, are not phenotypically identical. Such subindividual variation reflects the potential of individual genotypes to vary with micro-environmental conditions. Furthermore, variation in organ traits imposes costs to foraging animals such as time, energy and increased predation risk. Therefore, animals that interact with plants may respond to this variation and affect plant fitness. Thus, phenotypic variation within an individual plant could be, in part, an adaptive trait. Here we investigated this idea and we found that subindividual variation of fruit size of Crataegus monogyna, in different populations throughout the latitudinal <span class="hlt">gradient</span> in Europe, was explained at some extent by the selective <span class="hlt">pressures</span> exerted by seed-dispersing birds. These findings support the hypothesis that within-individual variation in plants is an adaptive trait selected by interacting animals which may have important implications for plant evolution. PMID:24069297</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19323864','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19323864"><span>Social class-related <span class="hlt">gradient</span> in the association of skeletal growth with blood <span class="hlt">pressure</span> among adolescent boys in India.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rao, Shobha; Apte, Priti</p> <p>2009-12-01</p> <p>In view of the fact that height differences between socio-economic groups are apparent early in childhood, it is of interest to examine whether skeletal growth is reflective of the social class <span class="hlt">gradient</span> in CVD risk. The present study examined blood <span class="hlt">pressure</span> levels, adiposity and growth of adolescent boys from high and low social classes. In a cross-sectional study, skeletal growth (height and sitting height), adiposity (weight, BMI and body fat) and blood <span class="hlt">pressure</span> levels of the adolescents were measured. Pune, India. Adolescent schoolboys (9-16 years) from high socio-economic (HSE; n 1146) and low socio-economic (LSE; n 932) class. LSE boys were thin, short and undernourished (mean BMI: 15.5 kg/m2 v. 19.3 kg/m2 in HSE boys, P = 0.00). Social <span class="hlt">gradient</span> was revealed in differing health risks. The prevalence of high systolic blood <span class="hlt">pressure</span> (HSBP) was high in HSE class (10.5 % v. 2.7 % in LSE class, P = 0.00) and was associated with adiposity, while the prevalence of high diastolic blood <span class="hlt">pressure</span> (HDBP) was high in LSE class (9.8 % v. 7.0 % in HSE class, P = 0.00) and had only a weak association with adiposity. Despite this, lower ratio of leg length to height was associated with significantly higher respective health risks, i.e. for HDBP in LSE class (OR = 1.99, 95 % CI 1.14, 3.47) and for HSBP in HSE class (OR = 1.69, 95 % CI 1.02, 2.77). As stunting in childhood is a major problem in India and Asia, the leg length to height indicator needs to be validated in different populations to understand CVD risks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3948862','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3948862"><span>Osmosis-Based <span class="hlt">Pressure</span> Generation: Dynamics and Application</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Li, Suyi; Billeh, Yazan N.; Wang, K. W.; Mayer, Michael</p> <p>2014-01-01</p> <p>This paper describes osmotically-driven <span class="hlt">pressure</span> generation in a membrane-bound compartment while taking into account volume expansion, solute dilution, surface area to volume ratio, membrane hydraulic permeability, and changes in osmotic <span class="hlt">gradient</span>, bulk modulus, and degree of membrane fouling. The emphasis lies on the dynamics of <span class="hlt">pressure</span> generation; these dynamics have not previously been described in detail. Experimental results are compared to and supported by numerical simulations, which we make accessible as an open source tool. This approach reveals unintuitive results about the quantitative dependence of the speed of <span class="hlt">pressure</span> generation on the relevant and interdependent parameters that will be encountered in most osmotically-driven <span class="hlt">pressure</span> generators. For instance, restricting the volume expansion of a compartment allows it to generate its first 5 kPa of <span class="hlt">pressure</span> seven times faster than without a restraint. In addition, this dynamics study shows that plants are near-<span class="hlt">ideal</span> osmotic <span class="hlt">pressure</span> generators, as they are composed of many small compartments with large surface area to volume ratios and strong cell wall reinforcements. Finally, we demonstrate two applications of an osmosis-based <span class="hlt">pressure</span> generator: actuation of a soft robot and continuous volume delivery over long periods of time. Both applications do not need an external power source but rather take advantage of the energy released upon watering the <span class="hlt">pressure</span> generators. PMID:24614529</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930091005','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930091005"><span>The Compressible Laminar Boundary Layer with Heat Transfer and Arbitrary <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cohen, Clarence B; Reshotko, Eli</p> <p>1956-01-01</p> <p>An approximate method for the calculation of the compressible laminar boundary layer with heat transfer and arbitrary <span class="hlt">pressure</span> <span class="hlt">gradient</span>, based on Thwaites' correlation concept, is presented. With the definition of dimensionless shear and heat-transfer parameters and an assumed correlation of these parameters in terms of a momentum parameter, a complete system of relations for calculating skin friction and heat transfer results. Knowledge of velocity or temperature profiles is not necessary in using this calculation method. When the method is applied to a convergent-divergent, axially symmetric rocket nozzle, it shows that high rates of heat transfer are obtained at the initial stagnation point and at the throat of the nozzle. Also indicated are negative displacement thicknesses in the convergent portion of the nozzle; these occur because of the high density within the lower portions of the cooled boundary layer. (author)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28404476','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28404476"><span>Body size <span class="hlt">ideals</span> and dissatisfaction in Ghanaian adolescents: role of media, lifestyle and well-being.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Michels, N; Amenyah, S D</p> <p>2017-05-01</p> <p>To inspire effective health promotion campaigns, we tested the relationship of <span class="hlt">ideal</span> body size and body size dissatisfaction with (1) the potential resulting health-influencing factors diet, physical activity and well-being; and (2) with media as a potential influencer of body <span class="hlt">ideals</span>. This is a cross-sectional study in 370 Ghanaian adolescents (aged 11-18 years). Questionnaires included disordered eating (EAT26), diet quality (FFQ), physical activity (IPAQ), well-being (KINDL) and media influence on appearance (SATAQ: <span class="hlt">pressure</span>, internalisation and information). <span class="hlt">Ideal</span> body size and body size dissatisfaction were assessed using the Stunkard figure rating scale. Body mass index (BMI), skinfolds and waist were measured. Linear regressions were adjusted for gender, age and parental education. Also, mediation was tested: 'can perceived media influence play a role in the effects of actual body size on body size dissatisfaction?'. Body size dissatisfaction was associated with lower well-being and more media influence (<span class="hlt">pressure</span> and internalisation) but not with physical activity, diet quality or disordered eating. An underweight body size <span class="hlt">ideal</span> might worsen disordered eating but was not significantly related to the other predictors of interest. Only a partial mediation effect by media <span class="hlt">pressure</span> was found: especially overweight adolescents felt media <span class="hlt">pressure</span>, and this media <span class="hlt">pressure</span> was associated with more body size dissatisfaction. To prevent disordered eating and low well-being, health messages should include strategies that reduce body size dissatisfaction and increase body esteem by not focussing on the thin body <span class="hlt">ideal</span>. Changing body size <span class="hlt">ideals</span> in the media might be an appropriate way since media <span class="hlt">pressure</span> was a mediator in the BMI-dissatisfaction relation. Copyright © 2017 The Royal Society for Public Health. Published by Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27810603','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27810603"><span>Overdrainage after ventriculoperitoneal shunting in a patient with a wide depressed skull bone defect: The effect of atmospheric <span class="hlt">pressure</span> <span class="hlt">gradient</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhou, Lixiang; Yu, Jinlu; Sun, Lichao; Han, Yanwu; Wang, Guangming</p> <p>2016-01-01</p> <p>In patients with traumatic brain injury, an effective approach for managing refractory intracranial hypertension is wide decompressive craniectomy. Postoperative hydrocephalus is a frequent complication requiring cerebrospinal fluid (CSF) diversion. A 50-year-old male who underwent decompressive craniectomy after traumatic brain injury. He developed hydrocephalus postoperatively, and accordingly we placed a ventriculoperitoneal shunt. However, an imbalance between the intra- and extra-cranial atmospheric <span class="hlt">pressures</span> led to overdrainage, and he suffered cognitive disorders and extremity weakness. He remained supine for 5days to avoid the effect of gravity on CSF diversion. After 20days, we performed a cranioplasty using a titanium plate. The postoperative course was uneventful, and the patient achieved satisfactory recovery. The gravitational effect and the atmospheric <span class="hlt">pressure</span> <span class="hlt">gradient</span> effect are two factors associated in the ventriculoperitoneal (VP) shunt treatment of hydrocephalus for the patient who had decompressive craniectomy. These effects can be eliminated by supine bed rest and cranioplasty. We herein emphasize the efficacy of VP shunt, supine bed rest and cranioplasty in treating hydrocephalus patients who have undergone craniectomy. A flexible application of these procedures to change the gravitational effect and the atmospheric <span class="hlt">pressure</span> <span class="hlt">gradient</span> effect should promote a favorable outcome. Copyright © 2016 The Authors. Published by Elsevier Ltd.. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060041530&hterms=torque&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dtorque','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060041530&hterms=torque&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dtorque"><span>A General <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> Formulation for Ocean Models, Part 1: Scheme Design and Diagnostic Analysis, Part II: Energy, Momentum, and Bottom Torque Consistency</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Song, Y. T.</p> <p>1998-01-01</p> <p>A Jacobian formulation of the <span class="hlt">pressure</span> <span class="hlt">gradient</span> force for use in models with topography following coordinates is proposed. It can be used in conjunction with any vertical coordinate system and is easily implemented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3210749','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3210749"><span>Evaluation of Transmitral <span class="hlt">Pressure</span> <span class="hlt">Gradients</span> in the Intraoperative Echocardiographic Diagnosis of Mitral Stenosis after Mitral Valve Repair</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Segal, Scott; Fox, John A.; Eltzschig, Holger K.; Shernan, Stanton K.</p> <p>2011-01-01</p> <p>Objective Acute mitral stenosis (MS) following mitral valve (MV) repair is a rare but severe complication. We hypothesize that intraoperative echocardiography can be utilized to diagnose iatrogenic MS immediately after MV repair. Methods The medical records of 552 consecutive patients undergoing MV repair at a single institution were reviewed. Post-cardiopulmonary bypass peak and mean transmitral <span class="hlt">pressure</span> <span class="hlt">gradients</span> (TMPG), and <span class="hlt">pressure</span> half time (PHT) were obtained from intraoperative transesophageal echocardiographic (TEE) examinations in each patient. Results Nine patients (9/552 = 1.6%) received a reoperation for primary MS, prior to hospital discharge. Interestingly, all of these patients already showed intraoperative post-CPB mean and peak TMPGs that were significantly higher compared to values for those who did not: 10.7±4.8 mmHg vs 2.9±1.6 mmHg; p<0.0001 and 22.9±7.9 mmHg vs 7.6±3.7 mmHg; p<0.0001, respectively. However, PHT varied considerably (87±37 ms; range: 20–439 ms) within the entire population, and only weakly predicted the requirement for reoperation (113±56 vs. 87±37 ms, p = 0.034). Receiver operating characteristic curves showed strong discriminating ability for mean <span class="hlt">gradients</span> (AUC = 0.993) and peak <span class="hlt">gradients</span> (area under the curve, AUC = 0.996), but poor performance for PHT (AUC = 0.640). A value of ≥7 mmHg for mean, and ≥17 mmHg for peak TMPG, best separated patients who required reoperation for MS from those who did not. Conclusions Intraoperative TEE diagnosis of a peak TMPG ≥17 mmHg or mean TMPG ≥7 mmHg immediately following CPB are suggestive of clinically relevant MS after MV repair. PMID:22087230</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24008165','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24008165"><span>Radial mean arterial <span class="hlt">pressure</span> reliably reflects femoral mean arterial <span class="hlt">pressure</span> in uncomplicated pediatric cardiac surgery.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cetin, Secil; Pirat, Arash; Kundakci, Aycan; Camkiran, Aynur; Zeyneloglu, Pinar; Ozkan, Murat; Arslan, Gulnaz</p> <p>2014-02-01</p> <p>To see if radial mean arterial <span class="hlt">pressure</span> reliably reflects femoral mean arterial <span class="hlt">pressure</span> in uncomplicated pediatric cardiac surgery. An ethics committee-approved prospective interventional study. Operating room of a tertiary care hospital. Forty-five children aged 3 months to 4 years who underwent pediatric cardiac surgery with hypothermic cardiopulmonary bypass. Simultaneous femoral and radial arterial <span class="hlt">pressures</span> were recorded at 10-minute intervals intraoperatively. A <span class="hlt">pressure</span> <span class="hlt">gradient</span>>5mmHg was considered to be clinically significant. The patients' mean age was 14±11 months and and mean weight was 8.0±3.0kg. A total of 1,816 simultaneous measurements of arterial <span class="hlt">pressure</span> from the radial and femoral arteries were recorded during the pre-cardiopulmonary bypass, cardiopulmonary bypass, and post-cardiopulmonary bypass periods, including 520 (29%) systolic arterial <span class="hlt">pressures</span>, 520 (29%) diastolic arterial <span class="hlt">pressures</span>, and 776 (43%) mean arterial <span class="hlt">pressures</span>. The paired mean arterial <span class="hlt">pressure</span> measurements across the 3 periods were significantly and strongly correlated, and this was true for systolic arterial <span class="hlt">pressures</span> and diastolic arterial <span class="hlt">pressures</span> as well (r>0.93 and p<0.001 for all). Bland-Altman plots demonstrated good agreement between femoral and radial mean arterial <span class="hlt">pressures</span> during the pre-cardiopulmonary bypass, cardiopulmonary bypass, and post-cardiopulmonary bypass periods. A significant radial-to-femoral <span class="hlt">pressure</span> <span class="hlt">gradient</span> was observed in 150 (8%) of the total 1,816 measurements. These <span class="hlt">gradients</span> occurred most frequently between pairs of systolic arterial <span class="hlt">pressure</span> measurements (n = 113, 22% of all systolic arterial <span class="hlt">pressures</span>), followed by mean arterial <span class="hlt">pressure</span> measurements (n = 28, 4% of all mean arterial <span class="hlt">pressures</span>) and diastolic arterial <span class="hlt">pressures</span> measurements (n = 9, 2% of all diastolic arterial <span class="hlt">pressures</span>). These significant <span class="hlt">gradients</span> were not sustained (ie, were not recorded at 2 or more successive time points). The results suggested that radial mean</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JAP...123c4901W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JAP...123c4901W"><span>Near-field multiple traps of paraxial acoustic vortices with strengthened <span class="hlt">gradient</span> force generated by sector transducer array</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Qingdong; Li, Yuzhi; Ma, Qingyu; Guo, Gepu; Tu, Juan; Zhang, Dong</p> <p>2018-01-01</p> <p>In order to improve the capability of particle trapping close to the source plane, theoretical and experimental studies on near-field multiple traps of paraxial acoustic vortices (AVs) with a strengthened acoustic <span class="hlt">gradient</span> force (AGF) generated by a sector transducer array were conducted. By applying the integration of point source radiation, numerical simulations for the acoustic fields generated by the sector transducer array were conducted and compared with those produced by the circular transducer array. It was proved that strengthened AGFs of near-field multiple AVs with higher peak <span class="hlt">pressures</span> and smaller vortex radii could be produced by the sector transducer array with a small topological charge. The axial distributions of the equivalent potential <span class="hlt">gradient</span> indicated that the AGFs of paraxial AVs in the near field were much higher than those in the far field, and the distances at the near-field vortex antinodes were also proved to be the <span class="hlt">ideal</span> trapping positions with relatively higher AGFs. With the established 8-channel AV generation system, theoretical studies were also verified by the experimental measurements of <span class="hlt">pressure</span> and phase for AVs with various topological charges. The formation of near-field multiple paraxial AVs was verified by the cross-sectional circular <span class="hlt">pressure</span> distributions with perfect phase spirals around central <span class="hlt">pressure</span> nulls, and was also proved by the vortex nodes and antinodes along the center axis. The favorable results demonstrated the feasibility of generating near-field multiple traps of paraxial AVs with strengthened AGF using the sector transducer array, and suggested the potential applications of close-range particle trapping in biomedical engineering.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5152585','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5152585"><span><span class="hlt">Ideal</span> Cardiovascular Health and Incident Cardiovascular Events</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ommerborn, Mark J.; Blackshear, Chad T.; Hickson, DeMarc A.; Griswold, Michael E.; Kwatra, Japneet; Djousse, Luc; Clark, Cheryl R.</p> <p>2016-01-01</p> <p>Introduction The epidemiology of American Heart Association <span class="hlt">ideal</span> cardiovascular health (CVH) metrics has not been fully examined in African Americans. This study examines associations of CVH metrics with incident cardiovascular disease (CVD) in the Jackson Heart Study, a longitudinal cohort study of CVD in African Americans. Methods Jackson Heart Study participants without CVD (N=4,702) were followed prospectively between 2000 and 2011. Incidence rates and Cox proportional hazard ratios estimated risks for incident CVD (myocardial infarction, stroke, cardiac procedures, and CVD mortality) associated with seven CVH metrics by sex. Analyses were performed in 2015. Results Participants were followed for a median 8.3 years; none had <span class="hlt">ideal</span> health on all seven CVH metrics. The prevalence of <span class="hlt">ideal</span> health was low for nutrition, physical activity, BMI, and blood <span class="hlt">pressure</span> metrics. The age-adjusted CVD incidence rate (IR) per 1,000 person years was highest for individuals with the least <span class="hlt">ideal</span> health metrics: zero to one (IR=12.5, 95% CI=9.7, 16.1), two (IR=8.2, 95% CI=6.5, 10.4), three (IR=5.7, 95% CI=4.2, 7.6), and four or more (IR=3.4, 95% CI=2.0, 5.9). Adjusting for covariates, individuals with four or more <span class="hlt">ideal</span> CVH metrics had lower risks of incident CVD compared with those with zero or one <span class="hlt">ideal</span> CVH metric (hazard ratio, 0.29; 95% CI=0.17, 0.52; p<0.001). Conclusions African Americans with more <span class="hlt">ideal</span> CVH metrics have lower risks of incident CVD. Comprehensive preventive behavioral and clinical supports should be intensified to improve CVD risk for African Americans with few <span class="hlt">ideal</span> CVH metrics. PMID:27539974</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19353651','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19353651"><span>Rapid water and lipid imaging with T2 mapping using a radial <span class="hlt">IDEAL</span>-GRASE technique.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Zhiqiang; Graff, Christian; Gmitro, Arthur F; Squire, Scott W; Bilgin, Ali; Outwater, Eric K; Altbach, Maria I</p> <p>2009-06-01</p> <p>Three-point Dixon methods have been investigated as a means to generate water and fat images without the effects of field inhomogeneities. Recently, an iterative algorithm (<span class="hlt">IDEAL</span>, iterative decomposition of water and fat with echo asymmetry and least squares estimation) was combined with a <span class="hlt">gradient</span> and spin-echo acquisition strategy (<span class="hlt">IDEAL</span>-GRASE) to provide a time-efficient method for lipid-water imaging with correction for the effects of field inhomogeneities. The method presented in this work combines <span class="hlt">IDEAL</span>-GRASE with radial data acquisition. Radial data sampling offers robustness to motion over Cartesian trajectories as well as the possibility of generating high-resolution T(2) maps in addition to the water and fat images. The radial <span class="hlt">IDEAL</span>-GRASE technique is demonstrated in phantoms and in vivo for various applications including abdominal, pelvic, and cardiac imaging.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018EJPh...39c5102S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018EJPh...39c5102S"><span>The energy density distribution of an <span class="hlt">ideal</span> gas and Bernoulli’s equations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Santos, Leonardo S. F.</p> <p>2018-05-01</p> <p>This work discusses the energy density distribution in an <span class="hlt">ideal</span> gas and the consequences of Bernoulli’s equation and the corresponding relation for compressible fluids. The aim of this work is to study how Bernoulli’s equation determines the energy flow in a fluid, although Bernoulli’s equation does not describe the energy density itself. The model from molecular dynamic considerations that describes an <span class="hlt">ideal</span> gas at rest with uniform density is modified to explore the gas in motion with non-uniform density and gravitational effects. The difference between the component of the speed of a particle that is parallel to the gas speed and the gas speed itself is called ‘parallel random speed’. The <span class="hlt">pressure</span> from the ‘parallel random speed’ is denominated as parallel <span class="hlt">pressure</span>. The modified model predicts that the energy density is the sum of kinetic and potential gravitational energy densities plus two terms with static and parallel <span class="hlt">pressures</span>. The application of Bernoulli’s equation and the corresponding relation for compressible fluids in the energy density expression has resulted in two new formulations. For incompressible and compressible gas, the energy density expressions are written as a function of stagnation, static and parallel <span class="hlt">pressures</span>, without any dependence on kinetic or gravitational potential energy densities. These expressions of the energy density are the main contributions of this work. When the parallel <span class="hlt">pressure</span> was uniform, the energy density distribution for incompressible approximation and compressible gas did not converge to zero for the limit of null static <span class="hlt">pressure</span>. This result is rather unusual because the temperature tends to zero for null <span class="hlt">pressure</span>. When the gas was considered incompressible and the parallel <span class="hlt">pressure</span> was equal to static <span class="hlt">pressure</span>, the energy density maintained this unusual behaviour with small <span class="hlt">pressures</span>. If the parallel <span class="hlt">pressure</span> was equal to static <span class="hlt">pressure</span>, the energy density converged to zero for the limit of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhPl...24g2110S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhPl...24g2110S"><span><span class="hlt">Ideal</span> relaxation of the Hopf fibration</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smiet, Christopher Berg; Candelaresi, Simon; Bouwmeester, Dirk</p> <p>2017-07-01</p> <p><span class="hlt">Ideal</span> magnetohydrodynamics relaxation is the topology-conserving reconfiguration of a magnetic field into a lower energy state where the net force is zero. This is achieved by modeling the plasma as perfectly conducting viscous fluid. It is an important tool for investigating plasma equilibria and is often used to study the magnetic configurations in fusion devices and astrophysical plasmas. We study the equilibrium reached by a localized magnetic field through the topology conserving relaxation of a magnetic field based on the Hopf fibration in which magnetic field lines are closed circles that are all linked with one another. Magnetic fields with this topology have recently been shown to occur in non-<span class="hlt">ideal</span> numerical simulations. Our results show that any localized field can only attain equilibrium if there is a finite external <span class="hlt">pressure</span>, and that for such a field a Taylor state is unattainable. We find an equilibrium plasma configuration that is characterized by a lowered <span class="hlt">pressure</span> in a toroidal region, with field lines lying on surfaces of constant <span class="hlt">pressure</span>. Therefore, the field is in a Grad-Shafranov equilibrium. Localized helical magnetic fields are found when plasma is ejected from astrophysical bodies and subsequently relaxes against the background plasma, as well as on earth in plasmoids generated by, e.g., a Marshall gun. This work shows under which conditions an equilibrium can be reached and identifies a toroidal depression as the characteristic feature of such a configuration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19740007863','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19740007863"><span>Correlation of heat transfer for the zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> hypersonic laminar boundary layer for several gases</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cook, W. J.</p> <p>1973-01-01</p> <p>A theoretical study of heat transfer for zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> hypersonic laminar boundary layers for various gases with particular application to the flows produced in an expansion tube facility was conducted. A correlation based on results obtained from solutions to the governing equations for five gases was formulated. Particular attention was directed toward the laminar boundary layer shock tube splitter plates in carbon dioxide flows generated by high speed shock waves. Computer analysis of the splitter plate boundary layer flow provided information that is useful in interpreting experimental data obtained in shock tube gas radiation studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..1215286L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..1215286L"><span>Effects Of Bedrock Shape And Hillslope <span class="hlt">Gradient</span> On The Pore-Water <span class="hlt">Pressure</span> Development: Implication For Slope Stability</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lanni, Cristiano; McDonnell, Jeff</p> <p>2010-05-01</p> <p>Shallow Landslides are one of the most important causes of loss of human life and socio-economic damage related to the hydro-geological risk issues. The danger of these phenomena is related to their speed of development, the diffculty of foreseeing their location, and the high density of individual phenomena, whose downhill trajectories have a relevant probability of interfering with urbanized areas. Research activity on precipitation-induced landslides has focused mainly on developing predictive understanding of where and when landslides are likely to occur. Nevertheless, some major aspects that may be related to activation of landslides have been poorly investigated. For instance, landslide susceptibility zones are generally predicted assuming constant thickness of soil over an impervious bedrock layer. Nevertheless, recent studies showed subsurface topography could be a first order control for subsurface water-flow dynamics, because of the effects of its own irregular shape. Tromp-van Meerveld and McDonnell (2006) argued that connectivity of patches of transient saturation were a necessary prerequisite for exceeding the rainfall threshold necessary to drive lateral flow. Connectivity - "how the hillslope architecture controls the filling and spilling of isolated patches of saturation" (Hopp and McDonnell, 2009) - appears to be a possible unifying concept and theoretical platform for moving hillslope and watershed hydrology forward. Connectivity could also have important implications on triggering of shallow landslides, because the particular shape of bedrock may limit the water-flow downhill. Here we present a number of virtual numerical experiments performed to investigate the role of bedrock shape and hillslope <span class="hlt">gradient</span> on pore-water <span class="hlt">pressure</span> development. On this purpose, our test is represented by the subsurface topography of the Panola Experiment Hillslope (PEH). That is because scientific literature on PEH provides substantial documentation about the role</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5377364','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5377364"><span>Controlled droplet transport to target on a high adhesion surface with multi-<span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Deng, Siyan; Shang, Weifeng; Feng, Shile; Zhu, Shiping; Xing, Yan; Li, Dan; Hou, Yongping; Zheng, Yongmei</p> <p>2017-01-01</p> <p>We introduce multi-<span class="hlt">gradients</span> including Laplace <span class="hlt">pressure</span> <span class="hlt">gradient</span>, wettable <span class="hlt">gradient</span> and wettable different <span class="hlt">gradient</span> on a high adhesion surface via special wedge-pattern and improved anodic oxidation method. As a result of the cooperative effect mentioned above, controlled directional motion of a droplet on a high adhesion surface is realized, even when the surface is turned upside down. The droplet motion can be predicted and the movement distances can be controlled by simply adjusting the wedge angle and droplet volume. More interestingly, when Laplace <span class="hlt">pressure</span> <span class="hlt">gradient</span> is introduced on a V-shaped wettable <span class="hlt">gradient</span> surface, two droplets can move toward one another as designed. PMID:28368020</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16134110','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16134110"><span>In vivo social comparison to a thin-<span class="hlt">ideal</span> peer promotes body dissatisfaction: a randomized experiment.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Krones, Pamela G; Stice, Eric; Batres, Carla; Orjada, Kendra</p> <p>2005-09-01</p> <p>Although social comparison with media-portrayed thin-<span class="hlt">ideal</span> images has been found to increase body dissatisfaction and negative affect, research has not yet tested whether social comparison with attractive peers in the real world produces similar effects. We randomly assigned 119 young women to interact either with a confederate who conformed to the thin <span class="hlt">ideal</span> or one who conformed to the average body dimensions of women, within the context of an ostensive dating study. Exposure to the thin-<span class="hlt">ideal</span> confederate resulted in an increase in body dissatisfaction but not negative affect or heart rate. Initial thin-<span class="hlt">ideal</span> internalization, perceived sociocultural <span class="hlt">pressure</span>, self-esteem, and observer-rated attractiveness did not moderate these effects. Results suggest that social comparative <span class="hlt">pressure</span> to be thin fosters body dissatisfaction but may not promote negative affect. 2005 by Wiley Periodicals, Inc.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_10 --> <div id="page_11" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="201"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NIMPA.890...35Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NIMPA.890...35Y"><span>Fluid-flow measurements in low permeability media with high <span class="hlt">pressure</span> <span class="hlt">gradients</span> using neutron imaging: Application to concrete</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yehya, Mohamad; Andò, Edward; Dufour, Frédéric; Tengattini, Alessandro</p> <p>2018-05-01</p> <p>This article focuses on a new experimental apparatus for investigating fluid flow under high <span class="hlt">pressure</span> <span class="hlt">gradients</span> within low-permeability porous media by means of neutron imaging. A titanium Hassler cell which optimises neutron transparency while allowing high <span class="hlt">pressure</span> confinement (up to 50 MPa) and injection is designed for this purpose and presented here. This contribution focuses on the development of the proposed methodology thanks to some preliminary results obtained using a new neutron imaging facility named NeXT on the D50 beamline at the Institute Laue Langevin (Grenoble). The preliminary test was conducted by injecting normal water into concrete sample prepared and saturated with heavy water to take advantage of the isotope sensitivity of neutrons. The front between these two types of water is tracked in space and time with a combination of neutron radiography and tomography.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17279351','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17279351"><span>Nurse plants, tree saplings and grazing <span class="hlt">pressure</span>: changes in facilitation along a biotic environmental <span class="hlt">gradient</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Smit, Christian; Vandenberghe, Charlotte; den Ouden, Jan; Müller-Schärer, Heinz</p> <p>2007-05-01</p> <p>Current conceptual models predict that an increase in stress shifts interactions between plants from competitive to facilitative; hence, facilitation is expected to gain in ecological importance with increasing stress. Little is known about how facilitative interactions between plants change with increasing biotic stress, such as that incurred by consumer <span class="hlt">pressure</span> or herbivory (i.e. disturbance sensu Grime). In grazed ecosystems, the presence of unpalatable plants is reported to protect tree saplings against cattle grazing and enhance tree establishment. In accordance with current conceptual facilitation-stress models, we hypothesised a positive relationship between facilitation and grazing <span class="hlt">pressure</span>. We tested this hypothesis in a field experiment in which tree saplings of four different species (deciduous Fagus sylvatica, Acer pseudoplatanus and coniferous Abies alba, Picea abies) were planted either inside or outside of the canopy of the spiny nurse shrub Rosa rubiginosa in enclosures differing in grazing <span class="hlt">pressure</span> (low and high) and in exclosures. During one grazing season we followed the survival of the different tree saplings and the level of browsing on these; we also estimated browsing damage to the nurse shrubs. Shrub damage was highest at the higher grazing <span class="hlt">pressure</span>. Correspondingly, browsing increased and survival decreased in saplings located inside the canopy of the shrubs at the high grazing <span class="hlt">pressure</span> compared to the low grazing <span class="hlt">pressure</span>. Saplings of both deciduous species showed a higher survival than the evergreens, while sapling browsing did not differ between species. The relative facilitation of sapling browsing and sapling survival - i.e. the difference between saplings inside and outside the shrub canopy - decreased at high grazing <span class="hlt">pressure</span> as the facilitative species became less protective. Interestingly, these findings do not agree with current conceptual facilitation-stress models predicting increasing facilitation with abiotic stress. We used</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008PhDT.......247K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008PhDT.......247K"><span>Separation control in adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> using high-speed microjets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kumar, Vikas</p> <p></p> <p>Inlets to aircraft propulsion systems must supply flow to the compressor with minimal <span class="hlt">pressure</span> loss, flow distortion or unsteadiness. Flow separation in internal flows such as inlets and ducts in aircraft propulsion systems and external flows such as over aircraft wings, is undesirable as it reduces the overall system performance. The objective of present study is to understand the nature of separation and more importantly, to explore the applicability of high-speed microjets to actively control this flow separation. The geometry used for this experimental study was a generic backward facing "Stratford Ramp" equipped with arrays of high-speed microjets. The incoming flow was examined over a freestream velocity range of 10-65m/s and at ramp angle in range of 0-10°. It was observed that the flow separates at 30m/s and beyond for all angle of attack. The magnitude and extent of separation bubble increases with increasing adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> and/or increase in free-stream velocity. The separated flow for all the examined conditions was completely attached using suitable array of high-speed microjets. The most notable fact was that elimination of reverse velocity regions was accompanied by a reduction in flow unsteadiness and increased two-dimensionality in the flow. In particular, these gains were achieved with a minimal mass flux, less than 0.2% of the primary flow based on 30% Boundary Layer Ingesting duct. Detailed measurements were obtained to understand the flow control dynamics. The control effectiveness was found to be dependent on the actuation location with respect to separation, jet to cross-flow momentum ratio and the angle at which microjets supply the momentum. It was also determined that the control effect of the microjets, in part, is due to creation of strong stream-wise vortices which enhance the mixing between low-momentum fluid closer to the surface and high-momentum fluid further away from the surface. The penetration depth of microjets was</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.H43I1764I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.H43I1764I"><span>Modeling Study: Mechanism of Foam Propagation in Porous Media at Different Levels of Minimum Mobilization <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Izadi, M.; Kam, S.</p> <p>2017-12-01</p> <p>Scope: Numerous laboratory and field tests revealed that foam can effectively control gas mobility and improve sweep efficiency in enhanced-oil-recovery and subsurface-remediation processes, if correctly designed. The objective of this study is to answer (i) how mechanistic foam model parameters can be determined by fitting lab experiments in a step-by-step manner; (ii) how different levels of mobilization <span class="hlt">pressure</span> <span class="hlt">gradient</span> for foam generation affects the fundamentals of foam propagation; and (iii) how foam propagation distance can be estimated in the subsurface. This study for the first time shows why, and by how much, supercritical CO2 foams are advantaged over other types of foams such as N2 foam. Methods: First of all, by borrowing experimental data existing in the literature, this study shows how to capture mechanistic foam model parameters. The model, then, is applied to a wide range of mobilization <span class="hlt">pressure</span> <span class="hlt">gradient</span> to represent different types of foams that have been applied in the field (Note that supercritical CO2 foams exhibit much lower mobilization <span class="hlt">pressure</span> compared to other types of foams (N2, steam, air, etc.). Finally, the model and parameters are used to evaluate different types of foam injection scenarios in order to predict how far foams can propagate with what properties in the field condition. Results and Conclusions: The results show that (i) the presence of three different foam states (strong, weak, intermediate) as well as two different strong-foam flow regimes (high-quality and low-quality regimes) plays a key role in model fit and field-scale propagation prediction and (ii) the importance of complex non-Newtonian foam rheology should not be underestimated. More specifically, this study finds that (i) supercritical CO2 foams can propagate a few hundreds of feet easily, which is a few orders of magnitude higher than other foams such as N2 foams; (ii) for dry foams (or, strong foams in the high-quality regime), the higher gas fractions the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5583542','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5583542"><span>Estimating <span class="hlt">pressure</span> <span class="hlt">gradients</span> by auscultation: How technology (echocardiography) can help improve clinical skills</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kadle, Rohini L; Phoon, Colin K L</p> <p>2017-01-01</p> <p>AIM To extend our previously-published experience in estimating <span class="hlt">pressure</span> <span class="hlt">gradients</span> (PG) via physical examination in a large patient cohort. METHODS From January 1, 1997 through December 31, 2009, an attending pediatric cardiologist compared clinical examination (EXAM) with Doppler-echo (ECHO), in 1193 patients with pulmonic stenosis (PS, including tetralogy of Fallot), aortic stenosis (AS), and ventricular septal defect (VSD). EXAM PG estimates were based primarily on a murmur’s pitch, grade, and length. ECHO peak instantaneous PG was derived from the modified Bernoulli equation. Patients were 0-38.4 years old (median 4.8). RESULTS For all patients, EXAM correlated highly with ECHO: ECHO = 0.99 (EXAM) + 3.2 mmHg; r = +0.89; P < 0.0001. Agreement was excellent (mean difference = -2.9 ± 16.1 mmHg). In 78% of all patients, agreement between EXAM and ECHO was within 15 mmHg and within 5 mmHg in 45%. Clinical estimates of PS PG were more accurate than of AS and VSD. A palpable precordial thrill and increasing loudness of the murmur predicted higher <span class="hlt">gradients</span> (P < 0.0001). Weight did not influence accuracy. A learning curve was evident, such that the most recent quartile of patients showed ECHO = 1.01 (EXAM) + 1.9, r = +0.92, P < 0.0001; during this time, the attending pediatric cardiologist had been > 10 years in practice. CONCLUSION Clinical examination can accurately estimate PG in PS, AS, or VSD. Continual correlation of clinical findings with echocardiography can lead to highly accurate diagnostic skills. PMID:28932358</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25821396','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25821396"><span>Not All <span class="hlt">Ideals</span> are Equal: Intrinsic and Extrinsic <span class="hlt">Ideals</span> in Relationships.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rodriguez, Lindsey M; Hadden, Benjamin W; Knee, C Raymond</p> <p>2015-03-01</p> <p>The <span class="hlt">ideal</span> standards model suggests that greater consistency between <span class="hlt">ideal</span> standards and actual perceptions of one's relationship predicts positive relationship evaluations; however, no research has evaluated whether this differs across types of <span class="hlt">ideals</span>. A self-determination theory perspective was derived to test whether satisfaction of intrinsic <span class="hlt">ideals</span> buffers the importance of extrinsic <span class="hlt">ideals</span>. Participants (N=195) in committed relationships directly and indirectly reported the extent to which their partner met their <span class="hlt">ideal</span> on two dimensions: intrinsic (e.g., warm, intimate) and extrinsic (e.g., attractive, successful). Relationship need fulfillment and relationship quality were also assessed. Hypotheses were largely supported, such that satisfaction of intrinsic <span class="hlt">ideals</span> more strongly predicted relationship functioning, and satisfaction of intrinsic <span class="hlt">ideals</span> buffered the relevance of extrinsic <span class="hlt">ideals</span> for outcomes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4371771','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4371771"><span>Not All <span class="hlt">Ideals</span> are Equal: Intrinsic and Extrinsic <span class="hlt">Ideals</span> in Relationships</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Rodriguez, Lindsey M.; Hadden, Benjamin W.; Knee, C. Raymond</p> <p>2015-01-01</p> <p>The <span class="hlt">ideal</span> standards model suggests that greater consistency between <span class="hlt">ideal</span> standards and actual perceptions of one’s relationship predicts positive relationship evaluations; however, no research has evaluated whether this differs across types of <span class="hlt">ideals</span>. A self-determination theory perspective was derived to test whether satisfaction of intrinsic <span class="hlt">ideals</span> buffers the importance of extrinsic <span class="hlt">ideals</span>. Participants (N=195) in committed relationships directly and indirectly reported the extent to which their partner met their <span class="hlt">ideal</span> on two dimensions: intrinsic (e.g., warm, intimate) and extrinsic (e.g., attractive, successful). Relationship need fulfillment and relationship quality were also assessed. Hypotheses were largely supported, such that satisfaction of intrinsic <span class="hlt">ideals</span> more strongly predicted relationship functioning, and satisfaction of intrinsic <span class="hlt">ideals</span> buffered the relevance of extrinsic <span class="hlt">ideals</span> for outcomes. PMID:25821396</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28292038','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28292038"><span>[Discordance between mitral valve area (MVA) and <span class="hlt">pressure</span> <span class="hlt">gradient</span> in patients with mitral valve stenosis: mean transmitral valve <span class="hlt">gradient</span> is a severity index or a tolerance index of severity of mitralss valve stenosis?</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Najih, Hayat; Arous, Salim; Laarje, Aziza; Baghdadi, Dalila; Benouna, Mohamed Ghali; Azzouzi, Leila; Habbal, Rachida</p> <p>2016-01-01</p> <p> significant correlation. Indeed, among patients in group 1, 96% had HR between 60 and 100 bpm and no patient had decompensated heart failure. In group 2, 54% (13 patients) had a HR> 100 bpm and 7 of them (53%) had left decompensated heart failure. The analysis of systolic pulmonary artery <span class="hlt">pressure</span> conducted in both groups of the study revealed the existence of a statistically significant correlation (R: 0,518 and P: 0,001) between systolic pulmonary artery <span class="hlt">pressure</span> (SPAP) and MTG. Ventricular rhythm regularity and right ventricular function were not correlated with MTG (R: 0,038 and R: - 0,002 respectively). Mean transmitral <span class="hlt">gradient</span> is a good indicator of mitral stenosis tolerance but it imperfectly reflects mitral stenosis severity as this depends on several hemodynamic parameters. True severe mitral stenosis may have mean transmitral <span class="hlt">gradient</span> < 10mmHg, that is why the value of MTG should never be interpreted as single value.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27742745','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27742745"><span>Establishing a <span class="hlt">gradient</span> between partial <span class="hlt">pressure</span> of arterial carbon dioxide and end-tidal carbon dioxide in patients with acute respiratory distress syndrome.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yousuf, Tariq; Brinton, Taylor; Murtaza, Ghulam; Wozniczka, Daniel; Ahmad, Khansa; Iskandar, Joy; Mehta, Raju; Keshmiri, Hesam; Hanif, Tabassum</p> <p>2017-02-01</p> <p>End-tidal carbon dioxide (ETCO 2 ) monitoring is useful in many situations. However, ETCO 2 monitoring is unreliable in patients with acute respiratory distress syndrome (ARDS) due to widespread lung inflammation. In our study, we attempt to establish the <span class="hlt">gradient</span> between the arterial <span class="hlt">pressure</span> of carbon dioxide (PaCO 2 ) and ETCO 2 in patients with ARDS, which we defined as the PaETCO 2 <span class="hlt">gradient</span>. The main objective of the study was to establish a PaETCO 2 <span class="hlt">gradient</span> in each severity of ARDS. We analyzed 35 patients with ARDS and a total of 88 arterial blood gases were included. PaCO 2 , PaO 2 /FiO 2 and ETCO 2 were measured. Patients were stratified into mild, moderate and severe ARDS as classified by the Berlin ARDS criteria. PaCO 2 and ETCO 2 were compared at each severity stratification. The mean PaCO 2 was 50.0, the mean ETCO 2 was 26.6 and the <span class="hlt">gradient</span> among all samples was 23.24 (±12.02). The mean <span class="hlt">gradient</span> for each severity is as follows: mild: 19.3 (±9.9), moderate: 27.9 (±13.2) and severe: 23.9 (±7.8). The difference between the PaETCO 2 <span class="hlt">gradient</span> of the mild to moderate (p=0.001) and mild to severe groups (p=0.01) reached statistical significance. However, the difference between the moderate to severe groups did not reach statistical significance (p=0.48). We found the <span class="hlt">gradient</span> between PaCO 2 and ETCO 2 in patients with ARDS is vast and tends to worsen with increasing severity of ARDS. This indicates that the <span class="hlt">gradient</span> between the 2 may be used as an indicator of increasing severity of ARDS. Copyright © 2016 American Federation for Medical Research.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140016390','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140016390"><span>Direct Numerical Simulation and Theories of Wall Turbulence with a Range of <span class="hlt">Pressure</span> <span class="hlt">Gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Coleman, G. N.; Garbaruk, A.; Spalart, P. R.</p> <p>2014-01-01</p> <p>A new Direct Numerical Simulation (DNS) of Couette-Poiseuille flow at a higher Reynolds number is presented and compared with DNS of other wall-bounded flows. It is analyzed in terms of testing semi-theoretical proposals for universal behavior of the velocity, mixing length, or eddy viscosity in <span class="hlt">pressure</span> <span class="hlt">gradients</span>, and in terms of assessing the accuracy of two turbulence models. These models are used in two modes, the traditional one with only a dependence on the wall-normal coordinate y, and a newer one in which a lateral dependence on z is added. For pure Couette flow and the Couette-Poiseuille case considered here, this z-dependence allows some models to generate steady streamwise vortices, which generally improves the agreement with DNS and experiment. On the other hand, it complicates the comparison between DNS and models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=ideal+AND+gas+AND+law&pg=4&id=EJ088264','ERIC'); return false;" href="https://eric.ed.gov/?q=ideal+AND+gas+AND+law&pg=4&id=EJ088264"><span><span class="hlt">Pressure</span> (Or No Royal Road)</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Bradley, J.</p> <p>1973-01-01</p> <p>Discusses how difficult the various problems of <span class="hlt">pressure</span>, partial <span class="hlt">pressure</span>, gas laws, and vapor <span class="hlt">pressure</span> are for students. Outlines the evolution of the concept of <span class="hlt">pressure</span>, the gas equation for a perfect gas, partial <span class="hlt">pressures</span>, saturated vapor <span class="hlt">pressure</span>, Avogadro's hypothesis, Raoult's law, and the vapor <span class="hlt">pressure</span> of <span class="hlt">ideal</span> solutions. (JR)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3863693','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3863693"><span>Childhood Lifestyle and Clinical Determinants of Adult <span class="hlt">Ideal</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Laitinen, Tomi T.; Pahkala, Katja; Venn, Alison; Woo, Jessica G; Oikonen, Mervi; Dwyer, Terence; Mikkilä, Vera; Hutri-Kähönen, Nina; Smith, Kylie J.; Gall, Seana L.; Morrison, John A.; Viikari, Jorma S.A.; Raitakari, Olli T.; Magnussen, Costan G.; Juonala, Markus</p> <p>2013-01-01</p> <p>Background The American Heart Association recently defined <span class="hlt">ideal</span> cardiovascular health by simultaneous presence of seven health behaviors and factors. The concept is associated with cardiovascular disease incidence, and cardiovascular disease and all-cause mortality. To effectively promote <span class="hlt">ideal</span> cardiovascular health already early in life, childhood factors predicting future <span class="hlt">ideal</span> cardiovascular health should be investigated. Our aim was thus to comprehensively explore childhood determinants of adult <span class="hlt">ideal</span> cardiovascular health in population based cohorts from three continents. Methods The sample comprised a total of 4409 participants aged 3–19 years at baseline from the Cardiovascular Risk in Young Finns Study (YFS; N=1883) from Finland, Childhood Determinants of Adult Health Study (CDAH; N=1803) from Australia and Princeton Follow-up Study (PFS; N=723) from the United States. Participants were re-examined 19–31 years later when aged 30–48 years. Results In multivariable analyses, independent childhood predictors of adult <span class="hlt">ideal</span> cardiovascular health were family socioeconomic status (P<0.01; direct association) and BMI (P<0.001; inverse association) in all cohorts. In addition, blood <span class="hlt">pressure</span> (P=0.007), LDL-cholesterol (P<0.001) and parental smoking (P=0.006) in the YFS, and own smoking (P=0.001) in CDAH were inversely associated with future <span class="hlt">ideal</span> cardiovascular health. Conclusions Among several lifestyle and clinical indicators studied, higher family socioeconomic status and non-smoking (parental/own) in childhood independently predict <span class="hlt">ideal</span> cardiovascular health in adulthood. As atherosclerotic cardiovascular diseases are rooted in childhood, our findings suggest that special attention could be paid to children who are from low socioeconomic status families, and who smoke or whose parents smoke, to prevent cardiovascular disease morbidity and mortality. PMID:24075574</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26936573','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26936573"><span><span class="hlt">Idealized</span> digital models for conical reed instruments, with focus on the internal <span class="hlt">pressure</span> waveform.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kergomard, J; Guillemain, P; Silva, F; Karkar, S</p> <p>2016-02-01</p> <p>Two models for the generation of self-oscillations of reed conical woodwinds are presented. The models use the fewest parameters (of either the resonator or the exciter), whose influence can be quickly explored. The formulation extends iterated maps obtained for lossless cylindrical pipes without reed dynamics. It uses spherical wave variables in <span class="hlt">idealized</span> resonators, with one parameter more than for cylinders: the missing length of the cone. The mouthpiece volume equals that of the missing part of the cone, and is implemented as either a cylindrical pipe (first model) or a lumped element (second model). Only the first model adds a length parameter for the mouthpiece and leads to the solving of an implicit equation. For the second model, any shape of nonlinear characteristic can be directly considered. The complex characteristic impedance for spherical waves requires sampling times smaller than a round trip in the resonator. The convergence of the two models is shown when the length of the cylindrical mouthpiece tends to zero. The waveform is in semi-quantitative agreement with experiment. It is concluded that the oscillations of the positive episode of the mouthpiece <span class="hlt">pressure</span> are related to the length of the missing part, not to the reed dynamics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19870002652','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19870002652"><span>Modification of a variational objective analysis model for new equations for <span class="hlt">pressure</span> <span class="hlt">gradient</span> and vertical velocity in the lower troposphere and for spatial resolution and accuracy of satellite data</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Achtemeier, G. L.</p> <p>1986-01-01</p> <p>Since late 1982 NASA has supported research to develop a numerical variational model for the diagnostic assimilation of conventional and space-based meteorological data. In order to analyze the model components, four variational models are defined dividing the problem naturally according to increasing complexity. The first of these variational models (MODEL I), the subject of this report, contains the two nonlinear horizontal momentum equations, the integrated continuity equation, and the hydrostatic equation. This report summarizes the results of research (1) to improve the way the large nonmeteorological parts of the <span class="hlt">pressure</span> <span class="hlt">gradient</span> force are partitioned between the two terms of the <span class="hlt">pressure</span> <span class="hlt">gradient</span> force terms of the horizontal momentum equations, (2) to generalize the integrated continuity equation to account for variable <span class="hlt">pressure</span> thickness over elevated terrain, and (3) to introduce horizontal variation in the precision modulus weights for the observations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29376691','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29376691"><span>Velocity <span class="hlt">Gradient</span> Power Functional for Brownian Dynamics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>de Las Heras, Daniel; Schmidt, Matthias</p> <p>2018-01-12</p> <p>We present an explicit and simple approximation for the superadiabatic excess (over <span class="hlt">ideal</span> gas) free power functional, admitting the study of the nonequilibrium dynamics of overdamped Brownian many-body systems. The functional depends on the local velocity <span class="hlt">gradient</span> and is systematically obtained from treating the microscopic stress distribution as a conjugate field. The resulting superadiabatic forces are beyond dynamical density functional theory and are of a viscous nature. Their high accuracy is demonstrated by comparison to simulation results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvL.120b8001D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvL.120b8001D"><span>Velocity <span class="hlt">Gradient</span> Power Functional for Brownian Dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de las Heras, Daniel; Schmidt, Matthias</p> <p>2018-01-01</p> <p>We present an explicit and simple approximation for the superadiabatic excess (over <span class="hlt">ideal</span> gas) free power functional, admitting the study of the nonequilibrium dynamics of overdamped Brownian many-body systems. The functional depends on the local velocity <span class="hlt">gradient</span> and is systematically obtained from treating the microscopic stress distribution as a conjugate field. The resulting superadiabatic forces are beyond dynamical density functional theory and are of a viscous nature. Their high accuracy is demonstrated by comparison to simulation results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDA24002Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDA24002Z"><span>Uncertainty based <span class="hlt">pressure</span> reconstruction from velocity measurement with generalized least squares</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Jiacheng; Scalo, Carlo; Vlachos, Pavlos</p> <p>2017-11-01</p> <p>A method using generalized least squares reconstruction of instantaneous <span class="hlt">pressure</span> field from velocity measurement and velocity uncertainty is introduced and applied to both planar and volumetric flow data. <span class="hlt">Pressure</span> <span class="hlt">gradients</span> are computed on a staggered grid from flow acceleration. The variance-covariance matrix of the <span class="hlt">pressure</span> <span class="hlt">gradients</span> is evaluated from the velocity uncertainty by approximating the <span class="hlt">pressure</span> <span class="hlt">gradient</span> error to a linear combination of velocity errors. An overdetermined system of linear equations which relates the <span class="hlt">pressure</span> and the computed <span class="hlt">pressure</span> <span class="hlt">gradients</span> is formulated and then solved using generalized least squares with the variance-covariance matrix of the <span class="hlt">pressure</span> <span class="hlt">gradients</span>. By comparing the reconstructed <span class="hlt">pressure</span> field against other methods such as solving the <span class="hlt">pressure</span> Poisson equation, the omni-directional integration, and the ordinary least squares reconstruction, generalized least squares method is found to be more robust to the noise in velocity measurement. The improvement on <span class="hlt">pressure</span> result becomes more remarkable when the velocity measurement becomes less accurate and more heteroscedastic. The uncertainty of the reconstructed <span class="hlt">pressure</span> field is also quantified and compared across the different methods.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20090019715&hterms=trend+reports&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dtrend%2Breports','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20090019715&hterms=trend+reports&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dtrend%2Breports"><span>Relationship between Trends in Land Precipitation and Tropical SST <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chung, Chul Eddy; Ramanathan, V.</p> <p>2007-01-01</p> <p>In this study, we examined global zonal/annual mean precipitation trends. Land precipitation trend from 1951 to 2002 shows widespread drying between 10 S to 20 N but the trend from 1977 to 2002 shows partial recovery. Based on general circulation model sensitivity studies, we suggested that these features are driven largely by the meridional SST <span class="hlt">gradient</span> trend in the tropics. Our <span class="hlt">idealized</span> CCM3 experiments substantiated that land precipitation is more sensitive to meridional SST <span class="hlt">gradient</span> than to an overall tropical warming. Various simulations produced for the IPCC 4th assessment report demonstrate that increasing CO2 increases SST in the entire tropics non-uniformly and increases land precipitation only in certain latitude belts, again pointing to the importance of SST <span class="hlt">gradient</span> change. Temporally varying aerosols in the IPCC simulations alter meridional SST <span class="hlt">gradient</span> and land precipitation substantially. Anthropogenic aerosol direct solar forcing without its effects on SST is shown by the CCM3 to have weak but non-negligible influence on land precipitation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5708728','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5708728"><span>Non-invasive assessment of pulsatile intracranial <span class="hlt">pressure</span> with phase-contrast magnetic resonance imaging</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Lindstrøm, Erika Kristina; Vatnehol, Svein Are Sirirud; Mardal, Kent-André; Emblem, Kyrre Eeg; Eide, Per Kristian</p> <p>2017-01-01</p> <p>Invasive monitoring of pulsatile intracranial <span class="hlt">pressure</span> can accurately predict shunt response in patients with idiopathic normal <span class="hlt">pressure</span> hydrocephalus, but may potentially cause complications such as bleeding and infection. We tested how a proposed surrogate parameter for pulsatile intracranial <span class="hlt">pressure</span>, the phase-contrast magnetic resonance imaging derived pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span>, compared with its invasive counterpart. In 22 patients with suspected idiopathic normal <span class="hlt">pressure</span> hydrocephalus, preceding invasive intracranial <span class="hlt">pressure</span> monitoring, and any surgical shunt procedure, we calculated the pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> from phase-contrast magnetic resonance imaging derived cerebrospinal fluid flow velocities obtained at the upper cervical spinal canal using a simplified Navier-Stokes equation. Repeated measurements of the pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> were also undertaken in four healthy controls. Of 17 shunted patients, 16 responded, indicating high proportion of “true” normal <span class="hlt">pressure</span> hydrocephalus in the patient cohort. However, there was no correlation between the magnetic resonance imaging derived pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> and pulsatile intracranial <span class="hlt">pressure</span> (R = -.18, P = .43). Pulse <span class="hlt">pressure</span> <span class="hlt">gradients</span> were also similar in patients and healthy controls (P = .26), and did not differ between individuals with pulsatile intracranial <span class="hlt">pressure</span> above or below established thresholds for shunt treatment (P = .97). Assessment of pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> at level C2 was therefore not found feasible to replace invasive monitoring of pulsatile intracranial <span class="hlt">pressure</span> in selection of patients with idiopathic normal <span class="hlt">pressure</span> hydrocephalus for surgical shunting. Unlike invasive, overnight monitoring, the pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> from magnetic resonance imaging comprises short-term <span class="hlt">pressure</span> fluctuations only. Moreover, complexity of cervical cerebrospinal fluid flow and -pulsatility at the upper cervical spinal canal may render the pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> a poor surrogate marker for</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29190788','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29190788"><span>Non-invasive assessment of pulsatile intracranial <span class="hlt">pressure</span> with phase-contrast magnetic resonance imaging.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ringstad, Geir; Lindstrøm, Erika Kristina; Vatnehol, Svein Are Sirirud; Mardal, Kent-André; Emblem, Kyrre Eeg; Eide, Per Kristian</p> <p>2017-01-01</p> <p>Invasive monitoring of pulsatile intracranial <span class="hlt">pressure</span> can accurately predict shunt response in patients with idiopathic normal <span class="hlt">pressure</span> hydrocephalus, but may potentially cause complications such as bleeding and infection. We tested how a proposed surrogate parameter for pulsatile intracranial <span class="hlt">pressure</span>, the phase-contrast magnetic resonance imaging derived pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span>, compared with its invasive counterpart. In 22 patients with suspected idiopathic normal <span class="hlt">pressure</span> hydrocephalus, preceding invasive intracranial <span class="hlt">pressure</span> monitoring, and any surgical shunt procedure, we calculated the pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> from phase-contrast magnetic resonance imaging derived cerebrospinal fluid flow velocities obtained at the upper cervical spinal canal using a simplified Navier-Stokes equation. Repeated measurements of the pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> were also undertaken in four healthy controls. Of 17 shunted patients, 16 responded, indicating high proportion of "true" normal <span class="hlt">pressure</span> hydrocephalus in the patient cohort. However, there was no correlation between the magnetic resonance imaging derived pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> and pulsatile intracranial <span class="hlt">pressure</span> (R = -.18, P = .43). Pulse <span class="hlt">pressure</span> <span class="hlt">gradients</span> were also similar in patients and healthy controls (P = .26), and did not differ between individuals with pulsatile intracranial <span class="hlt">pressure</span> above or below established thresholds for shunt treatment (P = .97). Assessment of pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> at level C2 was therefore not found feasible to replace invasive monitoring of pulsatile intracranial <span class="hlt">pressure</span> in selection of patients with idiopathic normal <span class="hlt">pressure</span> hydrocephalus for surgical shunting. Unlike invasive, overnight monitoring, the pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> from magnetic resonance imaging comprises short-term <span class="hlt">pressure</span> fluctuations only. Moreover, complexity of cervical cerebrospinal fluid flow and -pulsatility at the upper cervical spinal canal may render the pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> a poor surrogate marker for</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_11 --> <div id="page_12" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="221"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDM16008P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDM16008P"><span>Separation Dynamics of Controlled Internal Flow in an Adverse <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Peterson, C. J.; Vukasinovic, B.; Glezer, A.</p> <p>2017-11-01</p> <p>The effects of fluidic actuation on the dynamic evolution of aggressive internal flow separation is investigated at speeds up to M = 0.4 within a constant-width diffuser branching off of a primary flow duct. It is shown that a spanwise array of fluidic actuators upstream of the separation actively controls the flow constriction (and losses) within the diffuser and consequently the local <span class="hlt">pressure</span> <span class="hlt">gradient</span> at its entrance. The effectiveness of the actuation, as may be measured by the increased flow rate that is diverted through the diffuser, scales with its flow rate coefficient. In the presence of actuation (0.7% mass fraction), the mass flow rate in the primary duct increases by 10% while the fraction of the diverted mass flow rate in the diffuser increases by more than 45%. The flow dynamics near separation in the absence and presence of actuation are characterized using high speed particle image velocimetry and analyzed using proper orthogonal and spectral decompositions. In particular, the spectral contents of the incipient boundary layer separation are compared in the absence and presence of actuation with emphasis on the changes in local dynamics near separation as the characteristic cross stream scale of the boundary layer increases with separation delay.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/979401','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/979401"><span>Quantification of non-<span class="hlt">ideal</span> explosion violence with a shock tube</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Jackson, Scott I; Hill, Larry G</p> <p></p> <p>There is significant interest in quantifying the blast violence associated with various nonideal explosions. Such data is essential to evaluate the damage potential of both explosive cookoff and terrorist explosive scenarios. We present a technique designed to measure the source energy associated with a non-<span class="hlt">ideal</span>, asymmetrical, and three-dimensional explosion. A tube is used to confine and focus energy from a blast event into a one-dimensional, quasi-planar shock front. During propagation along the length of the tube, the wave is allowed to shocksteepen into a more <span class="hlt">ideal</span> form. <span class="hlt">Pressure</span> transducers then measure the shock overpressure as a function of the distancemore » from the source. One-dimensional blast scaling theory allows calculation of the source energy from this data. This small-scale test method addresses cost and noise concerns as well as boosting and symmetry issues associated with large-scale, three-dimensional, blast arena tests. Results from both <span class="hlt">ideal</span> explosives and non-<span class="hlt">ideal</span> explosives are discussed.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ExFl...59...86R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ExFl...59...86R"><span>Unit Reynolds number, Mach number and <span class="hlt">pressure</span> <span class="hlt">gradient</span> effects on laminar-turbulent transition in two-dimensional boundary layers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Risius, Steffen; Costantini, Marco; Koch, Stefan; Hein, Stefan; Klein, Christian</p> <p>2018-05-01</p> <p>The influence of unit Reynolds number (Re_1=17.5× 106-80× 106 {m}^{-1}), Mach number (M= 0.35-0.77) and incompressible shape factor (H_{12} = 2.50-2.66) on laminar-turbulent boundary layer transition was systematically investigated in the Cryogenic Ludwieg-Tube Göttingen (DNW-KRG). For this investigation the existing two-dimensional wind tunnel model, PaLASTra, which offers a quasi-uniform streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span>, was modified to reduce the size of the flow separation region at its trailing edge. The streamwise temperature distribution and the location of laminar-turbulent transition were measured by means of temperature-sensitive paint (TSP) with a higher accuracy than attained in earlier measurements. It was found that for the modified PaLASTra model the transition Reynolds number (Re_{ {tr}}) exhibits a linear dependence on the <span class="hlt">pressure</span> <span class="hlt">gradient</span>, characterized by H_{12}. Due to this linear relation it was possible to quantify the so-called `unit Reynolds number effect', which is an increase of Re_{ {tr}} with Re_1. By a systematic variation of M, Re_1 and H_{12} in combination with a spectral analysis of freestream disturbances, a stabilizing effect of compressibility on boundary layer transition, as predicted by linear stability theory, was detected (`Mach number effect'). Furthermore, two expressions were derived which can be used to calculate the transition Reynolds number as a function of the amplitude of total <span class="hlt">pressure</span> fluctuations, Re_1 and H_{12}. To determine critical N-factors, the measured transition locations were correlated with amplification rates, calculated by incompressible and compressible linear stability theory. By taking into account the spectral level of total <span class="hlt">pressure</span> fluctuations at the frequency of the most amplified Tollmien-Schlichting wave at transition location, the scatter in the determined critical N-factors was reduced. Furthermore, the receptivity coefficients dependence on incidence angle of acoustic waves was used to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17547657','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17547657"><span>Comparison between <span class="hlt">gradient</span>-dependent hydraulic conductivities of roots using the root <span class="hlt">pressure</span> probe: the role of <span class="hlt">pressure</span> propagations and implications for the relative roles of parallel radial pathways.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bramley, Helen; Turner, Neil C; Turner, David W; Tyerman, Stephen D</p> <p>2007-07-01</p> <p>Hydrostatic <span class="hlt">pressure</span> relaxations with the root <span class="hlt">pressure</span> probe are commonly used for measuring the hydraulic conductivity (Lp(r)) of roots. We compared the Lp(r) of roots from species with different root hydraulic properties (Lupinus angustifolius L. 'Merrit', Lupinus luteus L. 'Wodjil', Triticum aestivum L. 'Kulin' and Zea mays L. 'Pacific DK 477') using <span class="hlt">pressure</span> relaxations, a <span class="hlt">pressure</span> clamp and osmotic <span class="hlt">gradients</span> to induce water flow across the root. Only the <span class="hlt">pressure</span> clamp measures water flow under steady-state conditions. Lp(r) determined by <span class="hlt">pressure</span> relaxations was two- to threefold greater than Lp(r) from <span class="hlt">pressure</span> clamps and was independent of the direction of water flow. Lp(r) (<span class="hlt">pressure</span> clamp) was two- to fourfold higher than for Lp(r) (osmotic) for all species except Triticum aestivum where Lp(r) (<span class="hlt">pressure</span> clamp) and Lp(r) (osmotic) were not significantly different. A novel technique was developed to measure the propagation of <span class="hlt">pressure</span> through roots to investigate the cause of the differences in Lp(r). Root segments were connected between two <span class="hlt">pressure</span> probes so that when root <span class="hlt">pressure</span> (P(r)) was manipulated by one probe, the other probe recorded changes in P(r). <span class="hlt">Pressure</span> relaxations did not induce the expected kinetics in <span class="hlt">pressure</span> in the probe at the other end of the root when axial hydraulic conductance, and probe and root capacitances were accounted for. An electric circuit model of the root was constructed that included an additional capacitance in the root loaded by a series of resistances. This accounted for the double exponential kinetics for intact roots in <span class="hlt">pressure</span> relaxation experiments as well as the reduced response observed with the double probe experiments. Although there were potential errors with all the techniques, we considered that the measurement of Lp(r) using the <span class="hlt">pressure</span> clamp was the most unambiguous for small <span class="hlt">pressure</span> changes, and provided that sufficient time was allowed for <span class="hlt">pressure</span> propagation through the root. The differences in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=sexual+AND+development&pg=6&id=EJ810968','ERIC'); return false;" href="https://eric.ed.gov/?q=sexual+AND+development&pg=6&id=EJ810968"><span>Sex Education and <span class="hlt">Ideals</span></span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>de Ruyter, Doret J.; Spiecker, Ben</p> <p>2008-01-01</p> <p>This article argues that sex education should include sexual <span class="hlt">ideals</span>. Sexual <span class="hlt">ideals</span> are divided into sexual <span class="hlt">ideals</span> in the strict sense and sexual <span class="hlt">ideals</span> in the broad sense. It is argued that <span class="hlt">ideals</span> that refer to the context that is deemed to be most <span class="hlt">ideal</span> for the gratification of sexual <span class="hlt">ideals</span> in the strict sense are rightfully called sexual…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ApPhL.108x3503Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ApPhL.108x3503Z"><span>Wavelength-selective ultraviolet (Mg,Zn)O photodiodes: Tuning of parallel composition <span class="hlt">gradients</span> with oxygen <span class="hlt">pressure</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Zhipeng; von Wenckstern, Holger; Lenzner, Jörg; Grundmann, Marius</p> <p>2016-06-01</p> <p>We report on ultraviolet photodiodes with integrated optical filter based on the wurtzite (Mg,Zn)O thin films. Tuning of the bandgap of filter and active layers was realized by employing a continuous composition spread approach relying on the ablation of a single segmented target in pulsed-laser deposition. Filter and active layers of the device were deposited on opposite sides of a sapphire substrate with nearly parallel compositional <span class="hlt">gradients</span>. Ensure that for each sample position the bandgap of the filter layer blocking the high energy radiation is higher than that of the active layer. Different oxygen <span class="hlt">pressures</span> during the two depositions runs. The absorption edge is tuned over 360 meV and the spectral bandwidth of photodiodes is typically 100 meV and as low as 50 meV.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19720022609','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19720022609"><span>The turbulent boundary layer on a porous plate: An experimental study of the fluid mechanics for adverse free stream <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Anderson, P. S.; Kays, W. M.; Moffat, R. J.</p> <p>1972-01-01</p> <p>An experimental investigation of transpired turbulent boundary layers in zero and adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> has been carried out. Profiles of: (1) the mean velocity, (2) the three intensities of the turbulent fluctuations, and (3) the Reynolds stress were obtained by hot-wire anemometry. The friction coefficients were measured by using an integrated form of the boundary layer equation to extrapolate the measured shear stress profiles to the wall.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=combining+AND+chemicals&pg=5&id=EJ358505','ERIC'); return false;" href="https://eric.ed.gov/?q=combining+AND+chemicals&pg=5&id=EJ358505"><span>Textbook Forum. Thermodynamics of "Mixing" of <span class="hlt">Ideal</span> Gases: A Persistent Pitfall.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Meyer, Edwin F.</p> <p>1987-01-01</p> <p>Discusses some of the misconceptions commonly held suggesting that mixing <span class="hlt">ideal</span> gases causes an increase in entropy. Argues that the combining processes and resulting total <span class="hlt">pressure</span> have absolutely nothing to do with the mixing itself. (TW)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29395643','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29395643"><span><span class="hlt">Ideal</span> Cardiovascular Health and Arterial Stiffness in Spanish Adults-The EVIDENT Study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>García-Hermoso, Antonio; Martínez-Vizcaíno, Vicente; Gomez-Marcos, Manuel Ángel; Cavero-Redondo, Iván; Recio-Rodriguez, José Ignacio; García-Ortiz, Luis</p> <p>2018-05-01</p> <p>Studies concerning <span class="hlt">ideal</span> cardiovascular (CV) health and its relationship with arterial stiffness are lacking. This study examined the association between arterial stiffness with <span class="hlt">ideal</span> CV health as defined by the American Heart Association, across age groups and gender. The cross-sectional study included 1365 adults. <span class="hlt">Ideal</span> CV health was defined as meeting <span class="hlt">ideal</span> levels of the following components: 4 behaviors (smoking, body mass index, physical activity, and Mediterranean diet adherence) and 3 factors (total cholesterol, blood <span class="hlt">pressure</span>, and glycated hemoglobin). Patients were grouped into 3 categories according to their number of <span class="hlt">ideal</span> CV health metrics: <span class="hlt">ideal</span> (5-7 metrics), intermediate (3-4 metrics), and poor (0-2 metrics). We analyzed the pulse wave velocity (PWV), the central and radial augmentation indexes, and the ambulatory arterial stiffness index (AASI). The <span class="hlt">ideal</span> CV health profile was inversely associated with lower arterial radial augmentation index and AASI in both genders, particularly in middle-aged (45-65 years) and in elderly subjects (>65 years). Also in elderly subjects, adjusted models showed that adults with at least 3 health metrics at <span class="hlt">ideal</span> levels had significantly lower PWV than those with 2 or fewer <span class="hlt">ideal</span> health metrics. An association was found between a favorable level of <span class="hlt">ideal</span> CV health metrics and lower arterial stiffness across age groups. Copyright © 2018 National Stroke Association. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17180730','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17180730"><span>Mechanistic investigation of drug release from asymmetric membrane tablets: effect of media <span class="hlt">gradients</span> (osmotic <span class="hlt">pressure</span> and concentration), and potential coating failures on in vitro release.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Am Ende, Mary Tanya; Miller, Lee A</p> <p>2007-02-01</p> <p>An asymmetric membrane (AM) tablet was developed for a soluble model compound to study the in vitro drug release mechanisms in challenge conditions, including osmotic <span class="hlt">gradients</span>, concentration <span class="hlt">gradients</span>, and under potential coating failure modes. Porous, semipermable membrane integrity may be compromised by a high fat meal or by the presence of a defect in the coating that could cause a safety concern about dose-dumping. The osmotic and diffusional release mechanisms of the AM tablet were independently shut down such that their individual contribution to the overall drug release was measured. Shut off of osmotic and diffusional release was accomplished by performing dissolution studies into receptor solutions with osmotic <span class="hlt">pressure</span> above the internal core osmotic <span class="hlt">pressure</span> and into receptor solutions saturated with drug, respectively. The effect of coating failure modes on in vitro drug release from the AM tablet was assessed through a simulated high-fat meal and by intentionally compromising the coating integrity. The predominant drug release mechanism for the AM tablet was osmotic and accounted for approximately 90-95% of the total release. Osmotic release was shutoff when the receptor media osmotic <span class="hlt">pressure</span> exceeded 76 atm. Diffusional release of the soluble drug amounted to 5-10% of the total release mechanism. The observed negative in vitro food effect was attributed to the increased osmotic <span class="hlt">pressure</span> from the high fat meal when compared to the predicted release rates in sucrose media with the same osmotic <span class="hlt">pressure</span>. This suppression in drug release rate due to a high fat meal is not anticipated to affect in vivo performance of the dosage form, as the rise in <span class="hlt">pressure</span> is short-lived. Drug release from the AM system studied was determined to be robust to varying and extreme challenge conditions. The conditions investigated included varying pH, agitation rate, media osmotic <span class="hlt">pressure</span>, media saturated with drug to eliminate the concentration <span class="hlt">gradient</span>, simulated high</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950008193','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950008193"><span>A Modified Mixing Length Turbulence Model for Zero and Adverse <span class="hlt">Pressure</span> <span class="hlt">Gradients</span>. M.S. Thesis - Akron Univ., 1993</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Conley, Julianne M.; Leonard, B. P.</p> <p>1994-01-01</p> <p>The modified mixing length (MML) turbulence model was installed in the Proteus Navier-Stokes code, then modified to make it applicable to a wider range of flows typical of aerospace propulsion applications. The modifications are based on experimental data for three flat-plate flows having zero, mild adverse, and strong adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span>. Three transonic diffuser test cases were run with the new version of the model in order to evaluate its performance. All results are compared with experimental data and show improvements over calculations made using the Baldwin-Lomax turbulence model, the standard algebraic model in Proteus.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1188277-millisecond-ordering-block-copolymer-films-via-photo-thermal-gradients','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1188277-millisecond-ordering-block-copolymer-films-via-photo-thermal-gradients"><span>Millisecond ordering of block-copolymer films via photo-thermal <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Majewski, Pawel W.; Yager, Kevin G.</p> <p>2015-03-12</p> <p>For the promise of self-assembly to be realized, processing techniques must be developed that simultaneously enable control of the nanoscale morphology, rapid assembly, and, <span class="hlt">ideally</span>, the ability to pattern the nanostructure. Here, we demonstrate how photo-thermal <span class="hlt">gradients</span> can be used to control the ordering of block-copolymer thin films. Highly localized laser heating leads to intense thermal <span class="hlt">gradients</span>, which induce a thermophoretic force on morphological defects. This increases the ordering kinetics by at least 3 orders-of-magnitude, compared to conventional oven annealing. By simultaneously exploiting the thermal <span class="hlt">gradients</span> to induce shear fields, we demonstrate uniaxial alignment of a block-copolymer film in lessmore » than a second. Finally, we provide examples of how control of the incident light-field can be used to generate prescribed configurations of block-copolymer nanoscale patterns.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29617746','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29617746"><span>Thoracoabdominal <span class="hlt">pressure</span> <span class="hlt">gradient</span> and gastroesophageal reflux: insights from lung transplant candidates.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Masuda, T; Mittal, S K; Kovacs, B; Smith, M; Walia, R; Huang, J; Bremner, R M</p> <p>2018-03-31</p> <p>Advanced lung disease is associated with gastroesophageal reflux disease (GERD). The thoracoabdominal <span class="hlt">pressure</span> <span class="hlt">gradient</span> (TAPG) facilitates gastroesophageal reflux, but the effects of TAPG on gastroesophageal reflux in patients with pulmonary disease have not been well defined. Patients diagnosed with end-stage lung disease are expected to have the most extreme derangement in respiratory mechanics. The aim of this study is to explore the relationship between TAPG and reflux in lung transplant (LTx) candidates. We reviewed LTx recipients who underwent pretransplant esophageal high-resolution manometry and a 24-hour pH study. Patients were excluded if they were undergoing redo LTx, had manometric hiatal hernia, or had previously undergone foregut surgery. TAPG was defined as the intra-abdominal <span class="hlt">pressure</span> minus the intrathoracic <span class="hlt">pressure</span> during inspiration. Adjusted TAPG was calculated by the TAPG minus the resting lower esophageal sphincter (LES) <span class="hlt">pressure</span> (LESP). Twenty-two patients with normal esophageal function tests (i.e., normal esophageal motility with neither manometric hiatal hernia nor pathological reflux on 24-hour pH monitoring) were selected as the pulmonary disease-free control group. In total, 204 patients underwent LTx between January 2015 and December 2016. Of these, 77 patients met inclusion criteria. We compared patients with obstructive lung disease (OLD, n = 33; 42.9%) and those with restrictive lung disease (RLD, n = 42; 54.5%). 2/77 patients (2.6%) had pulmonary arterial hypertension. GERD was more common in the RLD group than in the OLD group (24.2% vs. 47.6%, P = 0.038). TAPG was similar between the OLD group and the controls (14.2 vs. 15.3 mmHg, P = 0.850); however, patients in the RLD group had significantly higher TAPG than the controls (24.4 vs. 15.3 mmHg, P = 0.002). Although TAPG was not correlated with GERD, the adjusted TAPG correlated with reflux in all 77 patients with end-stage lung disease (DeMeester score, rs = 0.256, P</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29851215','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29851215"><span>Dynamic changes of portal vein <span class="hlt">pressure</span> <span class="hlt">gradient</span> under different degrees of liver cirrhosis and resection volume in the first week post hepatectomy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lan, Xiang; Zhang, Hua; Li, Hongyu; Chen, Kefei; Liu, Fei; Wei, Yonggang; Li, Bo</p> <p>2018-05-31</p> <p>We set out to acquire original pathophysiologic data of dynamic changes in portal vein <span class="hlt">pressure</span> <span class="hlt">gradient</span> (PVPG) following liver resection (LR) during post-operation days (POD) 1-7. Portal vein <span class="hlt">pressure</span> <span class="hlt">gradient</span> was measured in 31 patients daily until POD 7 at our liver surgery center. Patients were divided into non-, mild, moderate, and severe cirrhosis groups according to histopathology and were also divided into subgroups according to the volume of hepatectomy. Portal vein <span class="hlt">pressure</span> <span class="hlt">gradient</span> reached its peak on POD 3 in mild cirrhosis (F = 7.525, P < 0.001), moderate cirrhosis (F = 11.200, P < 0.001), and severe cirrhosis groups (F = 26.634, P < 0.001). There were no significant changes in PVPG in the non-cirrhosis group (F = 1.050, P = 0.411). Moreover, PVPG on POD 3 was higher with increasing severity of cirrhosis under the same interval of LR volume (resection volume <200 cm 3 : F = 13.040, P = 0.004; ≥200 cm 3 but <400 cm 3 : F = 13.243, P = 0.004; ≥400 cm 3 : F = 43.685, P < 0.001). Finally, the LR volume had significant impact on PVPG for patients with moderate cirrhosis (F = 6.339, P = 0.033) and severe cirrhosis (t = -7.000, P = 0.020). A similar tendency was also observed when patients were divided according to the ratio of the resected liver volume to total liver volume. The increase in PVPG following LR was positively associated with the degree of cirrhosis, significantly peaking on POD 3. The LR volume only had a significant impact on PVPG for patients with moderate and severe cirrhosis. This represents the first time, to our knowledge, that dynamic changes of PVPG after LR were measured and compared to cirrhosis and resection volume. © 2018 The Japan Society of Hepatology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22986439','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22986439"><span>Normal values for high-resolution anorectal manometry in healthy women: effects of age and significance of rectoanal <span class="hlt">gradient</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Noelting, Jessica; Ratuapli, Shiva K; Bharucha, Adil E; Harvey, Doris M; Ravi, Karthik; Zinsmeister, Alan R</p> <p>2012-10-01</p> <p>High-resolution manometry (HRM) is used to measure anal <span class="hlt">pressures</span> in clinical practice but normal values have not been available. Although rectal evacuation is assessed by the rectoanal <span class="hlt">gradient</span> during simulated evacuation, there is substantial overlap between healthy people and defecatory disorders, and the effects of age are unknown. We evaluated the effects of age on anorectal <span class="hlt">pressures</span> and rectal balloon expulsion in healthy women. Anorectal <span class="hlt">pressures</span> (HRM), rectal sensation, and balloon expulsion time (BET) were evaluated in 62 asymptomatic women ranging in age from 21 to 80 years (median age 44 years) without risk factors for anorectal trauma. In total, 30 women were aged <50 years. Age is associated with lower (r=-0.47, P<0.01) anal resting (63 (5) (≥50 years), 88 (3) (<50 years), mean (s.e.m.)) but not squeeze <span class="hlt">pressures</span>; higher rectal <span class="hlt">pressure</span> and rectoanal <span class="hlt">gradient</span> during simulated evacuation (r=0.3, P<0.05); and a shorter (r=-0.4, P<0.01) rectal BET (17 (9) s (≥50 years) vs. 31 (10) s (<50 years)). Only 5 women had a prolonged (>60 s) rectal BET but 52 had higher anal than rectal <span class="hlt">pressures</span> (i.e., negative <span class="hlt">gradient</span>) during simulated evacuation. The <span class="hlt">gradient</span> was more negative in younger (-41 (6) mm Hg) than older (-12 (6) mm Hg) women and negatively (r=-0.51, P<0.0001) correlated with rectal BET but only explained 16% of the variation in rectal BET. These observations provide normal values for anorectal <span class="hlt">pressures</span> by HRM. Increasing age is associated with lower anal resting <span class="hlt">pressure</span>, a more positive rectoanal <span class="hlt">gradient</span> during simulated evacuation, and a shorter BET in asymptomatic women. Although the rectoanal <span class="hlt">gradient</span> is negatively correlated with rectal BET, this <span class="hlt">gradient</span> is negative even in a majority of asymptomatic women, undermining the utility of a negative <span class="hlt">gradient</span> for diagnosing defecatory disorders by HRM.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16711923','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16711923"><span>Statistics of <span class="hlt">pressure</span> fluctuations in decaying isotropic turbulence.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kalelkar, Chirag</p> <p>2006-04-01</p> <p>We present results from a systematic direct-numerical simulation study of <span class="hlt">pressure</span> fluctuations in an unforced, incompressible, homogeneous, and isotropic three-dimensional turbulent fluid. At cascade completion, isosurfaces of low <span class="hlt">pressure</span> are found to be organized as slender filaments, whereas the predominant isostructures appear sheetlike. We exhibit several results, including plots of probability distributions of the spatial <span class="hlt">pressure</span> difference, the <span class="hlt">pressure-gradient</span> norm, and the eigenvalues of the <span class="hlt">pressure</span>-Hessian tensor. Plots of the temporal evolution of the mean <span class="hlt">pressure-gradient</span> norm, and the mean eigenvalues of the <span class="hlt">pressure</span>-Hessian tensor are also exhibited. We find the statistically preferred orientations between the eigenvectors of the <span class="hlt">pressure</span>-Hessian tensor, the <span class="hlt">pressure</span> <span class="hlt">gradient</span>, the eigenvectors of the strain-rate tensor, the vorticity, and the velocity. Statistical properties of the nonlocal part of the <span class="hlt">pressure</span>-Hessian tensor are also exhibited. We present numerical tests (in the viscous case) of some conjectures of Ohkitani [Phys. Fluids A 5, 2570 (1993)] and Ohkitani and Kishiba [Phys. Fluids 7, 411 (1995)] concerning the <span class="hlt">pressure</span>-Hessian and the strain-rate tensors, for the unforced, incompressible, three-dimensional Euler equations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810002545&hterms=ideal+gas&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dideal%2Bgas','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810002545&hterms=ideal+gas&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dideal%2Bgas"><span>Real-gas effects 1: Simulation of <span class="hlt">ideal</span> gas flow by cryogenic nitrogen and other selected gases</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hall, R. M.</p> <p>1980-01-01</p> <p>The thermodynamic properties of nitrogen gas do not thermodynamically approximate an <span class="hlt">ideal</span>, diatomic gas at cryogenic temperatures. Choice of a suitable equation of state to model its behavior is discussed and the equation of Beattie and Bridgeman is selected as best meeting the needs for cryogenic wind tunnel use. The real gas behavior of nitrogen gas is compared to an <span class="hlt">ideal</span>, diatomic gas for the following flow processes: isentropic expansion; normal shocks; boundary layers; and shock wave boundary layer interactions. The only differences in predicted <span class="hlt">pressure</span> ratio between nitrogen and an <span class="hlt">ideal</span> gas that may limit the minimum operating temperatures of transonic cryogenic wind tunnels seem to occur at total <span class="hlt">pressures</span> approaching 9atmospheres and total temperatures 10 K below the corresponding saturation temperature, where the differences approach 1 percent for both isentropic expansions and normal shocks. Several alternative cryogenic test gases - air, helium, and hydrogen - are also analyzed. Differences in air from an <span class="hlt">ideal</span>, diatomic gas are similar in magnitude to those of nitrogen. Differences for helium and hydrogen are over an order of magnitude greater than those for nitrogen or air. Helium and hydrogen do not approximate the compressible flow of an <span class="hlt">ideal</span>, diatomic gas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3681314','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3681314"><span>Morphogengineering roots: comparing mechanisms of morphogen <span class="hlt">gradient</span> formation</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2012-01-01</p> <p>Background In developmental biology, there has been a recent focus on the robustness of morphogen <span class="hlt">gradients</span> as possible providers of positional information. It was shown that functional morphogen <span class="hlt">gradients</span> present strong biophysical constraints and lack of robustness to noise. Here we explore how the details of the mechanism which underlies the generation of a morphogen <span class="hlt">gradient</span> can influence those properties. Results We contrast three <span class="hlt">gradient</span>-generating mechanisms, (i) a source-decay mechanism; and (ii) a unidirectional transport mechanism; and (iii) a so-called reflux-loop mechanism. Focusing on the dynamics of the phytohormone auxin in the root, we show that only the reflux-loop mechanism can generate a <span class="hlt">gradient</span> that would be adequate to supply functional positional information for the Arabidopsis root, for biophysically reasonable kinetic parameters. Conclusions We argue that traits that differ in spatial and temporal time-scales can impose complex selective <span class="hlt">pressures</span> on the mechanism of morphogen <span class="hlt">gradient</span> formation used for the development of the particular organism. PMID:22583698</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MNRAS.470.2240F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MNRAS.470.2240F"><span>How important is non-<span class="hlt">ideal</span> physics in simulations of sub-Eddington accretion on to spinning black holes?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Foucart, Francois; Chandra, Mani; Gammie, Charles F.; Quataert, Eliot; Tchekhovskoy, Alexander</p> <p>2017-09-01</p> <p>Black holes with accretion rates well below the Eddington rate are expected to be surrounded by low-density, hot, geometrically thick accretion discs. This includes the two black holes being imaged at subhorizon resolution by the Event Horizon Telescope. In these discs, the mean free path for Coulomb interactions between charged particles is large, and the accreting matter is a nearly collisionless plasma. Despite this, numerical simulations have so far modelled these accretion flows using <span class="hlt">ideal</span> magnetohydrodynamics. Here, we present the first global, general relativistic, 3D simulations of accretion flows on to a Kerr black hole including the non-<span class="hlt">ideal</span> effects most likely to affect the dynamics of the disc: the anisotropy between the <span class="hlt">pressure</span> parallel and perpendicular to the magnetic field, and the heat flux along magnetic field lines. We show that for both standard and magnetically arrested discs, the <span class="hlt">pressure</span> anisotropy is comparable to the magnetic <span class="hlt">pressure</span>, while the heat flux remains dynamically unimportant. Despite this large <span class="hlt">pressure</span> anisotropy, however, the time-averaged structure of the accretion flow is strikingly similar to that found in simulations treating the plasma as an <span class="hlt">ideal</span> fluid. We argue that these similarities are largely due to the interchangeability of the viscous and magnetic shear stresses as long as the magnetic <span class="hlt">pressure</span> is small compared to the gas <span class="hlt">pressure</span>, and to the subdominant role of <span class="hlt">pressure</span>/viscous effects in magnetically arrested discs. We conclude by highlighting outstanding questions in modelling the dynamics of low-collisionality accretion flows.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.7110C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.7110C"><span>Tropical deep convection and density current signature on surface <span class="hlt">pressure</span>: comparison of <span class="hlt">idealized</span> and real WRF simulations with infra-sounder measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Costantino, Lorenzo; Heinrich, Philippe</p> <p>2013-04-01</p> <p> wind speed (between 10 and 20 m/s), somewhat proportional to the density change. We note that if the surface density variation is strong and rapid enough, the surface <span class="hlt">pressure</span> filed results strongly affected as well. We observe a surface <span class="hlt">pressure</span> peak (with maximum amplitude of about ±40 Pa), that moves together with the density current leading edge. At cold pool boundaries, the outflow converges with warmer and moister surface inflow and create a curl. As a consequence, warmer air is lifted up and transported above the denser layer where it may trigger new convection and provide the vapor supply to new cloud formation. Results from the 3D real data case (that uses a horizontal resolution of 2 km and a convective cumulus parametrization scheme) show a very good agreement with ground measurements of <span class="hlt">pressure</span>, wind speed and wind direction and confirm that this model configuration reliably reproduces the dynamical and thermodynamical evolution of a tropical deep convective storm. The simulated <span class="hlt">pressure</span> peak (due to a strong density current that originates from a huge precipitating squall line) is very similar to that measured by the infra-sounders (with maximum amplitude of about ±50 Pa) and coherent with the <span class="hlt">idealized</span> case. As in the 2D experiment, the development of tropical heavy rain events associated with strong density currents leads to a sub cloud layer which is not only denser and colder (as a consequence of rain evaporation, that works as a heat sink) but also sensibly dryer in correspondence of the gust front, sing that saturation mixing ration of subsiding air is lower than that of the boundary layer.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_12 --> <div id="page_13" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="241"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014APS..DFDG26007M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014APS..DFDG26007M"><span>Numerical simulation of adverse-<span class="hlt">pressure-gradient</span> boundary layer with or without roughness</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mottaghian, Pouya; Yuan, Junlin; Piomelli, Ugo</p> <p>2014-11-01</p> <p>Large-eddy and direct numerical simulations are carried out on flat-plate boundary layer over smooth and rough surfaces, with adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span>.The deceleration is achieved by imposing a wall-normal freestream velocity profile, and is strong enough to cause separation at the wall. The Reynolds number based on momentum thickness and freestream velocity at inlet is 600. Numerical sandgrain roughness is applied based on an immersed boundary method, yielding a flow that is transitionally rough. The turbulence intensity increases before separation, and reaches a higher value for the rough case, indicating stronger mixing. Roughness also causes higher momentum deficit near the wall, leading to earlier separation. This is consistent with previous observation made on rough-wall flow separation over a ramp. In both cases, the turbulent kinetic energy peaks inside the shear layer above the detachment region, with higher values in the rough case; it then decreases approaching the reattachment region. Near the wall inside the separation bubble, the near-zero turbulent intensity indicates that the turbulent structures are lifted up in the separation region. Compared with the smooth case, the shear layer is farther from the wall and the reattachment length is longer on the rough wall.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=physics+AND+glass&pg=4&id=EJ755354','ERIC'); return false;" href="https://eric.ed.gov/?q=physics+AND+glass&pg=4&id=EJ755354"><span>Experimental Verification of Boyle's Law and the <span class="hlt">Ideal</span> Gas Law</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Ivanov, Dragia Trifonov</p> <p>2007-01-01</p> <p>Two new experiments are offered concerning the experimental verification of Boyle's law and the <span class="hlt">ideal</span> gas law. To carry out the experiments, glass tubes, water, a syringe and a metal manometer are used. The <span class="hlt">pressure</span> of the saturated water vapour is taken into consideration. For educational purposes, the experiments are characterized by their…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860021148','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860021148"><span>Fugacity and concentration <span class="hlt">gradients</span> in a gravity field</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>May, C. E.</p> <p>1986-01-01</p> <p>Equations are reviewed which show that at equilibrium fugacity and concentration <span class="hlt">gradients</span> can exist in gravitational fields. At equilibrium, the logarithm of the ratio of the fugacities of a species at two different locations in a gravitational field is proportional to the difference in the heights of the two locations and the molecular weight of the species. An analogous relation holds for the concentration ratios in a multicomponent system. The ratio is calculated for a variety of examples. The kinetics for the general process are derived, and the time required to approach equilibrium is calculated for several systems. The following special topics are discussed: ionic solutions, polymers, multiphase systems, hydrostatic <span class="hlt">pressure</span>, osmotic <span class="hlt">pressure</span>, and solubility <span class="hlt">gradients</span> in a gravity field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27720242','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27720242"><span>Handgrip Strength and <span class="hlt">Ideal</span> Cardiovascular Health among Colombian Children and Adolescents.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ramírez-Vélez, Robinson; Tordecilla-Sanders, Alejandra; Correa-Bautista, Jorge Enrique; Peterson, Mark D; Garcia-Hermoso, Antonio</p> <p>2016-12-01</p> <p>To evaluate the association between handgrip strength and <span class="hlt">ideal</span> cardiovascular health (CVH) in Colombian children and adolescents. During the 2014-2015 school years, we examined a cross-sectional component of the FUPRECOL (Association for Muscular Strength with Early Manifestation of Cardiovascular Disease Risk Factors among Colombian Children and Adolescents) study. Participants included 1199 (n = 627 boys) youths from Bogota (Colombia). Handgrip strength was measured with a standard adjustable hand held dynamometer and expressed relative to body mass (handgrip/body mass) and as absolute values in kilograms. <span class="hlt">Ideal</span> CVH, as defined by the American Heart Association, was determined as meeting <span class="hlt">ideal</span> levels of the following components: 4 behaviors (smoking status, body mass index, cardiorespiratory fitness, and diet) and 3 factors (total cholesterol, blood <span class="hlt">pressure</span>, and glucose). Higher levels of handgrip strength (both absolute and relative values) were associated with a higher frequency of <span class="hlt">ideal</span> CVH metrics in both sexes (P for trend ≤ .001). Also, higher levels of handgrip strength were associated with a greater number of <span class="hlt">ideal</span> health behaviors (P for trend < .001 in both boys and girls), and with a higher number of <span class="hlt">ideal</span> health factors in boys (P for trend < .001). Finally, levels of handgrip strength were similar between <span class="hlt">ideal</span> versus nonideal glucose or total cholesterol groups in girls. Handgrip strength was strongly associated with <span class="hlt">ideal</span> CVH in Colombian children and adolescents, and thus supports the relevance of early targeted interventions to promote strength adaptation and preservation as part of primordial prevention. Copyright © 2016 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014APS..DFDG27005D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014APS..DFDG27005D"><span><span class="hlt">Pressure</span> measurements in a rapidly sheared turbulent wall layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Diwan, Sourabh; Morrison, Jonathan</p> <p>2014-11-01</p> <p>The aim of the present work is to improve understanding of the role of <span class="hlt">pressure</span> fluctuations in the generation of coherent structures in wall-bounded turbulent flows, with particular regard to the rapid and slow source terms. The work is in part motivated by the recent numerical simulations of Sharma et al. (Phy. Fluids, 23, 2011), which showed the importance of <span class="hlt">pressure</span> fluctuations (and their spatial <span class="hlt">gradients</span>) in the dynamics of large-scale turbulent motions. Our experimental design consists of first generating a shearless boundary layer in a wind tunnel by passing a grid-generated turbulent flow over a moving floor whose speed is matched to the freestream velocity, and then shearing it rapidly by passing it over a stationary floor further downstream. Close to the leading edge of the stationary floor, the resulting flow is expected to satisfy the approximations of the Rapid Distortion Theory and therefore would be an <span class="hlt">ideal</span> candidate for studying linear processes in wall turbulence. We carry out <span class="hlt">pressure</span> measurements on the wall as well as within the flow - the former using surface mounted <span class="hlt">pressure</span> transducers and the latter using a static <span class="hlt">pressure</span> probe similar in design to that used by Tsuji et al. (J. Fluid. Mech. 585, 2007). We also present a comparison between the rapidly sheared flow and a more conventional boundary layer subjected to a turbulent free stream. We acknowledge the financial support from EPSRC (Grant No. EP/I037938).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22946033','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22946033"><span>Implementing quantum logic gates with <span class="hlt">gradient</span> ascent pulse engineering: principles and practicalities.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rowland, Benjamin; Jones, Jonathan A</p> <p>2012-10-13</p> <p>We briefly describe the use of <span class="hlt">gradient</span> ascent pulse engineering (GRAPE) pulses to implement quantum logic gates in nuclear magnetic resonance quantum computers, and discuss a range of simple extensions to the core technique. We then consider a range of difficulties that can arise in practical implementations of GRAPE sequences, reflecting non-<span class="hlt">idealities</span> in the experimental systems used.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADC040572','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADC040572"><span>Dynamic <span class="hlt">Pressure</span> Impulse for Near-<span class="hlt">Ideal</span> and Non-<span class="hlt">Ideal</span> Blast Waves -- Height of Burst Charts</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1981-05-15</p> <p>identI by block numiber) FIELD JGROUP ISUIS4NOUP Nucler Weapons Effects Dynamic <span class="hlt">Pressure</span> Impulse IB 1 3 1Airblast (Nuclear) Height of Burst 1 1 4...impulse versus displacement and vice versa. The power func- tions were used to separately fit the data for the WWII and the M38A1 1/4 ton trucks</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvF...3e3904B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvF...3e3904B"><span>Instability waves and transition in adverse-<span class="hlt">pressure-gradient</span> boundary layers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bose, Rikhi; Zaki, Tamer A.; Durbin, Paul A.</p> <p>2018-05-01</p> <p>Transition to turbulence in incompressible adverse-<span class="hlt">pressure-gradient</span> (APG) boundary layers is investigated by direct numerical simulations. Purely two-dimensional instability waves develop on the inflectional base velocity profile. When the boundary layer is perturbed by isotropic turbulence from the free stream, streamwise elongated streaks form and may interact with the instability waves. Subsequent mechanisms that trigger transition depend on the intensity of the free-stream disturbances. All evidence from the present simulations suggest that the growth rate of instability waves is sufficiently high to couple with the streaks. Under very low levels of free-stream turbulence (˜0.1 % ), transition onset is highly sensitive to the inlet disturbance spectrum and is accelerated if the spectrum contains frequency-wave-number combinations that are commensurate with the instability waves. Transition onset and completion in this regime is characterized by formation and breakdown of Λ vortices, but they are more sporadic than in natural transition. Beneath free-stream turbulence with higher intensity (1-2 % ), bypass transition mechanisms are dominant, but instability waves are still the most dominant disturbances in wall-normal and spanwise perturbation spectra. Most of the breakdowns were by disturbances with critical layers close to the wall, corresponding to inner modes. On the other hand, the propensity of an outer mode to occur increases with the free-stream turbulence level. Higher intensity free-stream disturbances induce strong streaks that favorably distort the boundary layer and suppress the growth of instability waves. But the upward displacement of high amplitude streaks brings them to the outer edge of the boundary layer and exposes them to ambient turbulence. Consequently, high-amplitude streaks exhibit an outer-mode secondary instability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25489050','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25489050"><span>Cardiorespiratory fitness and <span class="hlt">ideal</span> cardiovascular health in European adolescents.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ruiz, Jonatan R; Huybrechts, Inge; Cuenca-García, Magdalena; Artero, Enrique G; Labayen, Idoia; Meirhaeghe, Aline; Vicente-Rodriguez, German; Polito, Angela; Manios, Yannis; González-Gross, Marcela; Marcos, Ascensión; Widhalm, Kurt; Molnar, Denes; Kafatos, Anthony; Sjöström, Michael; Moreno, Luis A; Castillo, Manuel J; Ortega, Francisco B</p> <p>2015-05-15</p> <p>We studied in European adolescents (i) the association between cardiorespiratory fitness and <span class="hlt">ideal</span> cardiovascular health as defined by the American Heart Association and (ii) whether there is a cardiorespiratory fitness threshold associated with a more favourable cardiovascular health profile. Participants included 510 (n=259 girls) adolescents from 9 European countries. The 20 m shuttle run test was used to estimate cardiorespiratory fitness. <span class="hlt">Ideal</span> cardiovascular health was defined as meeting <span class="hlt">ideal</span> levels of the following components: four behaviours (smoking, body mass index, physical activity and diet) and three factors (total cholesterol, blood <span class="hlt">pressure</span> and glucose). Higher levels of cardiorespiratory fitness were associated with a higher number of <span class="hlt">ideal</span> cardiovascular health components in both boys and girls (both p for trend ≤0.001). Levels of cardiorespiratory fitness were significantly higher in adolescents meeting at least four <span class="hlt">ideal</span> components (13% higher in boys, p<0.001; 6% higher in girls, p=0.008). Receiver operating characteristic curve analyses showed a significant discriminating accuracy of cardiorespiratory fitness in identifying the presence of at least four <span class="hlt">ideal</span> cardiovascular health components (43.8 mL/kg/min in boys and 34.6 mL/kg/min in girls, both p<0.001). The results suggest a hypothetical cardiorespiratory fitness level associated with a healthier cardiovascular profile in adolescents. The fitness standards could be used in schools as part of surveillance and/or screening systems to identify youth with poor health behaviours who might benefit from intervention programmes. Published by the BMJ Publishing Group Limited. For permission to use (where not already granted under a licence) please go to http://group.bmj.com/group/rights-licensing/permissions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19840052446&hterms=sonic+temperature&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsonic%2Btemperature','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19840052446&hterms=sonic+temperature&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsonic%2Btemperature"><span>Convective heat transfer studies at high temperatures with <span class="hlt">pressure</span> <span class="hlt">gradient</span> for inlet flow Mach number of 0.45</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pedrosa, A. C. F.; Nagamatsu, H. T.; Hinckel, J. A.</p> <p>1984-01-01</p> <p>Heat transfer measurements were determined for a flat plate with and without <span class="hlt">pressure</span> <span class="hlt">gradient</span> for various free stream temperatures, wall temperature ratios, and Reynolds numbers for an inlet flow Mach number of 0.45, which is a representative inlet Mach number for gas turbine rotor blades. A shock tube generated the high temperature and <span class="hlt">pressure</span> air flow, and a variable geometry test section was used to produce inlet flow Mach number of 0.45 and accelerate the flow over the plate to sonic velocity. Thin-film platinum heat gages recorded the local heat flux for laminar, transition, and turbulent boundary layers. The free stream temperatures varied from 611 R (339 K) to 3840 R (2133 K) for a T(w)/T(r,g) temperature ratio of 0.87 to 0.14. The Reynolds number over the heat gages varied from 3000 to 690,000. The experimental heat transfer data were correlated with laminar and turbulent boundary layer theories for the range of temperatures and Reynolds numbers and the transition phenomenon was examined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25716918','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25716918"><span>Periodic Vesicle Formation in Tectonic Fault Zones--an <span class="hlt">Ideal</span> Scenario for Molecular Evolution.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mayer, Christian; Schreiber, Ulrich; Dávila, María J</p> <p>2015-06-01</p> <p>Tectonic fault systems in the continental crust offer huge networks of interconnected channels and cavities. Filled mainly with water and carbon dioxide (CO2), containing a wide variety of hydrothermal chemistry and numerous catalytic surfaces, they may offer <span class="hlt">ideal</span> reaction conditions for prebiotic chemistry. In these systems, an accumulation zone for organic compounds will develop at a depth of approximately 1 km where CO2 turns sub-critical and dissolved components precipitate. At this point, periodic <span class="hlt">pressure</span> changes caused for example by tidal influences or geyser activity may generate a cyclic process involving repeated phase transitions of carbon dioxide. In the presence of amphiphilic compounds, this will necessarily lead to the transient formation of coated water droplets in the gas phase and corresponding vesicular structures in the aqueous environment. During this process, the concentration of organic components inside the droplets and vesicles would be drastically increased, allowing for favorable reaction conditions and, in case of the vesicles generated, large trans-membrane concentration <span class="hlt">gradients</span>. Altogether, the process of periodic formation and destruction of vesicles could offer a perfect environment for molecular evolution in small compartments and for the generation of protocells. The basic process of vesicle formation is reproduced experimentally with a lipid in a water/CO2 system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26514160','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26514160"><span>Optimal Lifestyle Components in Young Adulthood Are Associated With Maintaining the <span class="hlt">Ideal</span> Cardiovascular Health Profile Into Middle Age.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gooding, Holly C; Shay, Christina M; Ning, Hongyan; Gillman, Matthew W; Chiuve, Stephanie E; Reis, Jared P; Allen, Norrina B; Lloyd-Jones, Donald M</p> <p>2015-10-29</p> <p>Middle-aged adults with <span class="hlt">ideal</span> blood <span class="hlt">pressure</span>, cholesterol, and glucose levels exhibit substantially lower cardiovascular mortality than those with unfavorable levels. Four healthy lifestyle components-optimal body weight, diet, physical activity, and not smoking-are recommended for cardiovascular health (CVH). This study quantified associations between combinations of healthy lifestyle components measured in young adulthood and loss of the <span class="hlt">ideal</span> CVH profile into middle age. Analyses included 2164 young adults in the Coronary Artery Risk Development in Young Adults study with the <span class="hlt">ideal</span> CVH profile (defined as untreated blood <span class="hlt">pressure</span> <120/80 mm Hg, total cholesterol <200 mg/dL, fasting blood glucose <100 mg/dL, and absence of cardiovascular disease) at baseline. Cox proportional hazards regression models estimated hazard ratios for loss of the <span class="hlt">ideal</span> CVH profile over 25 years according to 4 individual and 16 combinations of optimal healthy lifestyle components measured in young adulthood: body mass index, physical activity, nonsmoking status, and diet quality. Models were adjusted for age, sex, race, education, study center, and baseline blood <span class="hlt">pressure</span>, cholesterol, and glucose. Eighty percent (n=1737) of participants lost the <span class="hlt">ideal</span> CVH profile by middle age; loss was greatest for young adults with no optimal healthy lifestyle components at baseline. Relative to young adults with no optimal healthy lifestyle components, those with all 4 were less likely to lose the <span class="hlt">ideal</span> CVH profile (hazard ratio 0.59, 95% CI 0.44-0.80). Combinations that included optimal body mass index and nonsmoking status were each associated with lower risk. Optimal body mass index and not smoking in young adulthood were protective against loss of the <span class="hlt">ideal</span> CVH profile through middle age. Importance of diet and physical activity may be included through their effects on healthy weight. © 2015 The Authors. Published on behalf of the American Heart Association, Inc., by Wiley Blackwell.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21574184','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21574184"><span>Estimation of liver T₂ in transfusion-related iron overload in patients with weighted least squares T₂ <span class="hlt">IDEAL</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Vasanawala, Shreyas S; Yu, Huanzhou; Shimakawa, Ann; Jeng, Michael; Brittain, Jean H</p> <p>2012-01-01</p> <p>MRI imaging of hepatic iron overload can be achieved by estimating T(2) values using multiple-echo sequences. The purpose of this work is to develop and clinically evaluate a weighted least squares algorithm based on T(2) Iterative Decomposition of water and fat with Echo Asymmetry and Least-squares estimation (<span class="hlt">IDEAL</span>) technique for volumetric estimation of hepatic T(2) in the setting of iron overload. The weighted least squares T(2) <span class="hlt">IDEAL</span> technique improves T(2) estimation by automatically decreasing the impact of later, noise-dominated echoes. The technique was evaluated in 37 patients with iron overload. Each patient underwent (i) a standard 2D multiple-echo <span class="hlt">gradient</span> echo sequence for T(2) assessment with nonlinear exponential fitting, and (ii) a 3D T(2) <span class="hlt">IDEAL</span> technique, with and without a weighted least squares fit. Regression and Bland-Altman analysis demonstrated strong correlation between conventional 2D and T(2) <span class="hlt">IDEAL</span> estimation. In cases of severe iron overload, T(2) <span class="hlt">IDEAL</span> without weighted least squares reconstruction resulted in a relative overestimation of T(2) compared with weighted least squares. Copyright © 2011 Wiley-Liss, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27845176','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27845176"><span>Transmural <span class="hlt">gradients</span> of myocardial structure and mechanics: Implications for fiber stress and strain in <span class="hlt">pressure</span> overload.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Carruth, Eric D; McCulloch, Andrew D; Omens, Jeffrey H</p> <p>2016-12-01</p> <p>Although a truly complete understanding of whole heart activation, contraction, and deformation is well beyond our current reach, a significant amount of effort has been devoted to discovering and understanding the mechanisms by which myocardial structure determines cardiac function to better treat patients with cardiac disease. Several experimental studies have shown that transmural fiber strain is relatively uniform in both diastole and systole, in contrast to predictions from traditional mechanical theory. Similarly, mathematical models have largely predicted uniform fiber stress across the wall. The development of this uniform pattern of fiber stress and strain during filling and ejection is due to heterogeneous transmural distributions of several myocardial structures. This review summarizes these transmural <span class="hlt">gradients</span>, their contributions to fiber mechanics, and the potential functional effects of their remodeling during <span class="hlt">pressure</span> overload hypertrophy. Copyright © 2016 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1984GeoRL..11..761H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1984GeoRL..11..761H"><span>Zonal <span class="hlt">pressure</span> <span class="hlt">gradient</span>, velocity and transport in the Atlantic Equatorial Undercurrent from focal cruises (July 1982-February 1984)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hisard, Philippe; Hénin, Christian</p> <p></p> <p>The zonal <span class="hlt">pressure</span> <span class="hlt">gradient</span> (ZPG) along the Atlantic equator and the Equatorial Undercurrent (EUC) transport are discussed for four cruises representative of each season. A very clear sea surface slope reversal occurred in the eastern area during autumn as far west as 14°W. An early onset of the equatorial thermocline rising was evident during spring 1983. An eastward equatorial surface jet clearly distinct from the EUC was observed at 35°W and 29°W. The greatest ZPG but the lowest EUC transport were observed during summer 1983. A nearly total absence of the ZPG and a large surfacing of the EUC as far as 10°W characterized the 1984 winter.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930081504','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930081504"><span>A preliminary investigation of boundary-layer transition along a flat plate with adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Von Doenhoff, Albert E</p> <p>1938-01-01</p> <p>Boundary-layer surveys were made throughout the transition region along a smooth flat plate placed in an airstream of practically zero turbulence and with an adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The boundary-layer Reynolds number at the laminar separation point was varied from 1,800 to 2,600. The test data, when considered in the light of certain theoretical deductions, indicated that transition probably began with separation of the laminar boundary layer. The extent of the transition region, defined as the distance from a calculated laminar separation point to the position of the first fully developed turbulent boundary-layer profile, could be expressed as a constant Reynolds number run of approximately 70,000. Some speculations are presented concerning the application of the foregoing concepts, after certain assumptions have been made, to the problem of the connection between transition on the upper surface of an airfoil at high angles of attack and the maximum lift.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22490117-existence-three-dimensional-ideal-magnetohydrodynamic-equilibria-current-sheets','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22490117-existence-three-dimensional-ideal-magnetohydrodynamic-equilibria-current-sheets"><span>Existence of three-dimensional <span class="hlt">ideal</span>-magnetohydrodynamic equilibria with current sheets</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Loizu, J.; Princeton Plasma Physics Laboratory, PO Box 451, Princeton, New Jersey 08543; Hudson, S. R.</p> <p>2015-09-15</p> <p>We consider the linear and nonlinear <span class="hlt">ideal</span> plasma response to a boundary perturbation in a screw pinch. We demonstrate that three-dimensional, <span class="hlt">ideal</span>-MHD equilibria with continuously nested flux-surfaces and with discontinuous rotational-transform across the resonant rational-surfaces are well defined and can be computed both perturbatively and using fully nonlinear equilibrium calculations. This rescues the possibility of constructing MHD equilibria with current sheets and continuous, smooth <span class="hlt">pressure</span> profiles. The results predict that, even if the plasma acts as a perfectly conducting fluid, a resonant magnetic perturbation can penetrate all the way into the center of a tokamak without being shielded at themore » resonant surface.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19960015572','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19960015572"><span>Effects of Periodic Unsteady Wake Flow and <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> on Boundary Layer Transition Along the Concave Surface of a Curved Plate. Part 3</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schobeiri, M. T.; Radke, R. E.</p> <p>1996-01-01</p> <p>Boundary layer transition and development on a turbomachinery blade is subjected to highly periodic unsteady turbulent flow, <span class="hlt">pressure</span> <span class="hlt">gradient</span> in longitudinal as well as lateral direction, and surface curvature. To study the effects of periodic unsteady wakes on the concave surface of a turbine blade, a curved plate was utilized. On the concave surface of this plate, detailed experimental investigations were carried out under zero and negative <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The measurements were performed in an unsteady flow research facility using a rotating cascade of rods positioned upstream of the curved plate. Boundary layer measurements using a hot-wire probe were analyzed by the ensemble-averaging technique. The results presented in the temporal-spatial domain display the transition and further development of the boundary layer, specifically the ensemble-averaged velocity and turbulence intensity. As the results show, the turbulent patches generated by the wakes have different leading and trailing edge velocities and merge with the boundary layer resulting in a strong deformation and generation of a high turbulence intensity core. After the turbulent patch has totally penetrated into the boundary layer, pronounced becalmed regions were formed behind the turbulent patch and were extended far beyond the point they would occur in the corresponding undisturbed steady boundary layer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018EPJWC.18002037H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018EPJWC.18002037H"><span>Development of Modified Incompressible <span class="hlt">Ideal</span> Gas Model for Natural Draft Cooling Tower Flow Simulation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hyhlík, Tomáš</p> <p>2018-06-01</p> <p>The article deals with the development of incompressible <span class="hlt">ideal</span> gas like model, which can be used as a part of mathematical model describing natural draft wet-cooling tower flow, heat and mass transfer. It is shown, based on the results of a complex mathematical model of natural draft wet-cooling tower flow, that behaviour of <span class="hlt">pressure</span>, temperature and density is very similar to the case of hydrostatics of moist air, where heat and mass transfer in the fill zone must be taken into account. The behaviour inside the cooling tower is documented using density, <span class="hlt">pressure</span> and temperature distributions. The proposed equation for the density is based on the same idea like the incompressible <span class="hlt">ideal</span> gas model, which is only dependent on temperature, specific humidity and in this case on elevation. It is shown that normalized density difference of the density based on proposed model and density based on the nonsimplified model is in the order of 10-4. The classical incompressible <span class="hlt">ideal</span> gas model, Boussinesq model and generalised Boussinesq model are also tested. These models show deviation in percentages.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26841234','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26841234"><span><span class="hlt">Ideals</span> versus reality: Are weight <span class="hlt">ideals</span> associated with weight change in the population?</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kärkkäinen, Ulla; Mustelin, Linda; Raevuori, Anu; Kaprio, Jaakko; Keski-Rahkonen, Anna</p> <p>2016-04-01</p> <p>To quantify weight <span class="hlt">ideals</span> of young adults and to examine whether the discrepancy between actual and <span class="hlt">ideal</span> weight is associated with 10-year body mass index (BMI) change in the population. This study comprised 4,964 adults from the prospective population-based FinnTwin16 study. They reported their actual and <span class="hlt">ideal</span> body weight at age 24 (range 22-27) and 10 years later (attrition 24.6%). The correlates of discrepancy between actual and <span class="hlt">ideal</span> body weight and the impact on subsequent BMI change were examined. The discrepancy between actual and <span class="hlt">ideal</span> weight at 24 years was on average 3.9 kg (1.4 kg/m(2) ) among women and 1.2 kg (0.4 kg/m(2) ) among men. On average, participants gained weight during follow-up irrespective of baseline <span class="hlt">ideal</span> weight: women ¯x = +4.8 kg (1.7 kg/m(2) , 95% CI 1.6-1.9 kg/m(2) ), men ¯x = +6.3 kg (2.0 kg/m(2) , 95% CI 1.8-2.1 kg/m(2) ). Weight <span class="hlt">ideals</span> at 24 years were not correlated with 10-year weight change. At 34 years, just 13.2% of women and 18.9% of men were at or below the weight they had specified as their <span class="hlt">ideal</span> weight at 24 years. Women and men adjusted their <span class="hlt">ideal</span> weight upward over time. Irrespective of <span class="hlt">ideal</span> weight at baseline, weight gain was nearly universal. Weight <span class="hlt">ideals</span> were shifted upward over time. © 2016 The Obesity Society.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_13 --> <div id="page_14" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="261"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17813707','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17813707"><span>Ocean thermal <span class="hlt">gradient</span> hydraulic power plant.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Beck, E J</p> <p>1975-07-25</p> <p>Solar energy stored in the oceans may be used to generate power by exploiting ploiting thermal <span class="hlt">gradients</span>. A proposed open-cycle system uses low-<span class="hlt">pressure</span> steam to elevate vate water, which is then run through a hydraulic turbine to generate power. The device is analogous to an air lift pump.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19960014633','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19960014633"><span>A dynamic response model for <span class="hlt">pressure</span> sensors in continuum and high Knudsen number flows with large temperature <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Whitmore, Stephen A.; Petersen, Brian J.; Scott, David D.</p> <p>1996-01-01</p> <p>This paper develops a dynamic model for <span class="hlt">pressure</span> sensors in continuum and rarefied flows with longitudinal temperature <span class="hlt">gradients</span>. The model was developed from the unsteady Navier-Stokes momentum, energy, and continuity equations and was linearized using small perturbations. The energy equation was decoupled from momentum and continuity assuming a polytropic flow process. Rarefied flow conditions were accounted for using a slip flow boundary condition at the tubing wall. The equations were radially averaged and solved assuming gas properties remain constant along a small tubing element. This fundamental solution was used as a building block for arbitrary geometries where fluid properties may also vary longitudinally in the tube. The problem was solved recursively starting at the transducer and working upstream in the tube. Dynamic frequency response tests were performed for continuum flow conditions in the presence of temperature <span class="hlt">gradients</span>. These tests validated the recursive formulation of the model. Model steady-state behavior was analyzed using the final value theorem. Tests were performed for rarefied flow conditions and compared to the model steady-state response to evaluate the regime of applicability. Model comparisons were excellent for Knudsen numbers up to 0.6. Beyond this point, molecular affects caused model analyses to become inaccurate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1086682','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1086682"><span>System for detecting operating errors in a variable valve timing engine using <span class="hlt">pressure</span> sensors</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Wiles, Matthew A.; Marriot, Craig D</p> <p>2013-07-02</p> <p>A method and control module includes a <span class="hlt">pressure</span> sensor data comparison module that compares measured <span class="hlt">pressure</span> volume signal segments to <span class="hlt">ideal</span> <span class="hlt">pressure</span> volume segments. A valve actuation hardware remedy module performs a hardware remedy in response to comparing the measured <span class="hlt">pressure</span> volume signal segments to the <span class="hlt">ideal</span> <span class="hlt">pressure</span> volume segments when a valve actuation hardware failure is detected.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28209767','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28209767"><span><span class="hlt">Ideal</span> Cardiovascular Health, Cardiovascular Remodeling, and Heart Failure in Blacks: The Jackson Heart Study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Spahillari, Aferdita; Talegawkar, Sameera; Correa, Adolfo; Carr, J Jeffrey; Terry, James G; Lima, João; Freedman, Jane E; Das, Saumya; Kociol, Robb; de Ferranti, Sarah; Mohebali, Donya; Mwasongwe, Stanford; Tucker, Katherine L; Murthy, Venkatesh L; Shah, Ravi V</p> <p>2017-02-01</p> <p>The lifetime risk of heart failure (HF) is higher in the black population than in other racial groups in the United States. We measured the Life's Simple 7 <span class="hlt">ideal</span> cardiovascular health metrics in 4195 blacks in the JHS (Jackson Heart Study; 2000-2004). We evaluated the association of Simple 7 metrics with incident HF and left ventricular structure and function by cardiac magnetic resonance (n=1188). Mean age at baseline was 54.4 years (65% women). Relative to 0 to 2 Simple 7 factors, blacks with 3 factors had 47% lower incident HF risk (hazard ratio [HR], 0.53; 95% confidence interval [CI], 0.39-0.73; P <0.0001); and those with ≥4 factors had 61% lower HF risk (HR, 0.39; 95% CI, 0.24-0.64; P =0.0002). Higher blood <span class="hlt">pressure</span> (HR, 2.32; 95% CI, 1.28-4.20; P =0.005), physical inactivity (HR, 1.65; 95% CI, 1.07-2.55; P =0.02), smoking (HR, 2.04; 95% CI, 1.43-2.91; P <0.0001), and impaired glucose control (HR, 1.76; 95% CI, 1.34-2.29; P <0.0001) were associated with incident HF. The age-/sex-adjusted population attributable risk for these Simple 7 metrics combined was 37.1%. Achievement of <span class="hlt">ideal</span> blood <span class="hlt">pressure</span>, <span class="hlt">ideal</span> body mass index, <span class="hlt">ideal</span> glucose control, and nonsmoking was associated with less likelihood of adverse cardiac remodeling by cardiac magnetic resonance. Cardiovascular risk factors in midlife (specifically elevated blood <span class="hlt">pressure</span>, physical inactivity, smoking, and poor glucose control) are associated with incident HF in blacks and represent targets for intensified HF prevention. © 2017 American Heart Association, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4466498','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4466498"><span>(Fuzzy) <span class="hlt">Ideals</span> of BN-Algebras</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Walendziak, Andrzej</p> <p>2015-01-01</p> <p>The notions of an <span class="hlt">ideal</span> and a fuzzy <span class="hlt">ideal</span> in BN-algebras are introduced. The properties and characterizations of them are investigated. The concepts of normal <span class="hlt">ideals</span> and normal congruences of a BN-algebra are also studied, the properties of them are displayed, and a one-to-one correspondence between them is presented. Conditions for a fuzzy set to be a fuzzy <span class="hlt">ideal</span> are given. The relationships between <span class="hlt">ideals</span> and fuzzy <span class="hlt">ideals</span> of a BN-algebra are established. The homomorphic properties of fuzzy <span class="hlt">ideals</span> of a BN-algebra are provided. Finally, characterizations of Noetherian BN-algebras and Artinian BN-algebras via fuzzy <span class="hlt">ideals</span> are obtained. PMID:26125050</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980211652','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980211652"><span>Cardiovascular <span class="hlt">Pressures</span> with Venous Gas Embolism and Decompression</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Butler, B. D.; Robinson, R.; Sutton, T.; Kemper, G. B.</p> <p>1995-01-01</p> <p>Venous gas embolism (VGE) is reported with decompression to a decreased ambient <span class="hlt">pressure</span>. With severe decompression, or in cases where an intracardiac septal defect (patent foramen ovale) exists, the venous bubbles can become arterialized and cause neurological decompression illness. Incidence rates of patent foramen ovale in the general population range from 25-34% and yet aviators, astronauts, and deepsea divers who have decompression-induced venous bubbles do not demonstrate neurological symptoms at these high rates. This apparent disparity may be attributable to the normal <span class="hlt">pressure</span> <span class="hlt">gradient</span> across the atria of the heart that must be reversed for there to be flow potency. We evaluated the effects of: venous gas embolism (0.025, 0.05 and 0.15 ml/ kg min for 180 min.) hyperbaric decompression; and hypobaric decompression on the <span class="hlt">pressure</span> <span class="hlt">gradient</span> across the left and right atria in anesthetized dogs with intact atrial septa. Left ventricular end-diastolic <span class="hlt">pressure</span> was used as a measure of left atrial <span class="hlt">pressure</span>. In a total of 92 experimental evaluations in 22 dogs, there were no reported reversals in the mean <span class="hlt">pressure</span> <span class="hlt">gradient</span> across the atria; a total of 3 transient reversals occurred during the peak <span class="hlt">pressure</span> <span class="hlt">gradient</span> changes. The reasons that decompression-induced venous bubbles do not consistently cause serious symptoms of decompression illness may be that the amount of venous gas does not always cause sufficient <span class="hlt">pressure</span> reversal across a patent foramen ovale to cause arterialization of the venous bubbles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/923477','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/923477"><span><span class="hlt">Pressure</span> <span class="hlt">gradient</span> passivation of carbonaceous material normally susceptible to spontaneous combustion</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Ochs, Thomas L.; Sands, William D.; Schroeder, Karl; Summers, Cathy A.; Utz, Bruce R.</p> <p>2002-01-29</p> <p>This invention is a process for the passivation or deactivation with respect to oxygen of a carbonaceous material by the exposure of the carbonaceous material to an oxygenated gas in which the oxygenated gas <span class="hlt">pressure</span> is increased from a first <span class="hlt">pressure</span> to a second <span class="hlt">pressure</span> and then the <span class="hlt">pressure</span> is changed to a third <span class="hlt">pressure</span>. Preferably a cyclic process which comprises exposing the carbonaceous material to the gas at low <span class="hlt">pressure</span> and increasing the <span class="hlt">pressure</span> to a second higher <span class="hlt">pressure</span> and then returning the <span class="hlt">pressure</span> to a lower <span class="hlt">pressure</span> is used. The cycle is repeated at least twice wherein the higher <span class="hlt">pressure</span> may be increased after a selected number of cycles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/873370','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/873370"><span><span class="hlt">Pressure</span> <span class="hlt">gradient</span> passivation of carbonaceous material normally susceptible to spontaneous combustion</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Ochs, Thomas L.; Sands, William D.; Schroeder, Karl; Summers, Cathy A.; Utz, Bruce R.</p> <p>2000-11-14</p> <p>This invention is a process for the passivation or deactivation with resp to oxygen of a carbonaceous material by the exposure of the carbonaceous material to an oxygenated gas in which the oxygenated gas <span class="hlt">pressure</span> is increased from a first <span class="hlt">pressure</span> to a second <span class="hlt">pressure</span> and then the <span class="hlt">pressure</span> is changed to a third <span class="hlt">pressure</span>. Preferably a cyclic process which comprises exposing the carbonaceous material to the gas at low <span class="hlt">pressure</span> and increasing the <span class="hlt">pressure</span> to a second higher <span class="hlt">pressure</span> and then returning the <span class="hlt">pressure</span> to a lower <span class="hlt">pressure</span> is used. The cycle is repeated at least twice wherein the higher <span class="hlt">pressure</span> may be increased after a selected number of cycles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3667803','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3667803"><span>Comparison of Coral Reef Ecosystems along a Fishing <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Weijerman, Mariska; Fulton, Elizabeth A.; Parrish, Frank A.</p> <p>2013-01-01</p> <p>Three trophic mass-balance models representing coral reef ecosystems along a fishery <span class="hlt">gradient</span> were compared to evaluate ecosystem effects of fishing. The majority of the biomass estimates came directly from a large-scale visual survey program; therefore, data were collected in the same way for all three models, enhancing comparability. Model outputs–such as net system production, size structure of the community, total throughput, production, consumption, production-to-respiration ratio, and Finn’s cycling index and mean path length–indicate that the systems around the unpopulated French Frigate Shoals and along the relatively lightly populated Kona Coast of Hawai’i Island are mature, stable systems with a high efficiency in recycling of biomass. In contrast, model results show that the reef system around the most populated island in the State of Hawai’i, O’ahu, is in a transitional state with reduced ecosystem resilience and appears to be shifting to an algal-dominated system. Evaluation of the candidate indicators for fishing <span class="hlt">pressure</span> showed that indicators at the community level (e.g., total biomass, community size structure, trophic level of the community) were most robust (i.e., showed the clearest trend) and that multiple indicators are necessary to identify fishing perturbations. These indicators could be used as performance indicators when compared to a baseline for management purposes. This study shows that ecosystem models can be valuable tools in identification of the system state in terms of complexity, stability, and resilience and, therefore, can complement biological metrics currently used by monitoring programs as indicators for coral reef status. Moreover, ecosystem models can improve our understanding of a system’s internal structure that can be used to support management in identification of approaches to reverse unfavorable states. PMID:23737951</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27771587','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27771587"><span>Study on the effects of <span class="hlt">gradient</span> mechanical <span class="hlt">pressures</span> on the proliferation, apoptosis, chondrogenesis and hypertrophy of mandibular condylar chondrocytes in vitro.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Hui; Huang, Linjian; Xie, Qianyang; Cai, Xieyi; Yang, Chi; Wang, Shaoyi; Zhang, Min</p> <p>2017-01-01</p> <p>To investigate the effects of <span class="hlt">gradient</span> mechanical <span class="hlt">pressure</span> on chondrocyte proliferation, apoptosis, and the expression of markers of chondrogenesis and chondrocyte hypertrophy. Mandibular condylar chondrocytes from 5 rabbits were cultured in vitro, and pressed with static <span class="hlt">pressures</span> of 50kPa, 100kPa, 150kPa and 200kPa for 3h, respectively. The chondrocytes cultured without <span class="hlt">pressure</span> (0kPa) were used as control. Cell proliferation, apoptosis, and the expression of aggrecan (AGG), collagen II (COL2), collagen X (COL10), alkaline phosphatase (ALP) were investigated. Ultrastructures of the <span class="hlt">pressurized</span> chondrocytes under transmission electron microscopy (TEM) were observed. Chondrocyte proliferation increased at 100kPa and decreased at 200kPa. Chondrocyte apoptosis increased with peak <span class="hlt">pressure</span> at 200kPa in a dose-dependent manner. Chondrocyte necrosis increased at 200kPa. The expression of AGG increased at 200kPa. The expression of COL2 decreased at 50kPa and increased at 150kPa. The expression of COL10 and ALP increased at 150kPa. Ultrastructure of the <span class="hlt">pressurized</span> chondrocytes under TEM showed: at 100kPa, cells were enlarged with less cellular microvillus and a bigger nucleus; at 200kPa, cells shrank with the sign of apoptosis, and apoptosis cells were found. The mechanical loading of 150kPa is the moderate <span class="hlt">pressure</span> for chondrocyte: cell proliferation and apoptosis is balanced, necrosis is reduced, and chondrogenesis and chondrocyte hypertrophy are promoted. When the <span class="hlt">pressure</span> is lower, chondrogenesis and chondrocyte hypertrophy are inhibited. At 200kPa, degeneration of cartilage is implied. Copyright © 2016 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22599875-ideal-magnetohydrodynamic-theory-localized-interchange-modes-toroidal-anisotropic-plasmas','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22599875-ideal-magnetohydrodynamic-theory-localized-interchange-modes-toroidal-anisotropic-plasmas"><span><span class="hlt">Ideal</span> magnetohydrodynamic theory for localized interchange modes in toroidal anisotropic plasmas</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Shi, Tonghui, E-mail: thshi@ipp.ac.cn; Wan, B. N.; Sun, Y.</p> <p>2016-08-15</p> <p><span class="hlt">Ideal</span> magnetohydrodynamic theory for localized interchange modes is developed for toroidal plasmas with anisotropic <span class="hlt">pressure</span>. The work extends the existing theories of Johnson and Hastie [Phys. Fluids 31, 1609 (1988)], etc., to the low n mode case, where n is the toroidal mode number. Also, the plasma compressibility is included, so that the coupling of the parallel motion to perpendicular one, i.e., the so-called apparent mass effect, is investigated in the anisotropic <span class="hlt">pressure</span> case. The singular layer equation is obtained, and the generalized Mercier's criterion is derived.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26223678','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26223678"><span>Effect of fluid-colloid interactions on the mobility of a thermophoretic microswimmer in non-<span class="hlt">ideal</span> fluids.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fedosov, Dmitry A; Sengupta, Ankush; Gompper, Gerhard</p> <p>2015-09-07</p> <p>Janus colloids propelled by light, e.g., thermophoretic particles, offer promising prospects as artificial microswimmers. However, their swimming behavior and its dependence on fluid properties and fluid-colloid interactions remain poorly understood. Here, we investigate the behavior of a thermophoretic Janus colloid in its own temperature <span class="hlt">gradient</span> using numerical simulations. The dissipative particle dynamics method with energy conservation is used to investigate the behavior in non-<span class="hlt">ideal</span> and <span class="hlt">ideal</span>-gas like fluids for different fluid-colloid interactions, boundary conditions, and temperature-controlling strategies. The fluid-colloid interactions appear to have a strong effect on the colloid behavior, since they directly affect heat exchange between the colloid surface and the fluid. The simulation results show that a reduction of the heat exchange at the fluid-colloid interface leads to an enhancement of colloid's thermophoretic mobility. The colloid behavior is found to be different in non-<span class="hlt">ideal</span> and <span class="hlt">ideal</span> fluids, suggesting that fluid compressibility plays a significant role. The flow field around the colloid surface is found to be dominated by a source-dipole, in agreement with the recent theoretical and simulation predictions. Finally, different temperature-control strategies do not appear to have a strong effect on the colloid's swimming velocity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..SHK.O3003H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..SHK.O3003H"><span>Influence of Flow <span class="hlt">Gradients</span> on Mach Stem Initiation of PBX-9502</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hull, Lawrence; Miller, Phillip; Mas, Eric; Focused Experiments Team</p> <p>2017-06-01</p> <p>Recent experiments and theory explore the effect of flow <span class="hlt">gradients</span> on reaction acceleration and stability in the <span class="hlt">pressure</span>-enhanced region between colliding sub-detonative shock waves in PBX-9502. The experiments are designed to produce divergent curved incident shock waves that interact in a convergent irregular reflection, or ``Mach stem'', configuration. Although this flow is fundamentally unsteady, such a configuration does feature particle paths having a single shock wave that increases the <span class="hlt">pressure</span> from zero to the wave-reflected enhanced <span class="hlt">pressure</span>. Thus, the possibility of pre-shock desensitization is precluded in this interaction region. Diagnostics record arrival wave velocity, shape, and material velocity along the angled free surface face of a large wedge. The wedge is large enough to allow observation of the wave structure for distances much larger than the run-to-detonation derived from classical ``Pop plot'' data. The explosive driver system produces the incident shocks and allows some control of the flow <span class="hlt">gradients</span> in the collision region. Further, the incident shocks are very weak and do not transition to detonation. The experiments discussed feature incident shock waves that would be expected to cause initiation in the Mach stem, based on the Pop plot. Results show that the introduction of <span class="hlt">pressure</span>/velocity <span class="hlt">gradients</span> in the reaction zone strongly influences the ability of the flow to build to a steady ``CJ'' detonation. As expected, the ability of the Mach stem to stabilize or accelerate is strongly influenced by the incident shock <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28468120','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28468120"><span>Trace element concentrations along a <span class="hlt">gradient</span> of urban <span class="hlt">pressure</span> in forest and lawn soils of the Paris region (France).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Foti, Ludovic; Dubs, Florence; Gignoux, Jacques; Lata, Jean-Christophe; Lerch, Thomas Z; Mathieu, Jérôme; Nold, François; Nunan, Naoise; Raynaud, Xavier; Abbadie, Luc; Barot, Sébastien</p> <p>2017-11-15</p> <p>The concentration, degree of contamination and pollution of 7 trace elements (TEs) along an urban <span class="hlt">pressure</span> <span class="hlt">gradient</span> were measured in 180 lawn and wood soils of the Paris region (France). Iron (Fe), a major element, was used as reference element. Copper (Cu), cadmium (Cd), lead (Pb) and zinc (Zn) were of anthropogenic origin, while arsenic (As), chromium (Cr) and nickel (Ni) were of natural origin. Road traffic was identified as the main source of anthropogenic TEs. In addition, the industrial activity of the Paris region, especially cement plants, was identified as secondary source of Cd. Soil characteristics (such as texture, organic carbon (OC) and total nitrogen (tot N) contents) tell the story of the soil origins and legacies along the urban <span class="hlt">pressure</span> <span class="hlt">gradient</span> and often can explain TE concentrations. The history of the land-use types was identified as a factor that allowed understanding the contamination and pollution by TEs. Urban wood soils were found to be more contaminated and polluted than urban lawns, probably because woods are much older than lawns and because of the legacy of the historical management of soils in the Paris region (Haussmann period). Lawn soils are similar to the fertile agricultural soils and relatively recently (mostly from the 1950s onwards) imported from the surrounding of Paris, so that they may be less influenced by urban conditions in terms of TE concentrations. Urban wood soils are heavily polluted by Cd, posing a high risk to the biological communities. The concentration of anthropogenic TEs increased from the rural to the urban areas, and the concentrations of most anthropogenic TEs in urban areas were equivalent to or above the regulatory reference values, raising the question of longer-term monitoring. Copyright © 2017 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23003124','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23003124"><span>Diurnal blood <span class="hlt">pressure</span> variations are associated with changes in distal-proximal skin temperature <span class="hlt">gradient</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kräuchi, Kurt; Gompper, Britta; Hauenstein, Daniela; Flammer, Josef; Pflüger, Marlon; Studerus, Erich; Schötzau, Andy; Orgül, Selim</p> <p>2012-11-01</p> <p>It is generally assumed that skin vascular resistance contributes only to a small extent to total peripheral resistance and hence to blood <span class="hlt">pressure</span> (BP). However, little is known about the impact of skin blood flow (SBF) changes on the diurnal variations of BP under ambulatory conditions. The main aim of the study was to determine whether diurnal patterns of distal SBF are related to mean arterial BP (MAP). Twenty-four-hour ambulatory measurements of BP, heart rate (HR) and distal (mean of hands and feet) as well as proximal (mean of sternum and infraclavicular region) skin temperatures were carried out in 51 patients (men/women = 18/33) during a 2-d eye hospital investigation. The standardized ambulatory protocol allowed measurements with minimal interference from uncontrolled parameters and, hence, some conclusive interpretations. The distal minus proximal skin temperature <span class="hlt">gradient</span> (DPG) provided a measure for distal SBF. Individual cross-correlation analyses revealed that the diurnal pattern of MAP was nearly a mirror image of DPG and hence of distal SBF. Scheduled lunch and dinner induced an increase in DPG and a decline in MAP, while HR increased. Low daytime DPG (i.e. low distal SBF) levels significantly predicted sleep-induced BP dipping (r = -.436, p = .0014). Preliminary path analysis suggested that outdoor air temperature and atmospheric <span class="hlt">pressure</span> may act on MAP via changed distal SBF. Changes in distal SBF may contribute to diurnal variation in MAP, including sleep-induced BP dipping and changes related to food intake. This finding might have an impact on individual cardiovascular risk prediction with respect to diurnal, seasonal and weather variations; however, the underlying mechanisms remain to be discovered.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=ideal+AND+gas&pg=4&id=EJ943202','ERIC'); return false;" href="https://eric.ed.gov/?q=ideal+AND+gas&pg=4&id=EJ943202"><span>The Role of Multiple Representations in the Understanding of <span class="hlt">Ideal</span> Gas Problems</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Madden, Sean P.; Jones, Loretta L.; Rahm, Jrene</p> <p>2011-01-01</p> <p>This study examined the representational competence of students as they solved problems dealing with the temperature-<span class="hlt">pressure</span> relationship for <span class="hlt">ideal</span> gases. Seven students enrolled in a first-semester general chemistry course and two advanced undergraduate science majors participated in the study. The written work and transcripts from videotaped…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70025108','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70025108"><span>Subsurface fluid <span class="hlt">pressures</span> from drill-stem tests, Uinta Basin, Utah</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Nelson, P.H.</p> <p>2002-01-01</p> <p>High fluid <span class="hlt">pressures</span> are known to be associated with oil and gas fields in the Uinta Basin, Utah. Shut-in <span class="hlt">pressure</span> measurements from drill-stem tests show how <span class="hlt">pressure</span> varies with depth and by area within the basin. The data base used in this report incorporates over 2,000 <span class="hlt">pressure</span> measurements from drill-stem tests in wells completed prior to 1985. However, the number of useful <span class="hlt">pressure</span> measurements is considerably less, because many drill-stem tests fail to stabilize at the actual formation <span class="hlt">pressure</span> if the permeability is low. By extracting the maximum <span class="hlt">pressure</span> measurements recorded in a collection of wells within an area, the trend of formation <span class="hlt">pressure</span> within that area can be approximated. Areal compilations of <span class="hlt">pressures</span> from drill-stem tests show that overpressured rock formations occur throughout much of the northern and eastern areas of the Uinta Basin. In particular, significant overpressuring (0.5 < <span class="hlt">pressure</span> <span class="hlt">gradient</span> < 0.8 psi/ft) is found throughout much of the Altamont-Bluebell field at depths ranging from 10,000 to 13,000 ft, equivalent to 5,000 to 8,000 ft below sea level. Limited data indicate that the <span class="hlt">pressure</span> <span class="hlt">gradient</span> declines at depths greater than 13,000 ft. An underpressured zone appears to exist in the Altamont-Bluebell field at depths shallower than 5,000 ft. Throughout the eastern Uinta Basin, moderately overpressured zones (0.46 < <span class="hlt">pressure</span> <span class="hlt">gradient</span> < 0.5 psi/ft) are common, with local evidence of significantly overpressured zones, but <span class="hlt">pressure</span> <span class="hlt">gradients</span> greater than 0.6 psi/ft are rare.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140011550','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140011550"><span><span class="hlt">Gradient</span> Calculation Methods on Arbitrary Polyhedral Unstructured Meshes for Cell-Centered CFD Solvers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sozer, Emre; Brehm, Christoph; Kiris, Cetin C.</p> <p>2014-01-01</p> <p>A survey of <span class="hlt">gradient</span> reconstruction methods for cell-centered data on unstructured meshes is conducted within the scope of accuracy assessment. Formal order of accuracy, as well as error magnitudes for each of the studied methods, are evaluated on a complex mesh of various cell types through consecutive local scaling of an analytical test function. The tests highlighted several <span class="hlt">gradient</span> operator choices that can consistently achieve 1st order accuracy regardless of cell type and shape. The tests further offered error comparisons for given cell types, leading to the observation that the "<span class="hlt">ideal</span>" <span class="hlt">gradient</span> operator choice is not universal. Practical implications of the results are explored via CFD solutions of a 2D inviscid standing vortex, portraying the discretization error properties. A relatively naive, yet largely unexplored, approach of local curvilinear stencil transformation exhibited surprisingly favorable properties</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19810023875','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19810023875"><span>Simulation of <span class="hlt">ideal</span>-gas flow by nitrogen and other selected gases at cryogenic temperatures. [transonic flow in cryogenic wind tunnels</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hall, R. M.; Adcock, J. B.</p> <p>1981-01-01</p> <p>The real gas behavior of nitrogen, the gas normally used in transonic cryogenic tunnels, is reported for the following flow processes: isentropic expansion, normal shocks, boundary layers, and interactions between shock waves and boundary layers. The only difference in predicted <span class="hlt">pressure</span> ratio between nitrogen and an <span class="hlt">ideal</span> gas which may limit the minimum operating temperature of transonic cryogenic wind tunnels occur at total <span class="hlt">pressures</span> approaching 9 atm and total temperatures 10 K below the corresponding saturation temperature. These <span class="hlt">pressure</span> differences approach 1 percent for both isentropic expansions and normal shocks. Alternative cryogenic test gases were also analyzed. Differences between air and an <span class="hlt">ideal</span> diatomic gas are similar in magnitude to those for nitrogen and should present no difficulty. However, differences for helium and hydrogen are over an order of magnitude greater than those for nitrogen or air. It is concluded that helium and cryogenic hydrogen would not approximate the compressible flow of an <span class="hlt">ideal</span> diatomic gas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994JGR....99.2757B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994JGR....99.2757B"><span>Extent of partial melting beneath the Cascade Range, Oregon: Constraints from gravity anomalies and <span class="hlt">ideal</span>-body theory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Blakely, Richard J.</p> <p>1994-02-01</p> <p>The spatial correlation between a horizontal <span class="hlt">gradient</span> in heat flow and a horizontal <span class="hlt">gradient</span> in residual gravity in the Western Cascades of central Oregon has been interpreted by others as evidence of the western edge of a pervasive zone of high temperatures and partial melting at midcrustal depths (5-15 km). Both <span class="hlt">gradients</span> are steep and relatively linear over north-south distances in excess of 150 km. The Western Cascades gravity <span class="hlt">gradient</span> is the western margin of a broad gravity depression over most of the Oregon Cascade Range, implying that the midcrustal zone of anomalous temperatures lies throughout this region. <span class="hlt">Ideal</span>-body theory applied to the gravity <span class="hlt">gradient</span>, however, shows that the source of the Western Cascades gravity <span class="hlt">gradient</span> cannot be deeper than about 2.5 km and is considerably shallower in some locations. These calculations are unique determinations, assuming that density contrasts associated with partial melting and elevated temperatures in the crust do not exceed 500 kg/cu m. Consequently, the gravity <span class="hlt">gradient</span> and the heat flow <span class="hlt">gradient</span> in the Western Cascades cannot be caused directly by the same source if the heat flow <span class="hlt">gradient</span> originates at midcrustal depths. This conclusion in itself does not disprove the existence of a widespread midcrustal zone of anomalously high temperatures and partial melting in this area, but it does eliminate a major argument in support of its existence. The gravity <span class="hlt">gradient</span> is most likely caused by lithologic varitions in the shallow crust, perhaps reflecting a relict boundary between the Cascade extensional trough to the west and Tertiary oceanic crust to the west. The boundary must have formed prior to Oligocene time, the age of the oldest rocks that now conceal it.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_14 --> <div id="page_15" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="281"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28429723','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28429723"><span><span class="hlt">Pressure</span> Self-focusing Effect and Novel Methods for Increasing the Maximum <span class="hlt">Pressure</span> in Traditional and Rotational Diamond Anvil Cells.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Feng, Biao; Levitas, Valery I</p> <p>2017-04-21</p> <p>The main principles of producing a region near the center of a sample, compressed in a diamond anvil cell (DAC), with a very high <span class="hlt">pressure</span> <span class="hlt">gradient</span> and, consequently, with high <span class="hlt">pressure</span> are predicted theoretically. The revealed phenomenon of generating extremely high <span class="hlt">pressure</span> <span class="hlt">gradient</span> is called the <span class="hlt">pressure</span> self-focusing effect. Initial analytical predictions utilized generalization of a simplified equilibrium equation. Then, the results are refined using our recent advanced model for elastoplastic material under high <span class="hlt">pressures</span> in finite element method (FEM) simulations. The main points in producing the <span class="hlt">pressure</span> self-focusing effect are to use beveled anvils and reach a very thin sample thickness at the center. We find that the superposition of torsion in a rotational DAC (RDAC) offers drastic enhancement of the <span class="hlt">pressure</span> self-focusing effect and allows one to reach the same <span class="hlt">pressure</span> under a much lower force and deformation of anvils.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25662064','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25662064"><span>On axial temperature <span class="hlt">gradients</span> due to large <span class="hlt">pressure</span> drops in dense fluid chromatography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Colgate, Sam O; Berger, Terry A</p> <p>2015-03-13</p> <p>The effect of energy degradation (Degradation is the creation of net entropy resulting from irreversibility.) accompanying <span class="hlt">pressure</span> drops across chromatographic columns is examined with regard to explaining axial temperature <span class="hlt">gradients</span> in both high performance liquid chromatography (HPLC) and supercritical fluid chromatography (SFC). The observed effects of warming and cooling can be explained equally well in the language of thermodynamics or fluid dynamics. The necessary equivalence of these treatments is reviewed here to show the legitimacy of using whichever one supports the simpler determination of features of interest. The determination of temperature profiles in columns by direct application of the laws of thermodynamics is somewhat simpler than applying them indirectly by solving the Navier-Stokes (NS) equations. Both disciplines show that the preferred strategy for minimizing the reduction in peak quality caused by temperature <span class="hlt">gradients</span> is to operate columns as nearly adiabatically as possible (i.e. as Joule-Thomson expansions). This useful fact, however, is not widely familiar or appreciated in the chromatography community due to some misunderstanding of the meaning of certain terms and expressions used in these disciplines. In fluid dynamics, the terms "resistive heating" or "frictional heating" have been widely used as synonyms for the dissipation function, Φ, in the NS energy equation. These terms have been widely used by chromatographers as well, but often misinterpreted as due to friction between the mobile phase and the column packing, when in fact Φ describes the increase in entropy of the system (dissipation, ∫TdSuniv>0) due to the irreversible decompression of the mobile phase. Two distinctly different contributions to the irreversibility are identified; (1) ΔSext, viscous dissipation of work done by the external surroundings driving the flow (the pump) contributing to its warming, and (2) ΔSint, entropy change accompanying decompression of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1983BoLMe..27...69G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1983BoLMe..27...69G"><span>Low-level wind response to mesoscale <span class="hlt">pressure</span> systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Garratt, J. R.; Physick, W. L.</p> <p>1983-09-01</p> <p>Observations are presented which show a strong correlation between low-level wind behaviour (e.g., rotation near the surface) and the passage of mesoscale <span class="hlt">pressure</span> systems. The latter are associated with frontal transition zones, are dominated by a <span class="hlt">pressure</span>-jump line and a mesoscale high <span class="hlt">pressure</span> area, and produce locally large horizontal <span class="hlt">pressure</span> <span class="hlt">gradients</span>. The wind observations are simulated by specifying a time sequence of perturbation <span class="hlt">pressure</span> <span class="hlt">gradient</span> and subsequently solving the vertically-integrated momentum equations with appropriate initial conditions. Very good agreement is found between observed and calculated winds; in particular, (i) a 360 ° rotation in wind on passage of the mesoscale high; (ii) wind-shift lines produced dynamically by the <span class="hlt">pressure</span>-jump line; (iii) rapid linear increase in wind speed on passage of the <span class="hlt">pressure</span> jump.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25454130','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25454130"><span>Using contemporary liquid chromatography theory and technology to improve capillary <span class="hlt">gradient</span> ion-exchange separations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wouters, Bert; Broeckhoven, Ken; Wouters, Sam; Bruggink, Cees; Agroskin, Yury; Pohl, Christopher A; Eeltink, Sebastiaan</p> <p>2014-11-28</p> <p>The <span class="hlt">gradient</span>-performance limits of capillary ion chromatography have been assessed at maximum system <span class="hlt">pressure</span> (34.5 MPa) using capillary columns packed with 4.1 μm macroporous anion-exchange particles coated with 65 nm positively-charged nanobeads. In analogy to the van-Deemter curve, the <span class="hlt">gradient</span> performance was assessed applying different flow rates, while decreasing the <span class="hlt">gradient</span> time inversely proportional to the increase in flow rate in order to maintain the same retention properties. The <span class="hlt">gradient</span> kinetic-performance limits were determined at maximum system <span class="hlt">pressure</span>, applying tG/t0=5, 10, and 20. In addition, the effect of retention on peak width was assessed in <span class="hlt">gradient</span> mode for mono-, di-, and trivalent inorganic anions. The peak width of late-eluting ions can be significantly reduced by using concave <span class="hlt">gradient</span>, resulting in better detection sensitivity. A signal enhancement factor of 8 was measured for a late-eluting ion when applying a concave instead of a linear <span class="hlt">gradient</span>. For the analysis of a complex anion mixture, a coupled column with a total length of 1.05 m was operated at the kinetic-performance limit applying a linear 250 min <span class="hlt">gradient</span> (tG/t0=10). The peak capacity varied between 200 and 380 depending on analyte retention, and hence on charge and size of the ion. Copyright © 2014 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007APS..DPPTO3006H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007APS..DPPTO3006H"><span>A stepped <span class="hlt">pressure</span> profile model for internal transport barriers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hole, Matthew; Hudson, Stuart; Dewar, Robert</p> <p>2007-11-01</p> <p>B ∇x et al We develop a multiple interface variational model, comprising multiple Taylor-relaxed plasma regions separated by <span class="hlt">ideal</span> MHD barriers. The magnetic field in each region is Beltrami, = μ, and the <span class="hlt">pressure</span> constant. Between these regions the <span class="hlt">pressure</span>, field strength, and rotational transform may have step changes at the <span class="hlt">ideal</span> barrier. A principle motivation is the development of a mathematically rigorous <span class="hlt">ideal</span> MHD model to describe intrinsically 3D equilibria, with nonzero internal <span class="hlt">pressure</span>, using robust KAM surfaces as the barriers. As each region is locally relaxed however, such a model may also yield reasons for existence of internal transport barriers (ITBs). Focusing on the latter, we build on Hole Nuc. Fus. 47, pp746-753, 2007, which recently studied the stability of a two-interface periodic-cylinder configuration. In this work, we perform a stability scan over <span class="hlt">pressure</span> and for a two-interface configuration with no jump in , and compare the characteristics of stable equilibria to those of ITB's.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20309904','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20309904"><span>Comparison of various second-dimension <span class="hlt">gradient</span> types in comprehensive two-dimensional liquid chromatography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jandera, Pavel; Hájek, Tomás; Cesla, Petr</p> <p>2010-06-01</p> <p><span class="hlt">Gradient</span> elution provides significant improvement in peak capacity with respect to isocratic conditions. In the second dimension, <span class="hlt">gradients</span> are limited to a short-time period available for separation. Various types of second-dimension <span class="hlt">gradients</span> in comprehensive LC x LC are compared: (i) "full in fraction", (ii) "segment in fraction" and (iii) "continuously shifting" <span class="hlt">gradients</span>, applied in orthogonal LC x LC separations of phenolic acids and flavones on a polyethylene glycol column in the first dimension and two types of porous shell fused-core C18 columns in the second dimension (Ascentis Express and Kinetex). The porous shell columns provide narrow bandwidths and fast second-dimension separations at moderate operating <span class="hlt">pressure</span> that allows important savings of the overall separation time in comprehensive LC x LC separations. The effects of the <span class="hlt">gradient</span> type on the bandwidths, theoretical peak capacity, separation time and column <span class="hlt">pressure</span> in the second dimension were investigated. The type of <span class="hlt">gradient</span> program controls the range of lipophilicity of sample compounds that can be separated in the second-dimension reversed-phase time period. This range can be calibrated using alkylbenzene standards, to design the separation conditions for complete sample separation, avoiding harmful wrap around of non-eluted compounds to the subsequent second-dimension fractions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20665798','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20665798"><span>Shaping and timing <span class="hlt">gradient</span> pulses to reduce MRI acoustic noise.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Segbers, Marcel; Rizzo Sierra, Carlos V; Duifhuis, Hendrikus; Hoogduin, Johannes M</p> <p>2010-08-01</p> <p>A method to reduce the acoustic noise generated by <span class="hlt">gradient</span> systems in MRI has been recently proposed; such a method is based on the linear response theory. Since the physical cause of MRI acoustic noise is the time derivative of the <span class="hlt">gradient</span> current, a common trapezoid current shape produces an acoustic <span class="hlt">gradient</span> coil response mainly during the rising and falling edge. In the falling edge, the coil acoustic response presents a 180 degrees phase difference compared to the rising edge. Therefore, by varying the width of the trapezoid and keeping the ramps constant, it is possible to suppress one selected frequency and its higher harmonics. This value is matched to one of the prominent resonance frequencies of the <span class="hlt">gradient</span> coil system. The idea of cancelling a single frequency is extended to a second frequency, using two successive trapezoid-shaped pulses presented at a selected interval. Overall sound <span class="hlt">pressure</span> level reduction of 6 and 10 dB is found for the two trapezoid shapes and a single pulse shape, respectively. The acoustically optimized pulse shape proposed is additionally tested in a simulated echo planar imaging readout train, obtaining a sound <span class="hlt">pressure</span> level reduction of 12 dB for the best case.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4664389','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4664389"><span>Effects of Drought, Pest <span class="hlt">Pressure</span> and Light Availability on Seedling Establishment and Growth: Their Role for Distribution of Tree Species across a Tropical Rainfall <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Gaviria, Julian; Engelbrecht, Bettina M. J.</p> <p>2015-01-01</p> <p>Tree species distributions associated with rainfall are among the most prominent patterns in tropical forests. Understanding the mechanisms shaping these patterns is important to project impacts of global climate change on tree distributions and diversity in the tropics. Beside direct effects of water availability, additional factors co-varying with rainfall have been hypothesized to play an important role, including pest <span class="hlt">pressure</span> and light availability. While low water availability is expected to exclude drought-intolerant wet forest species from drier forests (physiological tolerance hypothesis), high pest <span class="hlt">pressure</span> or low light availability are hypothesized to exclude dry forest species from wetter forests (pest <span class="hlt">pressure</span> <span class="hlt">gradient</span> and light availability hypothesis, respectively). To test these hypotheses at the seed-to-seedling transition, the potentially most critical stage for species discrimination, we conducted a reciprocal transplant experiment combined with a pest exclosure treatment at a wet and a dry forest site in Panama with seeds of 26 species with contrasting origin. Establishment success after one year did not reflect species distribution patterns. However, in the wet forest, wet origin species had a home advantage over dry forest species through higher growth rates. At the same time, drought limited survival of wet origin species in the dry forest, supporting the physiological tolerance hypothesis. Together these processes sort species over longer time frames, and exclude species outside their respective home range. Although we found pronounced effects of pests and some effects of light availability on the seedlings, they did not corroborate the pest <span class="hlt">pressure</span> nor light availability hypotheses at the seed-to-seedling transition. Our results underline that changes in water availability due to climate change will have direct consequences on tree regeneration and distributions along tropical rainfall <span class="hlt">gradients</span>, while indirect effects of light and pests</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/ED441793.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/ED441793.pdf"><span>The Place of <span class="hlt">Ideals</span> in Teaching.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Hansen, David T.</p> <p></p> <p>This paper examines whether <span class="hlt">ideals</span> and <span class="hlt">idealism</span> have a role to play in teaching, identifying some ambiguities and problems associated with <span class="hlt">ideals</span> and arguing that <span class="hlt">ideals</span> figure importantly in teaching, but they are <span class="hlt">ideals</span> of character or personhood as much as they are <span class="hlt">ideals</span> of educational purpose. The first section focuses on the promise and…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920052415&hterms=weather+map+humidity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dweather%2Bmap%2Bhumidity','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920052415&hterms=weather+map+humidity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dweather%2Bmap%2Bhumidity"><span>Surface <span class="hlt">pressure</span> maps from scatterometer data</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Brown, R. A.; Levy, Gad</p> <p>1991-01-01</p> <p>The ability to determine surface <span class="hlt">pressure</span> fields from satellite scatterometer data was shown by Brown and Levy (1986). The surface winds are used to calculate the <span class="hlt">gradient</span> winds above the planetary boundary layer, and these are directly related to the <span class="hlt">pressure</span> <span class="hlt">gradients</span>. There are corrections for variable stratification, variable surface roughness, horizontal inhomogeneity, humidity and baroclinity. The Seasat-A Satellite Scatterometer (SASS) data have been used in a systematic study of 50 synoptic weather events (regions of approximately 1000 X 1000 km). The preliminary statistics of agreement with national weather service surface <span class="hlt">pressure</span> maps are calculated. The resulting surface <span class="hlt">pressure</span> maps can be used together with SASS winds and Scanning Multichannel Microwave Radiometer (SMMR) water vapor and liquid water analyses to provide good front and storm system analyses.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..GECDT1003G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..GECDT1003G"><span>Collisionless Spectral Kinetic Simulation of <span class="hlt">Ideal</span> Multipole Resonance Probe</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gong, Junbo; Wilczek, Sebastian; Szeremley, Daniel; Oberrath, Jens; Eremin, Denis; Dobrygin, Wladislaw; Schilling, Christian; Friedrichs, Michael; Brinkmann, Ralf Peter</p> <p>2016-09-01</p> <p>Active Plasma Resonance Spectroscopy denotes a class of industry-compatible plasma diagnostic methods which utilize the natural ability of plasmas to resonate on or near the electron plasma frequency ωpe. One particular realization of APRS with a high degree of geometric and electric symmetry is the Multipole Resonance Probe (MRP). The <span class="hlt">Ideal</span> MRP(IMRP) is an even more symmetric <span class="hlt">idealization</span> which is suited for theoretical investigations. In this work, a spectral kinetic scheme is presented to investigate the behavior of the IMRP in the low <span class="hlt">pressure</span> regime. However, due to the velocity difference, electrons are treated as particles whereas ions are only considered as stationary background. In the scheme, the particle pusher integrates the equations of motion for the studied particles, the Poisson solver determines the electric field at each particle position. The proposed method overcomes the limitation of the cold plasma model and covers kinetic effects like collisionless damping.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4995943','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4995943"><span>Intratumoral oxygen <span class="hlt">gradients</span> mediate sarcoma cell invasion</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Lewis, Daniel M.; Park, Kyung Min; Tang, Vitor; Xu, Yu; Pak, Koreana; Eisinger-Mathason, T. S. Karin; Simon, M. Celeste; Gerecht, Sharon</p> <p>2016-01-01</p> <p>Hypoxia is a critical factor in the progression and metastasis of many cancers, including soft tissue sarcomas. Frequently, oxygen (O2) <span class="hlt">gradients</span> develop in tumors as they grow beyond their vascular supply, leading to heterogeneous areas of O2 depletion. Here, we report the impact of hypoxic O2 <span class="hlt">gradients</span> on sarcoma cell invasion and migration. O2 <span class="hlt">gradient</span> measurements showed that large sarcoma mouse tumors (>300 mm3) contain a severely hypoxic core [≤0.1% partial <span class="hlt">pressure</span> of O2 (pO2)] whereas smaller tumors possessed hypoxic <span class="hlt">gradients</span> throughout the tumor mass (0.1–6% pO2). To analyze tumor invasion, we used O2-controllable hydrogels to recreate the physiopathological O2 levels in vitro. Small tumor grafts encapsulated in the hydrogels revealed increased invasion that was both faster and extended over a longer distance in the hypoxic hydrogels compared with nonhypoxic hydrogels. To model the effect of the O2 <span class="hlt">gradient</span> accurately, we examined individual sarcoma cells embedded in the O2-controllable hydrogel. We observed that hypoxic <span class="hlt">gradients</span> guide sarcoma cell motility and matrix remodeling through hypoxia-inducible factor-1α (HIF-1α) activation. We further found that in the hypoxic <span class="hlt">gradient</span>, individual cells migrate more quickly, across longer distances, and in the direction of increasing O2 tension. Treatment with minoxidil, an inhibitor of hypoxia-induced sarcoma metastasis, abrogated cell migration and matrix remodeling in the hypoxic <span class="hlt">gradient</span>. Overall, we show that O2 acts as a 3D physicotactic agent during sarcoma tumor invasion and propose the O2-controllable hydrogels as a predictive system to study early stages of the metastatic process and therapeutic targets. PMID:27486245</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27486245','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27486245"><span>Intratumoral oxygen <span class="hlt">gradients</span> mediate sarcoma cell invasion.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lewis, Daniel M; Park, Kyung Min; Tang, Vitor; Xu, Yu; Pak, Koreana; Eisinger-Mathason, T S Karin; Simon, M Celeste; Gerecht, Sharon</p> <p>2016-08-16</p> <p>Hypoxia is a critical factor in the progression and metastasis of many cancers, including soft tissue sarcomas. Frequently, oxygen (O2) <span class="hlt">gradients</span> develop in tumors as they grow beyond their vascular supply, leading to heterogeneous areas of O2 depletion. Here, we report the impact of hypoxic O2 <span class="hlt">gradients</span> on sarcoma cell invasion and migration. O2 <span class="hlt">gradient</span> measurements showed that large sarcoma mouse tumors (>300 mm(3)) contain a severely hypoxic core [≤0.1% partial <span class="hlt">pressure</span> of O2 (pO2)] whereas smaller tumors possessed hypoxic <span class="hlt">gradients</span> throughout the tumor mass (0.1-6% pO2). To analyze tumor invasion, we used O2-controllable hydrogels to recreate the physiopathological O2 levels in vitro. Small tumor grafts encapsulated in the hydrogels revealed increased invasion that was both faster and extended over a longer distance in the hypoxic hydrogels compared with nonhypoxic hydrogels. To model the effect of the O2 <span class="hlt">gradient</span> accurately, we examined individual sarcoma cells embedded in the O2-controllable hydrogel. We observed that hypoxic <span class="hlt">gradients</span> guide sarcoma cell motility and matrix remodeling through hypoxia-inducible factor-1α (HIF-1α) activation. We further found that in the hypoxic <span class="hlt">gradient</span>, individual cells migrate more quickly, across longer distances, and in the direction of increasing O2 tension. Treatment with minoxidil, an inhibitor of hypoxia-induced sarcoma metastasis, abrogated cell migration and matrix remodeling in the hypoxic <span class="hlt">gradient</span>. Overall, we show that O2 acts as a 3D physicotactic agent during sarcoma tumor invasion and propose the O2-controllable hydrogels as a predictive system to study early stages of the metastatic process and therapeutic targets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16231132','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16231132"><span>Thermodynamics of an <span class="hlt">ideal</span> generalized gas: I. Thermodynamic laws.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lavenda, B H</p> <p>2005-11-01</p> <p>The equations of state for an <span class="hlt">ideal</span> relativistic, or generalized, gas, like an <span class="hlt">ideal</span> quantum gas, are expressed in terms of power laws of the temperature. In contrast to an <span class="hlt">ideal</span> classical gas, the internal energy is a function of volume at constant temperature, implying that the <span class="hlt">ideal</span> generalized gas will show either attractive or repulsive interactions. This is a necessary condition in order that the third law be obeyed and for matter to have an electromagnetic origin. The transition from an <span class="hlt">ideal</span> generalized to a classical gas occurs when the two independent solutions of the subsidiary equation to Lagrange's equation coalesce. The equation of state relating the <span class="hlt">pressure</span> to the internal energy encompasses the full range of cosmological scenarios, from the radiation to the matter dominated universes and finally to the vacuum energy, enabling the coefficient of proportionality, analogous to the Grüeisen ratio, to be interpreted in terms of the degrees of freedom related to the temperature exponents of the internal energy and the absolute temperature expressed in terms of a power of the empirical temperature. The limit where these exponents merge is shown to be the <span class="hlt">ideal</span> classical gas limit. A corollary to Carnot's theorem is proved, asserting that the ratio of the work done over a cycle to the heat absorbed to increase the temperature at constant volume is the same for all bodies at the same volume. As power means, the energy and entropy are incomparable, and a new adiabatic potential is introduced by showing that the volume raised to a characteristic exponent is also the integrating factor for the quantity of heat so that the second law can be based on the property that power means are monotonically increasing functions of their order. The vanishing of the chemical potential in extensive systems implies that energy cannot be transported without matter and is equivalent to the condition that Clapeyron's equation be satisfied.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70016699','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70016699"><span>Determining the mean hydraulic <span class="hlt">gradient</span> of ground water affected by tidal fluctuations</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Serfes, Michael E.</p> <p>1991-01-01</p> <p>Tidal fluctuations in surface-water bodies produce progressive <span class="hlt">pressure</span> waves in adjacent aquifers. As these <span class="hlt">pressure</span> waves propagate inland, ground-water levels and hydraulic <span class="hlt">gradients</span> continuously fluctuate, creating a situation where a single set of water-level measurements cannot be used to accurately characterize ground-water flow. For example, a time series of water levels measured in a confined aquifer in Atlantic City, New Jersey, showed that the hydraulic <span class="hlt">gradient</span> ranged from .01 to .001 with a 22-degree change in direction during a tidal day of approximately 25 hours. At any point where ground water tidally fluctuates, the magnitude and direction of the hydraulic <span class="hlt">gradient</span> fluctuates about the mean or regional hydraulic <span class="hlt">gradient</span>. The net effect of these fluctuations on ground-water flow can be determined using the mean hydraulic <span class="hlt">gradient</span>, which can be calculated by comparing mean ground- and surface-water elevations. Filtering methods traditionally used to determine daily mean sea level can be similarly applied to ground water to determine mean levels. Method (1) uses 71 consecutive hourly water-level observations to accurately determine the mean level. Method (2) approximates the mean level using only 25 consecutive hourly observations; however, there is a small error associated with this method.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhPl...23d2509O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhPl...23d2509O"><span>Interaction between neoclassical effects and ion temperature <span class="hlt">gradient</span> turbulence in <span class="hlt">gradient</span>- and flux-driven gyrokinetic simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Oberparleiter, M.; Jenko, F.; Told, D.; Doerk, H.; Görler, T.</p> <p>2016-04-01</p> <p>Neoclassical and turbulent transport in tokamaks has been studied extensively over the past decades, but their possible interaction remains largely an open question. The two are only truly independent if the length scales governing each of them are sufficiently separate, i.e., if the ratio ρ* between ion gyroradius and the <span class="hlt">pressure</span> <span class="hlt">gradient</span> scale length is small. This is not the case in particularly interesting regions such as transport barriers. Global simulations of a collisional ion-temperature-<span class="hlt">gradient</span>-driven microturbulence performed with the nonlinear global gyrokinetic code Gene are presented. In particular, comparisons are made between systems with and without neoclassical effects. In fixed-<span class="hlt">gradient</span> simulations, the modified radial electric field is shown to alter the zonal flow pattern such that a significant increase in turbulent transport is observed for ρ*≳1 /300 . Furthermore, the dependency of the flux on the collisionality changes. In simulations with fixed power input, we find that the presence of neoclassical effects decreases the frequency and amplitude of intermittent turbulent transport bursts (avalanches) and thus plays an important role for the self-organisation behaviour.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110023790','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110023790"><span>Turbulence in Supercritical O2/H2 and C7H16/N2 Mixing Layers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bellan, Josette; Harstad, Kenneth; Okong'o, Nora</p> <p>2003-01-01</p> <p>This report presents a study of numerical simulations of mixing layers developing between opposing flows of paired fluids under supercritical conditions, the purpose of the study being to elucidate chemical-species-specific aspects of turbulence. The simulations were performed for two different fluid pairs O2/H2 and C7H16/N2 at similar reduced initial <span class="hlt">pressures</span> (reduced <span class="hlt">pressure</span> is defined as <span class="hlt">pressure</span> divided by critical <span class="hlt">pressure</span>). Thermodynamically, O2/H2 behaves more nearly like an <span class="hlt">ideal</span> mixture and has greater solubility, relative to C7H16/N2, which departs strongly from <span class="hlt">ideality</span>. Because of a specified smaller initial density stratification, the C7H16/N2 layers exhibited greater levels of growth, global molecular mixing, and turbulence. However, smaller density <span class="hlt">gradients</span> at the transitional state for the O2/H2 system were interpreted as indicating that locally, this system exhibits enhanced mixing as a consequence of its greater solubility and closer approach to <span class="hlt">ideality</span>. These thermodynamic features were shown to affect entropy dissipation, which was found to be larger for O2/H2 and concentrated in high-density-<span class="hlt">gradient</span>-magnitude regions that are distortions of the initial density-stratification boundary. In C7H16/N2, the regions of largest dissipation were found to lie in high-density-<span class="hlt">gradient</span>-magnitude regions that result from mixing of the two fluids.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5319800','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5319800"><span><span class="hlt">Ideal</span> Cardiovascular Health, Cardiovascular Remodeling, and Heart Failure in African-Americans: the Jackson Heart Study</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Spahillari, Aferdita; Talegawkar, Sameera; Correa, Adolfo; Carr, J. Jeffrey; Terry, James G.; Lima, Joao; Freedman, Jane E.; Das, Saumya; Kociol, Robb; de Ferranti, Sarah; Mohebali, Donya; Mwasongwe, Stanford; Tucker, Katherine L.; Murthy, Venkatesh L.; Shah, Ravi V.</p> <p>2017-01-01</p> <p>Background The lifetime risk of heart failure is higher in the African-American population than in other racial groups in the United States. Methods and Results We measured the Life’s Simple 7 <span class="hlt">ideal</span> cardiovascular health metrics in 4195 African-Americans in the Jackson Heart Study (2000–2004). We evaluated the association of Simple 7 metrics with incident HF and left ventricular (LV) structure and function by cardiac magnetic resonance (CMR; n=1188). Mean age at baseline was 54.4 years (65% women). Relative to 0–2 Simple 7 factors, African-Americans with 3 factors had 47% lower incident HF risk (HR 0.53, 95% CI 0.39–0.73, P<0.0001); those with ≥ 4 factors had 61% lower HF risk (HR 0.39, 95% CI 0.24–0.64, P=0.0002). Higher blood <span class="hlt">pressure</span> (HR 2.32, 95% CI 1.28–4.20, P=0.005), physical inactivity (HR 1.65, 95% CI 1.07–2.55, P=0.02), smoking (HR 2.04, 95% CI 1.43–2.91, P<0.0001) and impaired glucose control (HR 1.76, 95% CI 1.34–2.29, P<0.0001) were associated with incident HF. The age-/sex-adjusted population attributable risk for these Simple 7 metrics combined was 37.1%. Achievement of <span class="hlt">ideal</span> blood <span class="hlt">pressure</span>, <span class="hlt">ideal</span> body mass index, <span class="hlt">ideal</span> glucose control, and non-smoking was associated with less likelihood of adverse cardiac remodeling by CMR. Conclusions Cardiovascular risk factors in mid-life (specifically elevated blood <span class="hlt">pressure</span>, physical inactivity, smoking and poor glucose control) are associated with incident HF in African Americans, and represent targets for intensified HF prevention. PMID:28209767</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25516954','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25516954"><span>Medical ethics and more: <span class="hlt">ideal</span> theories, non-<span class="hlt">ideal</span> theories and conscientious objection.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Luna, Florencia</p> <p>2015-01-01</p> <p>Doing 'good medical ethics' requires acknowledgment that it is often practised in non-<span class="hlt">ideal</span> circumstances! In this article I present the distinction between <span class="hlt">ideal</span> theory (IT) and non-<span class="hlt">ideal</span> theory (NIT). I show how IT may not be the best solution to tackle problems in non-<span class="hlt">ideal</span> contexts. I sketch a NIT framework as a useful tool for bioethics and medical ethics and explain how NITs can contribute to policy design in non-<span class="hlt">ideal</span> circumstances. Different NITs can coexist and be evaluated vis-à-vis the IT. Additionally, I address what an individual doctor ought to do in this non-<span class="hlt">ideal</span> context with the view that knowledge of NITs can facilitate the decision-making process. NITs help conceptualise problems faced in the context of non-compliance and scarcity in a better and more realistic way. Deciding which policy is optimal in such contexts may influence physicians' decisions regarding their patients. Thus, this analysis-usually identified only with policy making-may also be relevant to medical ethics. Finally, I recognise that this is merely a first step in an unexplored but fundamental theoretical area and that more work needs to be done. Published by the BMJ Publishing Group Limited. For permission to use (where not already granted under a licence) please go to http://group.bmj.com/group/rights-licensing/permissions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28297963','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28297963"><span>Enhanced settling of nonheavy inertial particles in homogeneous isotropic turbulence: The role of the <span class="hlt">pressure</span> <span class="hlt">gradient</span> and the Basset history force.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>van Hinsberg, M A T; Clercx, H J H; Toschi, F</p> <p>2017-02-01</p> <p>The Stokes drag force and the gravity force are usually sufficient to describe the behavior of sub-Kolmogorov-size (or pointlike) heavy particles in turbulence, in particular when the particle-to-fluid density ratio ρ_{p}/ρ_{f}≳10^{3} (with ρ_{p} and ρ_{f} the particle and fluid density, respectively). This is, in general, not the case for smaller particle-to-fluid density ratios, in particular not for ρ_{p}/ρ_{f}≲10^{2}. In that case the <span class="hlt">pressure</span> <span class="hlt">gradient</span> force, added mass effects, and the Basset history force also play important roles. In this study we focus on the understanding of the role of these additional forces, all of hydrodynamic origin, in the settling of particles in turbulence. In order to qualitatively elucidate the complex dynamics of such particles in homogeneous isotropic turbulence, we first focus on the case of settling of such particles in the flow field of a single vortex. After having explored this simplified case we extend our analysis to homogeneous isotropic turbulence. In general, we found that the <span class="hlt">pressure</span> <span class="hlt">gradient</span> force leads to a decrease in the settling velocity. This can be qualitatively understood by the fact that this force prevents the particles from sweeping out of vortices, a mechanism known as preferential sweeping which causes enhanced settling. Additionally, we found that the Basset history force can both increase and decrease the enhanced settling, depending on the particle Stokes number. Finally, the role of the nonlinear Stokes drag has been explored, confirming that it affects settling of inertial particles in turbulence, but only in a limited way for the parameter settings used in this investigation.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_15 --> <div id="page_16" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="301"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27806903','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27806903"><span>High-<span class="hlt">pressure</span> balloon dilation in a dog with supravalvular aortic stenosis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pinkos, A; Stauthammer, C; Rittenberg, R; Barncord, K</p> <p>2017-02-01</p> <p>A 6-month-old female intact Goldendoodle was presented for diagnostic work up of a grade IV/VI left basilar systolic heart murmur. An echocardiogram was performed and revealed a ridge of tissue distal to the aortic valve leaflets at the sinotubular junction causing an instantaneous <span class="hlt">pressure</span> <span class="hlt">gradient</span> of 62 mmHg across the supravalvular aortic stenosis and moderate concentric hypertrophy of the left ventricle. Intervention with a high-<span class="hlt">pressure</span> balloon dilation catheter was pursued and significantly decreased the <span class="hlt">pressure</span> <span class="hlt">gradient</span> to 34 mmHg. No complications were encountered. The patient returned in 5 months for re-evaluation and static long-term reduction in the <span class="hlt">pressure</span> <span class="hlt">gradient</span> was noted. Copyright © 2016 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27702615','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27702615"><span>Development of a 45kpsi ultrahigh <span class="hlt">pressure</span> liquid chromatography instrument for <span class="hlt">gradient</span> separations of peptides using long microcapillary columns and sub-2μm particles.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Grinias, Kaitlin M; Godinho, Justin M; Franklin, Edward G; Stobaugh, Jordan T; Jorgenson, James W</p> <p>2016-10-21</p> <p>Commercial chromatographic instrumentation for bottom-up proteomics is often inadequate to resolve the number of peptides in many samples. This has inspired a number of complex approaches to increase peak capacity, including various multidimensional approaches, and reliance on advancements in mass spectrometry. One-dimensional reversed phase separations are limited by the <span class="hlt">pressure</span> capabilities of commercial instruments and prevent the realization of greater separation power in terms of speed and resolution inherent to smaller sorbents and ultrahigh <span class="hlt">pressure</span> liquid chromatography. Many applications with complex samples could benefit from the increased separation performance of long capillary columns packed with sub-2μm sorbents. Here, we introduce a system that operates at a constant <span class="hlt">pressure</span> and is capable of separations at <span class="hlt">pressures</span> up to 45kpsi. The system consists of a commercially available capillary liquid chromatography instrument, for sample management and <span class="hlt">gradient</span> creation, and is modified with a storage loop and isolated pneumatic amplifier pump for elevated separation <span class="hlt">pressure</span>. The system's performance is assessed with a complex peptide mixture and a range of microcapillary columns packed with sub-2μm C18 particles. Copyright © 2016 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160010267','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160010267"><span>Impact of an Exhaust Throat on Semi-<span class="hlt">Idealized</span> Rotating Detonation Engine Performance</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Paxson, Daniel E.</p> <p>2016-01-01</p> <p>A computational fluid dynamic (CFD) model of a rotating detonation engine (RDE) is used to examine the impact of an exhaust throat (i.e. a constriction) on performance. The model simulates an RDE which is premixed, adiabatic, inviscid, and which contains an inlet valve that prevents backflow from the high <span class="hlt">pressure</span> region directly behind the rotating detonation. Performance is assessed in terms of <span class="hlt">ideal</span> net specific impulse which is computed on the assumption of lossless expansion of the working fluid to the ambient <span class="hlt">pressure</span> through a notional diverging nozzle section downstream of the throat. Such a semi-<span class="hlt">idealized</span> analysis, while not real-world, allows the effect of the throat to be examined in isolation from, rather than coupled to (as it actually is) various loss mechanisms. For the single Mach 1.4 flight condition considered, it is found that the addition of a throat can yield a 9.4 percent increase in specific impulse. However, it is also found that when the exit throat restriction gets too small, an unstable type of operation ensues which eventually leads to the detonation failing. This behavior is found to be somewhat mitigated by the addition of an RDE inlet restriction across which there is an aerodynamic loss. Remarkably, this loss is overcome by the benefits of the further exhaust restrictions allowed. The end result is a configuration with a 10.3 percent improvement in <span class="hlt">ideal</span> net specific thrust.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160005410','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160005410"><span>Impact of an Exhaust Throat on Semi-<span class="hlt">Idealized</span> Rotating Detonation Engine Performance</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Paxson, Daniel E.</p> <p>2016-01-01</p> <p>A computational fluid dynamic (CFD) model of a rotating detonation engine (RDE) is used to examine the impact of an exhaust throat (i.e., a constriction) on performance. The model simulates an RDE which is premixed, adiabatic, inviscid, and which contains an inlet valve that prevents backflow from the high <span class="hlt">pressure</span> region directly behind the rotating detonation. Performance is assessed in terms of <span class="hlt">ideal</span> net specific impulse which is computed on the assumption of lossless expansion of the working fluid to the ambient <span class="hlt">pressure</span> through a notional diverging nozzle section downstream of the throat. Such a semi-<span class="hlt">idealized</span> analysis, while not real-world, allows the effect of the throat to be examined in isolation from, rather than coupled to (as it actually is) various loss mechanisms. For the single Mach 1.4 flight condition considered, it is found that the addition of a throat can yield a 9.4 percent increase in specific impulse. However, it is also found that when the exit throat restriction gets too small, an unstable type of operation ensues which eventually leads to the detonation failing. This behavior is found to be somewhat mitigated by the addition of an RDE inlet restriction across which there is an aerodynamic loss. Remarkably, this loss is overcome by the benefits of the further exhaust restrictions allowed. The end result is a configuration with a 10.3 percent improvement in <span class="hlt">ideal</span> net specific thrust.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/9165530','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/9165530"><span>Differential molar heat capacities to test <span class="hlt">ideal</span> solubility estimations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Neau, S H; Bhandarkar, S V; Hellmuth, E W</p> <p>1997-05-01</p> <p>Calculation of the <span class="hlt">ideal</span> solubility of a crystalline solute in a liquid solvent requires knowledge of the difference in the molar heat capacity at constant <span class="hlt">pressure</span> of the solid and the supercooled liquid forms of the solute, delta Cp. Since this parameter is not usually known, two assumptions have been used to simplify the expression. The first is that delta Cp can be considered equal to zero; the alternate assumption is that the molar entropy of fusion, delta Sf, is an estimate of delta Cp. Reports claiming the superiority of one assumption over the other, on the basis of calculations done using experimentally determined parameters, have appeared in the literature. The validity of the assumptions in predicting the <span class="hlt">ideal</span> solubility of five structurally unrelated compounds of pharmaceutical interest, with melting points in the range 420 to 470 K, was evaluated in this study. Solid and liquid heat capacities of each compound near its melting point were determined using differential scanning calorimetry. Linear equations describing the heat capacities were extrapolated to the melting point to generate the differential molar heat capacity. Linear data were obtained for both crystal and liquid heat capacities of sample and test compounds. For each sample, <span class="hlt">ideal</span> solubility at 298 K was calculated and compared to the two estimates generated using literature equations based on the differential molar heat capacity assumptions. For the compounds studied, delta Cp was not negligible and was closer to delta Sf than to zero. However, neither of the two assumptions was valid for accurately estimating the <span class="hlt">ideal</span> solubility as given by the full equation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5351808','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5351808"><span>Developmental <span class="hlt">Idealism</span> in China</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Thornton, Arland; Xie, Yu</p> <p>2016-01-01</p> <p>This paper examines the intersection of developmental <span class="hlt">idealism</span> with China. It discusses how developmental <span class="hlt">idealism</span> has been widely disseminated within China and has had enormous effects on public policy and programs, on social institutions, and on the lives of individuals and their families. This dissemination of developmental <span class="hlt">idealism</span> to China began in the 19th century, when China met with several military defeats that led many in the country to question the place of China in the world. By the beginning of the 20th century, substantial numbers of Chinese had reacted to the country’s defeats by exploring developmental <span class="hlt">idealism</span> as a route to independence, international respect, and prosperity. Then, with important but brief aberrations, the country began to implement many of the elements of developmental <span class="hlt">idealism</span>, a movement that became especially important following the assumption of power by the Communist Party of China in 1949. This movement has played a substantial role in politics, in the economy, and in family life. The beliefs and values of developmental <span class="hlt">idealism</span> have also been directly disseminated to the grassroots in China, where substantial majorities of Chinese citizens have assimilated them. These ideas are both known and endorsed by very large numbers in China today. PMID:28316833</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28316833','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28316833"><span>Developmental <span class="hlt">Idealism</span> in China.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Thornton, Arland; Xie, Yu</p> <p>2016-10-01</p> <p>This paper examines the intersection of developmental <span class="hlt">idealism</span> with China. It discusses how developmental <span class="hlt">idealism</span> has been widely disseminated within China and has had enormous effects on public policy and programs, on social institutions, and on the lives of individuals and their families. This dissemination of developmental <span class="hlt">idealism</span> to China began in the 19 th century, when China met with several military defeats that led many in the country to question the place of China in the world. By the beginning of the 20 th century, substantial numbers of Chinese had reacted to the country's defeats by exploring developmental <span class="hlt">idealism</span> as a route to independence, international respect, and prosperity. Then, with important but brief aberrations, the country began to implement many of the elements of developmental <span class="hlt">idealism</span>, a movement that became especially important following the assumption of power by the Communist Party of China in 1949. This movement has played a substantial role in politics, in the economy, and in family life. The beliefs and values of developmental <span class="hlt">idealism</span> have also been directly disseminated to the grassroots in China, where substantial majorities of Chinese citizens have assimilated them. These ideas are both known and endorsed by very large numbers in China today.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMNG14A..08F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMNG14A..08F"><span>The Effect of Large Scale Salinity <span class="hlt">Gradient</span> on Langmuir Turbulence</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fan, Y.; Jarosz, E.; Yu, Z.; Jensen, T.; Sullivan, P. P.; Liang, J.</p> <p>2017-12-01</p> <p>Langmuir circulation (LC) is believed to be one of the leading order causes of turbulent mixing in the upper ocean. It is important for momentum and heat exchange across the mixed layer (ML) and directly impact the dynamics and thermodynamics in the upper ocean and lower atmosphere including the vertical distributions of chemical, biological, optical, and acoustic properties. Based on Craik and Leibovich (1976) theory, large eddy simulation (LES) models have been developed to simulate LC in the upper ocean, yielding new insights that could not be obtained from field observations and turbulent closure models. Due its high computational cost, LES models are usually limited to small domain sizes and cannot resolve large-scale flows. Furthermore, most LES models used in the LC simulations use periodic boundary conditions in the horizontal direction, which assumes the physical properties (i.e. temperature and salinity) and expected flow patterns in the area of interest are of a periodically repeating nature so that the limited small LES domain is representative for the larger area. Using periodic boundary condition can significantly reduce computational effort in problems, and it is a good assumption for isotropic shear turbulence. However, LC is anisotropic (McWilliams et al 1997) and was observed to be modulated by crosswind tidal currents (Kukulka et al 2011). Using symmetrical domains, <span class="hlt">idealized</span> LES studies also indicate LC could interact with oceanic fronts (Hamlington et al 2014) and standing internal waves (Chini and Leibovich, 2005). The present study expands our previous LES modeling investigations of Langmuir turbulence to the real ocean conditions with large scale environmental motion that features fresh water inflow into the study region. Large scale <span class="hlt">gradient</span> forcing is introduced to the NCAR LES model through scale separation analysis. The model is applied to a field observation in the Gulf of Mexico in July, 2016 when the measurement site was impacted by</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1914596W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1914596W"><span>Towards improved estimation of the unsaturated soil hydraulic conductivity in the near saturated range by a fully automated, <span class="hlt">pressure</span> controlled unit <span class="hlt">gradient</span> experiment.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Werisch, Stefan; Müller, Marius</p> <p>2017-04-01</p> <p>Determination of soil hydraulic properties has always been an important part of soil physical research and model applications. While several experiments are available to measure the water retention of soil samples, the determination of the unsaturated hydraulic conductivity is often more complicated, bound to strong assumption and time consuming. Although, the application of unit <span class="hlt">gradient</span> experiments is recommended since the middle of the last century, as one method towards a (assumption free) direct measurement of the unsaturated hydraulic conductivity, data from unit <span class="hlt">gradient</span> experiments is seldom to never reported in literature. We developed and build a fully automated, <span class="hlt">pressure</span> controlled, unit <span class="hlt">gradient</span> experiment, which allows a precise determination of the unsaturated soil hydraulic conductivity K(h) and water retention VWC(h), especially in the highly dynamic near saturated range. The measurement apparatus applies the concept of hanging water columns and imposes the required soil water <span class="hlt">pressure</span> by dual porous plates. This concepts allows the simultaneous and direct measurement of water retention and hydraulic conductivity. Moreover, this approach results in a technically less demanding experiment than related flux controlled experiments, and virtually any flux can be measured. Thus, both soil properties can be measured in mm resolution, for wetting and drying processes, between saturation and field capacity for all soil types. Our results show, that it is important to establish separate measurements of the unsaturated hydraulic conductivity in the near saturated range, as the shape of the retention function and hydraulic conductivity curve do not necessarily match. Consequently, the prediction of the hydraulic conductivity curve from measurements of the water retention behavior in combination with a value for the saturated hydraulic conductivity can be misleading. Thus, separate parameterizations of the individual functions might be necessary and are</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29352698','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29352698"><span>Gastric Varices Bleed at Lower Portosystemic <span class="hlt">Pressure</span> <span class="hlt">Gradients</span> than Esophageal Varices.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Morrison, Joseph D; Mendoza-Elias, Nasya; Lipnik, Andrew J; Lokken, R Peter; Bui, James T; Ray, Charles E; Gaba, Ron C</p> <p>2018-05-01</p> <p>To quantify and compare portosystemic <span class="hlt">pressure</span> <span class="hlt">gradients</span> (PSGs) between bleeding esophageal varices (EV) and gastric varices (GV). In a single-center, retrospective study, 149 patients with variceal bleeding (90 men, 59 women, mean age 52 y) with EV (n = 69; 46%) or GV (n = 80; 54%) were selected from 320 consecutive patients who underwent successful transjugular intrahepatic portosystemic shunt (TIPS) creation from 1998 to 2016. GV were subcategorized using the Sarin classification as gastroesophageal varices (GEV) (n = 57) or isolated gastric varices (IGV) (n = 23). PSG before TIPS was measured from the main portal vein to the right atrium. PSGs were compared across EV, GEV, and IGV groups using 1-way analysis of variance. Overall mean baseline PSG was 21 mm Hg ± 6. PSG was significantly higher in patients with EV versus GV (23 mm Hg vs 19 mm Hg; P < .001). Mean PSG was highest among EV (23 mm Hg) with lower PSGs identified for GEV (20 mm Hg) and IGV (16 mm Hg); this difference was statistically significant (P < .001). Among 95 acute bleeding cases, a similar pattern was evident (EV 23 mm Hg vs GEV mm Hg 20 vs IGV 17 mm Hg; P < .001). At baseline PSG < 12 mm Hg, 13% (3/23) of IGV bled versus 9% (5/57) of GEV and 3% (2/69) of EVs (P = .169). Mean final PSG after TIPS was 8 mm Hg (IGV 6 mm Hg vs EV and GEV 8 mm Hg; P = .005). GV bleed at lower PSGs than EV. EV, GEV, and IGV bleeding is associated with successively lower PSGs. These findings highlight distinct physiology, anatomy, and behavior of GV compared with EV. Copyright © 2017 SIR. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016NatSR...622898D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016NatSR...622898D"><span><span class="hlt">Gradients</span> in pore size enhance the osteogenic differentiation of human mesenchymal stromal cells in three-dimensional scaffolds</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>di Luca, Andrea; Ostrowska, Barbara; Lorenzo-Moldero, Ivan; Lepedda, Antonio; Swieszkowski, Wojcech; van Blitterswijk, Clemens; Moroni, Lorenzo</p> <p>2016-03-01</p> <p>Small fractures in bone tissue can heal by themselves, but in case of larger defects current therapies are not completely successful due to several drawbacks. A possible strategy relies on the combination of additive manufactured polymeric scaffolds and human mesenchymal stromal cells (hMSCs). The architecture of bone tissue is characterized by a structural <span class="hlt">gradient</span>. Long bones display a structural <span class="hlt">gradient</span> in the radial direction, while flat bones in the axial direction. Such <span class="hlt">gradient</span> presents a variation in bone density from the cancellous bone to the cortical bone. Therefore, scaffolds presenting a <span class="hlt">gradient</span> in porosity could be <span class="hlt">ideal</span> candidates to improve bone tissue regeneration. In this study, we present a construct with a discrete <span class="hlt">gradient</span> in pore size and characterize its ability to further support the osteogenic differentiation of hMSCs. Furthermore, we studied the behaviour of hMSCs within the different compartments of the <span class="hlt">gradient</span> scaffolds, showing a correlation between osteogenic differentiation and ECM mineralization, and pore dimensions. Alkaline phosphatase activity and calcium content increased with increasing pore dimensions. Our results indicate that designing structural porosity <span class="hlt">gradients</span> may be an appealing strategy to support gradual osteogenic differentiation of adult stem cells.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADC041417','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADC041417"><span>Dynamic <span class="hlt">Pressure</span> Impulse for Near-<span class="hlt">Ideal</span> and Non-<span class="hlt">Ideal</span> Blast Waves -- Height of Burst Charts. Supplement</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1983-12-31</p> <p>Law 79-565), 22 April 1967. Other requests shall be referred to Director, Defense Nuclear Agency, Washington, DC 20305- 10101. THIS WORK WAS SPONSORED...JPUMNTNYNOTATIO This work was sponsored by the Defense Nuclear Agency under RDT&E RMSS Code 8344082466 Y99QAXSGO0039 H25900. I?. cosASI comR I& SUISCI TM...displacement which a vehicle exposed to a blast wave sufers can be used as a measure of the dynamic <span class="hlt">pressure</span> impulse it receives. ,hat is, the vehicle</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002CTM.....6..553K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002CTM.....6..553K"><span>Mechanisms of detonation formation due to a temperature <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kapila, A. K.; Schwendeman, D. W.; Quirk, J. J.; Hawa, T.</p> <p>2002-12-01</p> <p>Emergence of a detonation in a homogeneous, exothermically reacting medium can be deemed to occur in two phases. The first phase processes the medium so as to create conditions ripe for the onset of detonation. The actual events leading up to preconditioning may vary from one experiment to the next, but typically, at the end of this stage the medium is hot and in a state of nonuniformity. The second phase consists of the actual formation of the detonation wave via chemico-gasdynamic interactions. This paper considers an <span class="hlt">idealized</span> medium with simple, rate-sensitive kinetics for which the preconditioned state is modelled as one with an initially prescribed linear <span class="hlt">gradient</span> of temperature. Accurate and well-resolved numerical computations are carrried out to determine the mode of detonation formation as a function of the size of the initial <span class="hlt">gradient</span>. For shallow <span class="hlt">gradients</span>, the result is a decelerating supersonic reaction wave, a weak detonation, whose trajectory is dictated by the initial temperature profile, with only weak intervention from hydrodynamics. If the domain is long enough, or the <span class="hlt">gradient</span> less shallow, the wave slows down to the Chapman-Jouguet speed and undergoes a swift transition to the ZND structure. For sharp <span class="hlt">gradients</span>, gasdynamic nonlinearity plays a much stronger role. Now the path to detonation is through an accelerating pulse that runs ahead of the reaction wave and rearranges the induction-time distribution there to one that bears little resemblance to that corresponding to the initial temperature <span class="hlt">gradient</span>. The pulse amplifies and steepens, transforming itself into a complex consisting of a lead shock, an induction zone, and a following fast deflagration. As the pulse advances, its three constituent entities attain progressively higher levels of mutual coherence, to emerge as a ZND detonation. For initial <span class="hlt">gradients</span> that are intermediate in size, aspects of both the extreme scenarios appear in the path to detonation. The novel aspect of this study</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018RuMet2018...42P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018RuMet2018...42P"><span>Formation of <span class="hlt">Gradient</span> Structures in the Zone of Joining a Deformable Nickel Alloy and a Single-Crystal Intermetallic Alloy during Thermodiffusion <span class="hlt">Pressure</span> Welding and Subsequent Heat Treatment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Povarova, K. B.; Valitov, V. A.; Drozdov, A. A.; Bazyleva, O. A.; Galieva, E. V.; Arginbaeva, E. G.</p> <p>2018-01-01</p> <p>The possibility of formation of a high-quality solid-phase joint of an Ni3Al-based single-crystal intermetallic VKNA-25 blade alloy with a high-temperature deformable EP975 disk alloy by <span class="hlt">pressure</span> welding is studied to create high-performance one-piece blisk unit for the next-generation aviation gas turbine engines and to decrease the unit mass. The influence of the conditions of thermodiffusion <span class="hlt">pressure</span> welding under the hightemperature superplasticity of the disk alloy and the influence of heat treatment of welded joints on the <span class="hlt">gradient</span> structures in the welded joint zone and the structure at the periphery of the welded samples are investigated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140000685','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140000685"><span>Multiphase Transport in Porous Media: Gas-Liquid Separation Using Capillary <span class="hlt">Pressure</span> <span class="hlt">Gradients</span> International Space Station (ISS) Flight Experiment Development</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wheeler, Richard R., Jr.; Holtsnider, John T.; Dahl, Roger W.; Deeks, Dalton; Javanovic, Goran N.; Parker, James M.; Ehlert, Jim</p> <p>2013-01-01</p> <p>Advances in the understanding of multiphase flow characteristics under variable gravity conditions will ultimately lead to improved and as of yet unknown process designs for advanced space missions. Such novel processes will be of paramount importance to the success of future manned space exploration as we venture into our solar system and beyond. In addition, because of the ubiquitous nature and vital importance of biological and environmental processes involving airwater mixtures, knowledge gained about fundamental interactions and the governing properties of these mixtures will clearly benefit the quality of life here on our home planet. The techniques addressed in the current research involving multiphase transport in porous media and gas-liquid phase separation using capillary <span class="hlt">pressure</span> <span class="hlt">gradients</span> are also a logical candidate for a future International Space Station (ISS) flight experiment. Importantly, the novel and potentially very accurate Lattice-Boltzmann (LB) modeling of multiphase transport in porous media developed in this work offers significantly improved predictions of real world fluid physics phenomena, thereby promoting advanced process designs for both space and terrestrial applications.This 3-year research effort has culminated in the design and testing of a zero-g demonstration prototype. Both the hydrophilic (glass) and hydrophobic (Teflon) media Capillary <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> (CPG) cartridges prepared during the second years work were evaluated. Results obtained from ground testing at 1-g were compared to those obtained at reduced gravities spanning Martian (13-g), Lunar (16-g) and zero-g. These comparisons clearly demonstrate the relative strength of the CPG phenomena and the efficacy of its application to meet NASAs unique gas-liquid separation (GLS) requirements in non-terrestrial environments.LB modeling software, developed concurrently with the zero-g test effort, was shown to accurately reproduce observed CPG driven gas-liquid separation</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15476790','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15476790"><span>Spreading of nanofluids driven by the structural disjoining <span class="hlt">pressure</span> <span class="hlt">gradient</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chengara, Anoop; Nikolov, Alex D; Wasan, Darsh T; Trokhymchuk, Andrij; Henderson, Douglas</p> <p>2004-12-01</p> <p>This paper discusses the role of the structural disjoining <span class="hlt">pressure</span> exerted by nanoparticles on the spreading of a liquid film containing these particles. The origin of the structural disjoining <span class="hlt">pressure</span> in a confined geometry is due to the layering of the particles normal to the confining plane and has already been traced to the net increase in the entropy of the system in previous studies. In a recent paper, Wasan and Nikolov (Nature, 423 (2003) 156) pointed out that the structural component of the disjoining <span class="hlt">pressure</span> is strong enough to move a liquid wedge; this casts a new light on many applications-most notably, detergency. While the concept of spreading driven by the disjoining <span class="hlt">pressure</span> is not new, the importance of the structural disjoining <span class="hlt">pressure</span> arises from its long-range nature (as compared to the van der Waals' force), making it an important component of the overall force balance near the contact line. In this paper, we report on a parametric study of the spreading phenomena by examining the effects of nanoparticle size, concentration and polydispersity on the displacement of an oil-aqueous interface with the aqueous bulk containing nanoparticles. The solution of the extended Laplace-Young equations for the profile of the meniscus yields the position of the nominal contact line under the action of the structural disjoining <span class="hlt">pressure</span>. Simulations show that the displacement of the contact line is greater with a high nanoparticle volume fraction, small particles for the same volume fraction, monodispersed (in size) particles rather than polydispersed particles and when the resisting capillary <span class="hlt">pressure</span> is small, i.e., when the interfacial tension is low and/or the radius of the dispersed phase drop/bubble is large.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28295923','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28295923"><span>Effect of viral suppression on hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> in hepatitis C with cirrhosis and portal hypertension.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Afdhal, N; Everson, G T; Calleja, J L; McCaughan, G W; Bosch, J; Brainard, D M; McHutchison, J G; De-Oertel, S; An, D; Charlton, M; Reddy, K R; Asselah, T; Gane, E; Curry, M P; Forns, X</p> <p>2017-10-01</p> <p>Portal hypertension is a predictor of liver-related clinical events and mortality in patients with hepatitis C and cirrhosis. The effect of interferon-free hepatitis C treatment on portal <span class="hlt">pressure</span> is unknown. Fifty patients with Child-Pugh-Turcotte (CPT) A and B cirrhosis and portal hypertension (hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> [HVPG] >6 mm Hg) were randomized to receive 48 weeks of open-label sofosbuvir plus ribavirin at Day 1 or after a 24-week observation period. The primary endpoint was sustained virologic response 12 weeks after therapy (SVR12) in patients who received ≥1 dose of treatment. Secondary endpoints included changes in HVPG, laboratory parameters, and MELD and CPT scores. A subset of patients was followed 48 weeks posttreatment to determine late changes in HVPG. SVR12 occurred in 72% of patients (33/46). In the 37 patients with paired HVPG measurements at baseline and the end of treatment, mean HVPG decreased by -1.0 (SD 3.97) mm Hg. Nine patients (24%) had ≥20% decreases in HVPG during treatment. Among 39 patients with pretreatment HVPG ≥12 mm Hg, 27 (69%) achieved SVR12. Four of the 33 (12%) patients with baseline HVPG ≥12 mm Hg had HVPG <12 mm Hg at the end of treatment. Of nine patients with pretreatment HVPG ≥12 mm Hg who achieved SVR12 and completed 48 weeks of follow-up, eight (89%) had a ≥20% reduction in HVPG, and three reduced their <span class="hlt">pressure</span> to <12 mm Hg. Patients with chronic HCV and compensated or decompensated cirrhosis who achieve SVR can have clinically meaningful reductions in HVPG at long-term follow-up. (EudraCT 2012-002457-29). © 2017 John Wiley & Sons Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008Th%26Ae..15..369K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008Th%26Ae..15..369K"><span>Speed of sound and <span class="hlt">ideal</span>-gas heat capacity of freon R-236ea</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Komarov, S. G.; Gruzdev, V. A.; Stankus, S. V.</p> <p>2008-09-01</p> <p>Speed of sound in the gaseous freon R-236ea with the purity of 99.68 mol. % has been measured by the method of ultrasonic interferometer in the range from 263 to 423 K and at <span class="hlt">pressures</span> from 17 kPA to 4.2 MPa. Errors of temperature, <span class="hlt">pressure</span>, and speed of sound measurement were estimated to be within +/- 20 mK, ± 1.5 kPa, and ±(0.1+0.2) % respectively. Temperature dependence of <span class="hlt">ideal</span>-gas heat capacity of R-236ea has been calculated on the basis of the obtained data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19870007550','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19870007550"><span>Transitional Boundary Layers Under the Influence of High Free Stream Turbulence, Intensive Wall Cooling and High <span class="hlt">Pressure</span> <span class="hlt">Gradients</span> in Hot Gas Circulation. Ph.D. Thesis - Technische Hochschule, Karlsruhe, 1985</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rued, Klaus</p> <p>1987-01-01</p> <p>The requirements for fundamental experimental studies of the influence of free stream turbulence, <span class="hlt">pressure</span> <span class="hlt">gradients</span> and wall cooling are discussed. Under turbine-like free stream conditions, comprehensive tests of transitional boundary layers with laminar, reversing and turbulent flow increments were performed to decouple the effects of the parameters and to determine the effects during mutual interaction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29898823','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29898823"><span><span class="hlt">Ideal</span> cardiovascular health and its association with sedentary behaviour and fitness in psychiatric patients. The PsychiActive project.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bueno-Antequera, J; Oviedo-Caro, M Á; Munguía-Izquierdo, D</p> <p>2018-06-10</p> <p><span class="hlt">Ideal</span> cardiovascular health (CVH) was defined as meeting <span class="hlt">ideal</span> levels of 4 health behaviours (smoking, body mass index, physical activity, and diet) and 3 biological factors (blood <span class="hlt">pressure</span>, total cholesterol, and glucose) and is inversely related to cardiovascular disease and mortality. However, the prevalence of <span class="hlt">ideal</span> CVH in patients with severe mental illness and the possible independent associations of sedentary behaviour and fitness with CVH score are unexplored. This study included 142 (34 women) outpatients with severe mental illness (primarily schizophrenia, n = 92). CVH was evaluated according to the American Heart Association guidelines. Sedentary behaviour, cardiorespiratory fitness, and muscular strength were measured by an activity-monitor, the 6-min walk test, and handgrip dynamometry. Cardiorespiratory fitness and strength values were combined in a composite fitness score. The prevalence of <span class="hlt">ideal</span> CVH was: non-smoking (47.9%), body mass index (16.9), physical activity (83.1%), diet (10.4%), blood <span class="hlt">pressure</span> (40.4%), total cholesterol (62.9%), and plasma glucose (66.7%). Low levels of sedentary behaviour and high cardiorespiratory, strength, and composite fitness score were associated with meeting the <span class="hlt">ideal</span> threshold in most CVH metrics and having higher global CVH score; however, only cardiorespiratory and composite fitness score remained significantly related to global CVH score independent of sedentary behaviour and multiple confounders. Patients with severe mental illness generally have low prevalence of <span class="hlt">ideal</span> CVH metrics, especially diet and body mass index. Additionally, our findings suggest the need or considering cardiorespiratory fitness, regardless of sedentary behaviour, to promote <span class="hlt">ideal</span> CVH in this population. Copyright © 2018 The Italian Society of Diabetology, the Italian Society for the Study of Atherosclerosis, the Italian Society of Human Nutrition, and the Department of Clinical Medicine and Surgery, Federico II University. Published</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_16 --> <div id="page_17" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="321"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800000223&hterms=sensors+pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dsensors%2Bpressure','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800000223&hterms=sensors+pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dsensors%2Bpressure"><span>Downhole <span class="hlt">pressure</span> sensor</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Berdahl, C. M.</p> <p>1980-01-01</p> <p>Sensor remains accurate in spite of varying temperatures. Very accurate, sensitive, and stable downhole <span class="hlt">pressure</span> measurements are needed for vaiety of reservoir engineering applications, such as deep petroleum reservoirs, especially gas reservoirs, and in areas of high geothermal <span class="hlt">gradient</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvE..97a2908E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvE..97a2908E"><span><span class="hlt">Pressure</span> evolution and deformation of confined granular media during pneumatic fracturing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Eriksen, Fredrik K.; Toussaint, Renaud; Turquet, Antoine Léo; Mâløy, Knut J.; Flekkøy, Eirik G.</p> <p>2018-01-01</p> <p>By means of digital image correlation, we experimentally characterize the deformation of a dry granular medium confined inside a Hele-Shaw cell due to air injection at a constant overpressure high enough to deform it (from 50 to 250 kPa). Air injection at these overpressures leads to the formation of so-called pneumatic fractures, i.e., channels empty of beads, and we discuss the typical deformations of the medium surrounding these structures. In addition we simulate the diffusion of the fluid overpressure into the medium, comparing it with the Laplacian solution over time and relating <span class="hlt">pressure</span> <span class="hlt">gradients</span> with corresponding granular displacements. In the compacting medium we show that the diffusing <span class="hlt">pressure</span> field becomes similar to the Laplace solution on the order of a characteristic time given by the properties of the pore fluid, the granular medium, and the system size. However, before the diffusing <span class="hlt">pressure</span> approaches the Laplace solution on the system scale, we find that it resembles the Laplacian field near the channels, with the highest <span class="hlt">pressure</span> <span class="hlt">gradients</span> on the most advanced channel tips and a screened <span class="hlt">pressure</span> <span class="hlt">gradient</span> behind them. We show that the granular displacements more or less always move in the direction against the local <span class="hlt">pressure</span> <span class="hlt">gradients</span>, and when comparing granular velocities with <span class="hlt">pressure</span> <span class="hlt">gradients</span> in the zone ahead of channels, we observe a Bingham type of rheology for the granular paste (the mix of air and beads), with an effective viscosity μB and displacement thresholds ∇ ⃗Pc evolving during mobilization and compaction of the medium. Such a rheology, with disorder in the displacement thresholds, could be responsible for placing the pattern growth at moderate injection <span class="hlt">pressures</span> in a universality class like the dielectric breakdown model with η =2 , where fractal dimensions are found between 1.5 and 1.6 for the patterns.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/977679','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/977679"><span>A low-cost <span class="hlt">gradient</span> system for high-performance liquid chromatography. Quantitation of complex pharmaceutical raw materials.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Erni, F; Frei, R W</p> <p>1976-09-29</p> <p>A device is described that makes use of an eight-port motor valve to generate step <span class="hlt">gradients</span> on the low-<span class="hlt">pressure</span> side of a piston pump with a low dead volume. Such a <span class="hlt">gradient</span> device with an automatic control unit, which also permits repetition of previous steps, can be built for about half the cost of a <span class="hlt">gradient</span> system with two pumps. Applications of this <span class="hlt">gradient</span> unit to the separation of complex mixtures of glycosides and alkaloids are discussed and compared with separations systems using two high-<span class="hlt">pressure</span> pumps. The <span class="hlt">gradients</span> that are used on reversed-phase material with solvent mixtures of water and completely miscible organic solvents are suitable for quantitative routine control of pharmaceutical products. The reproducibility of retention data is excellent over several months and, with the use of loop injectors, major components can be determined quantitatively with a reproducibility of better than 2% (relative standard deviation). The step <span class="hlt">gradient</span> selector valve can also be used as an introduction system for very large sample volumes. Up to 11 can be injected and samples with concentrations of less than 1 ppb can be determined with good reproducibilities.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27435687','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27435687"><span>Monitoring <span class="hlt">gradient</span> profile on-line in micro- and nano-high performance liquid chromatography using conductivity detection.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Min; Chen, Apeng; Lu, Joann J; Cao, Chengxi; Liu, Shaorong</p> <p>2016-08-19</p> <p>In micro- or nano-flow high performance liquid chromatography (HPLC), flow-splitters and <span class="hlt">gradient</span> elutions are commonly used for reverse phase HPLC separations. When a flow splitter was used at a high split-ratio (e.g., 1000:1 or higher), the actual <span class="hlt">gradient</span> may deviate away from the programmed <span class="hlt">gradient</span>. Sometimes, mobile phase concentrations can deviate by as much as 5%. In this work, we noticed that the conductivity (σ) of a <span class="hlt">gradient</span> decreased with the increasing organic-solvent fraction (φ). Based on the relationship between σ and φ, a method was developed for monitoring <span class="hlt">gradient</span> profile on-line to record any deviations in these HPLC systems. The conductivity could be measured by a traditional conductivity detector or a capacitively coupled contactless conductivity detector (C(4)D). The method was applied for assessing the performance of an electroosmotic pump (EOP) based nano-HPLC. We also observed that σ value of the <span class="hlt">gradient</span> changed with system <span class="hlt">pressure</span>; a=0.0175ΔP (R(2)=0.964), where a is the percentage of the conductivity increase and ΔP is the system <span class="hlt">pressure</span> in bar. This effect was also investigated. Copyright © 2016. Published by Elsevier B.V.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4643262','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4643262"><span>Feedback Regulation of Intracellular Hydrostatic <span class="hlt">Pressure</span> in Surface Cells of the Lens</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Gao, Junyuan; Sun, Xiurong; White, Thomas W.; Delamere, Nicholas A.; Mathias, Richard T.</p> <p>2015-01-01</p> <p>In wild-type lenses from various species, an intracellular hydrostatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> goes from ∼340 mmHg in central fiber cells to 0 mmHg in surface cells. This <span class="hlt">gradient</span> drives a center-to-surface flow of intracellular fluid. In lenses in which gap-junction coupling is increased, the central <span class="hlt">pressure</span> is lower, whereas if gap-junction coupling is reduced, the central <span class="hlt">pressure</span> is higher but surface <span class="hlt">pressure</span> is always zero. Recently, we found that surface cell <span class="hlt">pressure</span> was elevated in PTEN null lenses. This suggested disruption of a feedback control system that normally maintained zero surface cell <span class="hlt">pressure</span>. Our purpose in this study was to investigate and characterize this feedback control system. We measured intracellular hydrostatic <span class="hlt">pressures</span> in mouse lenses using a microelectrode/manometer-based system. We found that all feedback went through transport by the Na/K ATPase, which adjusted surface cell osmolarity such that <span class="hlt">pressure</span> was maintained at zero. We traced the regulation of Na/K ATPase activity back to either TRPV4, which sensed positive <span class="hlt">pressure</span> and stimulated activity, or TRPV1, which sensed negative <span class="hlt">pressure</span> and inhibited activity. The inhibitory effect of TRPV1 on Na/K pumps was shown to signal through activation of the PI3K/AKT axis. The stimulatory effect of TRPV4 was shown in previous studies to go through a different signal transduction path. Thus, there is a local two-legged feedback control system for <span class="hlt">pressure</span> in lens surface cells. The surface <span class="hlt">pressure</span> provides a pedestal on which the <span class="hlt">pressure</span> <span class="hlt">gradient</span> sits, so surface <span class="hlt">pressure</span> determines the absolute value of <span class="hlt">pressure</span> at each radial location. We speculate that the absolute value of intracellular <span class="hlt">pressure</span> may set the radial <span class="hlt">gradient</span> in the refractive index, which is essential for visual acuity. PMID:26536260</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvF...3a2601W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvF...3a2601W"><span>Derivation of Zagarola-Smits scaling in zero-<span class="hlt">pressure-gradient</span> turbulent boundary layers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wei, Tie; Maciel, Yvan</p> <p>2018-01-01</p> <p>This Rapid Communication derives the Zagarola-Smits scaling directly from the governing equations for zero-<span class="hlt">pressure-gradient</span> turbulent boundary layers (ZPG TBLs). It has long been observed that the scaling of the mean streamwise velocity in turbulent boundary layer flows differs in the near surface region and in the outer layer. In the inner region of small-velocity-defect boundary layers, it is generally accepted that the proper velocity scale is the friction velocity, uτ, and the proper length scale is the viscous length scale, ν /uτ . In the outer region, the most generally used length scale is the boundary layer thickness, δ . However, there is no consensus on velocity scales in the outer layer. Zagarola and Smits [ASME Paper No. FEDSM98-4950 (1998)] proposed a velocity scale, U ZS=(δ1/δ ) U∞ , where δ1 is the displacement thickness and U∞ is the freestream velocity. However, there are some concerns about Zagarola-Smits scaling due to the lack of a theoretical base. In this paper, the Zagarola-Smits scaling is derived directly from a combination of integral, similarity, and order-of-magnitude analysis of the mean continuity equation. The analysis also reveals that V∞, the mean wall-normal velocity at the edge of the boundary layer, is a proper scale for the mean wall-normal velocity V . Extending the analysis to the streamwise mean momentum equation, we find that the Reynolds shear stress in ZPG TBLs scales as U∞V∞ in the outer region. This paper also provides a detailed analysis of the mass and mean momentum balance in the outer region of ZPG TBLs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28117226','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28117226"><span>Aortoseptal angle and <span class="hlt">pressure</span> <span class="hlt">gradient</span> reduction following balloon valvuloplasty in dogs with severe subaortic stenosis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shen, L; Estrada, A H; Côté, E; Powell, M A; Winter, B; Lamb, K</p> <p>2017-04-01</p> <p>To determine the relationship between aortoseptal angle (AoSA) and the short- and long-term systolic <span class="hlt">pressure</span> <span class="hlt">gradient</span> (PG) reduction following combined cutting and high-<span class="hlt">pressure</span> balloon valvuloplasty (CB/HPBV) in dogs with severe subaortic stenosis. Retrospective study of 22 client-owned dogs of various breeds with severe subaortic stenosis (mean left ventricular to aortic PG = 143 mmHg; range = 80-322 mmHg) that underwent CB/HPBV. Initial angiographic and left apical and right-sided parasternal long-axis view echocardiographic video loops were used for measuring the angle between the plane of the interventricular septum and the longitudinal axis of the ascending aorta. The PG reduction ratio immediately after CB/HPBV and 6 and 12 months later were compared with AoSA. Weak correlations were observed for all instances of PG reduction ratio and AoSA type. Significantly greater mean differences of PG reduction ratio were observed for angles >160° than for angles <160° at 24 h (>160° mean: 54.45, standard error [SE]: ±3.8; <160° mean: 39.88, SE: ±2.09), 6 months (>160° mean: 57.73, SE: ±10.9; <160° mean: 28.22, SE: ±3.42), and 12 months (>160° mean: 76.11, SE: ±17.5; <160° mean: 27.61, SE: ±6.44; p=0.003). Dogs with AoSA >160° on right-sided parasternal long-axis view echocardiograms responded with a greater PG reduction following CB/HPBV than did dogs with AoSA <160°. This suggests that AoSA is associated with long-term outcomes of CB/HPBV, and measurement could help in the evaluation of dogs that are candidates for CB/HPBV. Crown Copyright © 2016. Published by Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhPl...25f2102V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhPl...25f2102V"><span>Diffusion-driven fluid dynamics in <span class="hlt">ideal</span> gases and plasmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vold, E. L.; Yin, L.; Taitano, W.; Molvig, K.; Albright, B. J.</p> <p>2018-06-01</p> <p>The classical transport theory based on Chapman-Enskog methods provides self-consistent approximations for the kinetic flux of mass, heat, and momentum in a fluid limit characterized with a small Knudsen number. The species mass fluxes relative to the center of mass, or "diffusive fluxes," are expressed as functions of known <span class="hlt">gradient</span> quantities with kinetic coefficients evaluated using similar analyses for mixtures of gases or plasma components. The sum over species of the diffusive mass fluxes is constrained to be zero in the Lagrange frame, and thus results in a non-zero molar flux leading to a <span class="hlt">pressure</span> perturbation. At an interface between two species initially in <span class="hlt">pressure</span> equilibrium, the <span class="hlt">pressure</span> perturbation driven by the diffusive molar flux induces a center of mass velocity directed from the species of greater atomic mass towards the lighter atomic mass species. As the ratio of the species particle masses increases, this center of mass velocity carries an increasingly greater portion of the mass across the interface and for a particle mass ratio greater than about two, the center of mass velocity carries more mass than the <span class="hlt">gradient</span> driven diffusion flux. Early time transients across an interface between two species in a 1D plasma regime and initially in equilibrium are compared using three methods; a fluid code with closure in a classical transport approximation, a particle in cell simulation, and an implicit Fokker-Planck solver for the particle distribution functions. The early time transient phenomenology is shown to be similar in each of the computational simulation methods, including a <span class="hlt">pressure</span> perturbation associated with the stationary "induced" component of the center of mass velocity which decays to <span class="hlt">pressure</span> equilibrium during diffusion. At early times, the diffusive process generates <span class="hlt">pressure</span> and velocity waves which propagate outward from the interface and are required to maintain momentum conservation. The energy in the outgoing waves dissipates</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998JChEd..75..587S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998JChEd..75..587S"><span>Is the Reaction Equilibrium Composition in Non-<span class="hlt">ideal</span> Mixtures Uniquely Determined by the Initial Composition?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sefcik, Jan</p> <p>1998-05-01</p> <p>Reaction equilibrium can be mathematically described by the equilibrium equation and the reaction equilibrium composition can be calculated by solving this equation. It can be proved by non-elementary thermodynamic arguments that for a generic system with given initial composition, temperature and <span class="hlt">pressure</span> there is a unique stable equilibrium state corresponding to the global minimum of the Gibbs free energy function. However, when the concept of equilibrium is introduced in undergraduate chemistry and chemical engineering courses, such arguments are generally not accessible. When there is a single reaction equilibrium among mixture components and the components form an <span class="hlt">ideal</span> mixture, it has been demonstrated by a simple, elegant mathematical argument that there is a unique composition satisfying the equilibrium equation. It has been also suggested that this particular argument extends to non-<span class="hlt">ideal</span> mixtures by simply incorporating activity coefficients. We show that the argument extension to non-<span class="hlt">ideal</span> systems is not generally valid. Increasing non-<span class="hlt">ideality</span> can result in non-monotonicity of the function crucial for the simple uniqueness argument, and only later it leads to non-uniqueness and hence phase separation. The main feature responsible for this is a composition dependence of activity coefficients in non-<span class="hlt">ideal</span> mixtures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MeScT..29e4006S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MeScT..29e4006S"><span>Dynamic <span class="hlt">pressure</span> sensitivity determination with Mach number method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sarraf, Christophe; Damion, Jean-Pierre</p> <p>2018-05-01</p> <p>Measurements of <span class="hlt">pressure</span> in fast transient conditions are often performed even if the dynamic characteristic of the transducer are not traceable to international standards. Moreover, the question of a primary standard in dynamic <span class="hlt">pressure</span> is still open, especially for gaseous applications. The question is to improve dynamic standards in order to respond to expressed industrial needs. In this paper, the method proposed in the EMRP IND09 ‘Dynamic’ project, which can be called the ‘<span class="hlt">ideal</span> shock tube method’, is compared with the ‘collective standard method’ currently used in the Laboratoire de Métrologie Dynamique (LNE/ENSAM). The input is a step of <span class="hlt">pressure</span> generated by a shock tube. The transducer is a piezoelectric <span class="hlt">pressure</span> sensor. With the ‘<span class="hlt">ideal</span> shock tube method’ the sensitivity of a <span class="hlt">pressure</span> sensor is first determined dynamically. This method requires a shock tube implemented with piezoelectric shock wave detectors. The measurement of the Mach number in the tube allows an evaluation of the incident <span class="hlt">pressure</span> amplitude of a step using a theoretical 1D model of the shock tube. Heat transfer, other actual effects and effects of the shock tube imperfections are not taken into account. The amplitude of the <span class="hlt">pressure</span> step is then used to determine the sensitivity in dynamic conditions. The second method uses a frequency bandwidth comparison to determine <span class="hlt">pressure</span> at frequencies from quasi-static conditions, traceable to static <span class="hlt">pressure</span> standards, to higher frequencies (up to 10 kHz). The measurand is also a step of <span class="hlt">pressure</span> generated by a supposed <span class="hlt">ideal</span> shock tube or a fast-opening device. The results are provided as a transfer function with an uncertainty budget assigned to a frequency range, also deliverable frequency by frequency. The largest uncertainty in the bandwidth of comparison is used to trace the final <span class="hlt">pressure</span> step level measured in dynamic conditions, owing that this <span class="hlt">pressure</span> is not measurable in a steady state on a shock tube. A reference</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26003622','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26003622"><span>Method transfer from high-<span class="hlt">pressure</span> liquid chromatography to ultra-high-<span class="hlt">pressure</span> liquid chromatography. II. Temperature and <span class="hlt">pressure</span> effects.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Åsberg, Dennis; Samuelsson, Jörgen; Leśko, Marek; Cavazzini, Alberto; Kaczmarski, Krzysztof; Fornstedt, Torgny</p> <p>2015-07-03</p> <p>The importance of the generated temperature and <span class="hlt">pressure</span> <span class="hlt">gradients</span> in ultra-high-<span class="hlt">pressure</span> liquid chromatography (UHPLC) are investigated and compared to high-<span class="hlt">pressure</span> liquid chromatography (HPLC). The drug Omeprazole, together with three other model compounds (with different chemical characteristics, namely uncharged, positively and negatively charged) were used. Calculations of the complete temperature profile in the column at UHPLC conditions showed, in our experiments, a temperature difference between the inlet and outlet of 16 °C and a difference of 2 °C between the column center and the wall. Through van't Hoff plots, this information was used to single out the decrease in retention factor (k) solely due to the temperature <span class="hlt">gradient</span>. The uncharged solute was least affected by temperature with a decrease in k of about 5% while for charged solutes the effect was more pronounced, with k decreases up to 14%. A <span class="hlt">pressure</span> increase of 500 bar gave roughly 5% increase in k for the uncharged solute, while omeprazole and the other two charged solutes gave about 25, 20 and 15% increases in k, respectively. The stochastic model of chromatography was applied to estimate the dependence of the average number of adsorption/desorption events (n) and the average time spent by a molecule in the stationary phase (τs) on temperature and <span class="hlt">pressure</span> on peak shape for the tailing, basic solute. Increasing the temperature yielded an increase in n and decrease in τs which resulted in less skew at high temperatures. With increasing <span class="hlt">pressure</span>, the stochastic modeling gave interesting results for the basic solute showing that the skew of the peak increased with <span class="hlt">pressure</span>. The conclusion is that <span class="hlt">pressure</span> effects are more pronounced for both retention and peak shape than the temperature effects for the polar or charged compounds in our study. Copyright © 2015 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhFl...23g3101A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhFl...23g3101A"><span>The influence of <span class="hlt">pressure</span> relaxation on the structure of an axial vortex</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ash, Robert L.; Zardadkhan, Irfan; Zuckerwar, Allan J.</p> <p>2011-07-01</p> <p>Governing equations including the effects of <span class="hlt">pressure</span> relaxation have been utilized to study an incompressible, steady-state viscous axial vortex with specified far-field circulation. When sound generation is attributed to a velocity <span class="hlt">gradient</span> tensor-<span class="hlt">pressure</span> <span class="hlt">gradient</span> product, the modified conservation of momentum equations that result yield an exact solution for a steady, incompressible axial vortex. The vortex velocity profile has been shown to closely approximate experimental vortex measurements in air and water over a wide range of circulation-based Reynolds numbers. The influence of temperature and humidity on the <span class="hlt">pressure</span> relaxation coefficient in air has been examined using theoretical and empirical approaches, and published axial vortex experiments have been employed to estimate the <span class="hlt">pressure</span> relaxation coefficient in water. Non-equilibrium <span class="hlt">pressure</span> <span class="hlt">gradient</span> forces have been shown to balance the viscous stresses in the vortex core region, and the predicted <span class="hlt">pressure</span> deficits that result from this non-equilibrium balance can be substantially larger than the <span class="hlt">pressure</span> deficits predicted using a Bernoulli equation approach. Previously reported <span class="hlt">pressure</span> deficit distributions for dust devils and tornados have been employed to validate the non-equilibrium <span class="hlt">pressure</span> deficit predictions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/2013/1058/','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/2013/1058/"><span>Regional maps of subsurface geopressure <span class="hlt">gradients</span> of the onshore and offshore Gulf of Mexico basin</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Burke, Lauri A.; Kinney, Scott A.; Dubiel, Russell F.; Pitman, Janet K.</p> <p>2013-01-01</p> <p>The U.S. Geological Survey created a comprehensive geopressure-<span class="hlt">gradient</span> model of the regional <span class="hlt">pressure</span> system spanning the onshore and offshore Gulf of Mexico basin, USA. This model was used to generate ten maps that included (1) five contour maps characterizing the depth to the surface defined by the first occurrence of isopressure <span class="hlt">gradients</span> ranging from 0.60 psi/ft to 1.00 psi/ft, in 0.10-psi/ft increments; and (2) five supporting maps illustrating the spatial density of the data used to construct the contour maps. These contour maps of isopressure-<span class="hlt">gradients</span> at various increments enable the identification and quantification of the occurrence, magnitude, location, and depth of the subsurface <span class="hlt">pressure</span> system, which allows for the broad characterization of regions exhibiting overpressured, underpressured, and normally <span class="hlt">pressured</span> strata. Identification of overpressured regions is critical for exploration and evaluation of potential undiscovered hydrocarbon accumulations based on petroleum-generation <span class="hlt">pressure</span> signatures and <span class="hlt">pressure</span>-retention properties of reservoir seals. Characterization of normally <span class="hlt">pressured</span> regions is essential for field development decisions such as determining the dominant production drive mechanisms, evaluating well placement and drainage patterns, and deciding on well stimulation methods such as hydraulic fracturing. Identification of underpressured regions is essential for evaluating the feasibility of geological sequestration and long-term containment of fluids such as supercritical carbon dioxide for alternative disposal methods of greenhouse gases. This study is the first, quantitative investigation of the regional <span class="hlt">pressure</span> systems of one of the most important petroleum provinces in the United States. Although this methodology was developed for <span class="hlt">pressure</span> studies in the Gulf of Mexico basin, it is applicable to any basin worldwide.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JEMat..46.5136M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JEMat..46.5136M"><span>Thermoelectric Generation Using Counter-Flows of <span class="hlt">Ideal</span> Fluids</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Meng, Xiangning; Lu, Baiyi; Zhu, Miaoyong; Suzuki, Ryosuke O.</p> <p>2017-08-01</p> <p>Thermoelectric (TE) performance of a three-dimensional (3-D) TE module is examined by exposing it between a pair of counter-flows of <span class="hlt">ideal</span> fluids. The <span class="hlt">ideal</span> fluids are thermal sources of TE module flow in the opposite direction at the same flow rate and generate temperature differences on the hot and cold surfaces due to their different temperatures at the channel inlet. TE performance caused by different inlet temperatures of thermal fluids are numerically analyzed by using the finite-volume method on 3-D meshed physical models and then compared with those using a constant boundary temperature. The results show that voltage and current of the TE module increase gradually from a beginning moment to a steady flow and reach a stable value. The stable values increase with inlet temperature of the hot fluid when the inlet temperature of cold fluid is fixed. However, the time to get to the stable values is almost consistent for all the temperature differences. Moreover, the trend of TE performance using a fluid flow boundary is similar to that of using a constant boundary temperature. Furthermore, 3-D contours of fluid <span class="hlt">pressure</span>, temperature, enthalpy, electromotive force, current density and heat flux are exhibited in order to clarify the influence of counter-flows of <span class="hlt">ideal</span> fluids on TE generation. The current density and heat flux homogeneously distribute on an entire TE module, thus indicating that the counter-flows of thermal fluids have high potential to bring about fine performance for TE modules.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020075595&hterms=supercritical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dsupercritical','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020075595&hterms=supercritical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dsupercritical"><span>Aspects of Supercritical Turbulence: Direct Numerical Simulation of O2/H2 and C7H16/N2 Temporal Mixing Layers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bellan, J.; Okongo, N. A.; Harstad, K. G.; Hutt, John (Technical Monitor)</p> <p>2002-01-01</p> <p>Results from Direct Numerical Simulations of temporal, supercritical mixing layers for two species systems are analyzed to elucidate species-specific turbulence aspects. The two species systems, O2/H2 and C7HG16/N2, have different thermodynamic characteristics; thus, although the simulations are performed at similar reduced <span class="hlt">pressure</span> (ratio of the <span class="hlt">pressure</span> to the critical <span class="hlt">pressure</span>), the former system is dose to mixture <span class="hlt">ideality</span> and has a relatively high solubility with respect to the latter, which exhibits strong departures from mixture <span class="hlt">ideality</span> Due to the specified, smaller initial density stratification, the C7H16/N2 layers display higher growth and increased global molecular mixing as well as larger turbulence levels. However, smaller density <span class="hlt">gradients</span> at the transitional state for the O2/H2 system indicate that on a local basis, the layer exhibits an enhanced mixing, this being attributed to the increased solubility and to mixture <span class="hlt">ideality</span>. These thermodynamic features are shown to affect the irreversible entropy production (i.e. the dissipation), which is larger for the O2/H2 layer and is primarily concentrated in high density-<span class="hlt">gradient</span> magnitude regions that are distortions of the initial density stratification boundary. In contrast, the regions of largest dissipation in the C7H16/N2 layer are located in high density-<span class="hlt">gradient</span> magnitude regions resulting from the mixing of the two fluids.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19800009140','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19800009140"><span>First results of a study on turbulent boundary layers in oscillating flow with a mean adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Houdeville, R.; Cousteix, J.</p> <p>1979-01-01</p> <p>The development of a turbulent unsteady boundary layer with a mean <span class="hlt">pressure</span> <span class="hlt">gradient</span> strong enough to induce separation, in order to complete the extend results obtained for the flat plate configuration is presented. The longitudinal component of the velocity is measured using constant temperature hot wire anemometer. The region where negative velocities exist is investigated with a laser Doppler velocimeter system with BRAGG cells. The boundary layer responds by forced pulsation to the perturbation of potential flow. The unsteady effects observed are very important. The average location of the zero skin friction point moves periodically at the perturbation frequency. Average velocity profiles from different instants in the cycle are compared. The existence of a logarithmic region enables a simple calculation of the maximum phase shift of the velocity in the boundary layer. An attempt of calculation by an integral method of boundary layer development is presented, up to the point where reverse flow starts appearing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21270474','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21270474"><span>From the <span class="hlt">ideal</span> market to the <span class="hlt">ideal</span> clinic: constructing a normative standard of fairness for human subjects research.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Phillips, Trisha</p> <p>2011-02-01</p> <p>Preventing exploitation in human subjects research requires a benchmark of fairness against which to judge the distribution of the benefits and burdens of a trial. This paper proposes the <span class="hlt">ideal</span> market and its fair market price as a criterion of fairness. The <span class="hlt">ideal</span> market approach is not new to discussions about exploitation, so this paper reviews Wertheimer's inchoate presentation of the <span class="hlt">ideal</span> market as a principle of fairness, attempt of Emanuel and colleagues to apply the <span class="hlt">ideal</span> market to human subjects research, and Ballantyne's criticisms of both the <span class="hlt">ideal</span> market and the resulting benchmark of fairness. It argues that the criticism of this particular benchmark is on point, but the rejection of the <span class="hlt">ideal</span> market is mistaken. After presenting a complete account of the <span class="hlt">ideal</span> market, this paper proposes a new method for applying the <span class="hlt">ideal</span> market to human subjects research and illustrates the proposal by considering a sample case.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15178302','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15178302"><span>An analysis of induced <span class="hlt">pressure</span> fields in electroosmotic flows through microchannels.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Yonghao; Gu, Xiao-Jun; Barber, Robert W; Emerson, David R</p> <p>2004-07-15</p> <p>Induced <span class="hlt">pressure</span> <span class="hlt">gradients</span> are found to cause band-broadening effects which are important to the performance of microfluidic devices, such as capillary electrophoresis and capillary chromatography. An improved understanding of the underlying mechanisms causing an induced <span class="hlt">pressure</span> <span class="hlt">gradient</span> in electroosmotic flows is presented. The analysis shows that the induced <span class="hlt">pressure</span> distribution is the key to understanding the experimentally observed phenomena of leakage flows. A novel way of determining the static <span class="hlt">pressures</span> at the inlet and outlet of microchannels is also presented that takes account of the <span class="hlt">pressure</span> losses due to flow contraction and expansion. These commonly neglected <span class="hlt">pressure</span> losses at the channel entrance and outlet are shown to be important in accurately describing the flow. The important parameters that define the effect of induced <span class="hlt">pressure</span> on the flows are discussed, which may facilitate the design of improved microfluidic devices. The present model clearly identifies the mechanism behind the experimentally observed leakage flows, which is further confirmed by numerical simulations. Not only can the leakage flow occur from the electric-field-free side channel to the main channel, but also the fluid in the main channel can be attracted into the side channel by the induced <span class="hlt">pressure</span> <span class="hlt">gradient</span>. Copyright 2004 Elsevier Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21347153-edge-localized-linear-ideal-magnetohydrodynamic-instability-studies-extended-magnetohydrodynamic-code','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21347153-edge-localized-linear-ideal-magnetohydrodynamic-instability-studies-extended-magnetohydrodynamic-code"><span>Edge localized linear <span class="hlt">ideal</span> magnetohydrodynamic instability studies in an extended-magnetohydrodynamic code</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Burke, B. J.; Kruger, S. E.; Hegna, C. C.</p> <p></p> <p>A linear benchmark between the linear <span class="hlt">ideal</span> MHD stability codes ELITE [H. R. Wilson et al., Phys. Plasmas 9, 1277 (2002)], GATO [L. Bernard et al., Comput. Phys. Commun. 24, 377 (1981)], and the extended nonlinear magnetohydrodynamic (MHD) code, NIMROD [C. R. Sovinec et al.., J. Comput. Phys. 195, 355 (2004)] is undertaken for edge-localized (MHD) instabilities. Two ballooning-unstable, shifted-circle tokamak equilibria are compared where the stability characteristics are varied by changing the equilibrium plasma profiles. The equilibria model an H-mode plasma with a pedestal <span class="hlt">pressure</span> profile and parallel edge currents. For both equilibria, NIMROD accurately reproduces the transition tomore » instability (the marginally unstable mode), as well as the <span class="hlt">ideal</span> growth spectrum for a large range of toroidal modes (n=1-20). The results use the compressible MHD model and depend on a precise representation of '<span class="hlt">ideal</span>-like' and 'vacuumlike' or 'halo' regions within the code. The halo region is modeled by the introduction of a Lundquist-value profile that transitions from a large to a small value at a flux surface location outside of the pedestal region. To model an <span class="hlt">ideal</span>-like MHD response in the core and a vacuumlike response outside the transition, separate criteria on the plasma and halo Lundquist values are required. For the benchmarked equilibria the critical Lundquist values are 10{sup 8} and 10{sup 3} for the <span class="hlt">ideal</span>-like and halo regions, respectively. Notably, this gives a ratio on the order of 10{sup 5}, which is much larger than experimentally measured values using T{sub e} values associated with the top of the pedestal and separatrix. Excellent agreement with ELITE and GATO calculations are made when sharp boundary transitions in the resistivity are used and a small amount of physical dissipation is added for conditions very near and below marginal <span class="hlt">ideal</span> stability.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4838189','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4838189"><span><span class="hlt">Ideals</span> as Anchors for Relationship Experiences</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Frye, Margaret; Trinitapoli, Jenny</p> <p>2016-01-01</p> <p>Research on young-adult sexuality in sub-Saharan Africa typically conceptualizes sex as an individual-level risk behavior. We introduce a new approach that connects the conditions surrounding the initiation of sex with subsequent relationship well-being, examines relationships as sequences of interdependent events, and indexes relationship experiences to individually held <span class="hlt">ideals</span>. New card-sort data from southern Malawi capture young women’s relationship experiences and their <span class="hlt">ideals</span> in a sequential framework. Using optimal matching, we measure the distance between <span class="hlt">ideal</span> and experienced relationship sequences to (1) assess the associations between ideological congruence and perceived relationship well-being, (2) compare this <span class="hlt">ideal</span>-based approach to other experience-based alternatives, and (3) identify individual- and couple-level correlates of congruence between <span class="hlt">ideals</span> and experiences in the romantic realm. We show that congruence between <span class="hlt">ideals</span> and experiences conveys relationship well-being along four dimensions: expressions of love and support, robust communication habits, perceived biological safety, and perceived relationship stability. We further show that congruence is patterned by socioeconomic status and supported by shared <span class="hlt">ideals</span> within romantic dyads. We argue that conceiving of <span class="hlt">ideals</span> as anchors for how sexual experiences are manifest advances current understandings of romantic relationships, and we suggest that this approach has applications for other domains of life. PMID:27110031</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_17 --> <div id="page_18" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="341"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=tree+AND+b&pg=2&id=EJ945332','ERIC'); return false;" href="https://eric.ed.gov/?q=tree+AND+b&pg=2&id=EJ945332"><span><span class="hlt">Ideals</span> and Category Typicality</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Kim, ShinWoo; Murphy, Gregory L.</p> <p>2011-01-01</p> <p>Barsalou (1985) argued that exemplars that serve category goals become more typical category members. Although this claim has received support, we investigated (a) whether categories have a single <span class="hlt">ideal</span>, as negatively valenced categories (e.g., cigarette) often have conflicting goals, and (b) whether <span class="hlt">ideal</span> items are in fact typical, as they often…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JMoSt1125..350E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JMoSt1125..350E"><span>First-principles study of the structural, elastic, vibrational, thermodynamic and electronic properties of the Mo2B intermetallic under <span class="hlt">pressure</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Escamilla, R.; Carvajal, E.; Cruz-Irisson, M.; Romero, M.; Gómez, R.; Marquina, V.; Galván, D. H.; Durán, A.</p> <p>2016-12-01</p> <p>The structural, elastic, vibrational, thermodynamic and electronic properties of the Mo2B intermetallic under <span class="hlt">pressure</span> are assessed using first-principles calculations based on the generalized <span class="hlt">gradient</span> approximation (GGA) proposed by Perdew-Wang (PW91). Our results show that the calculated structural parameters at a <span class="hlt">pressure</span> of zero GPa are in good agreement with the available experimental data. The effect of high <span class="hlt">pressures</span> on the lattice constants shows that the compression along the c-axis and along the a-axis are similar. The elastic constants were calculated using the static finite strain technique, and the bulk shear moduli are derived from the <span class="hlt">ideal</span> polycrystalline aggregate. We find that the elastic constants, elastic modulus and hardness monotonically increase as a function of <span class="hlt">pressure</span>; consequently, the structure is dynamically stable and tends from brittle to ductile behavior under <span class="hlt">pressure</span>. The Debye temperature θD increases and the so-called Gru¨ neisen constant γ decreases due to stiffening of the crystal structure. The phonon dispersion curves were obtained using the direct method. Additionally, the internal energy (ΔE), the Helmholtz free energy (ΔF), the entropy (S) and the lattice contribution to the heat capacity Cv were calculated and analyzed with the help of the phonon dispersion curves. The N(EF) and the electron transfer between the B and Mo atoms increase as a function of <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20129845','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20129845"><span><span class="hlt">Ideal</span> AFROC and FROC observers.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Khurd, Parmeshwar; Liu, Bin; Gindi, Gene</p> <p>2010-02-01</p> <p>Detection of multiple lesions in images is a medically important task and free-response receiver operating characteristic (FROC) analyses and its variants, such as alternative FROC (AFROC) analyses, are commonly used to quantify performance in such tasks. However, <span class="hlt">ideal</span> observers that optimize FROC or AFROC performance metrics have not yet been formulated in the general case. If available, such <span class="hlt">ideal</span> observers may turn out to be valuable for imaging system optimization and in the design of computer aided diagnosis techniques for lesion detection in medical images. In this paper, we derive <span class="hlt">ideal</span> AFROC and FROC observers. They are <span class="hlt">ideal</span> in that they maximize, amongst all decision strategies, the area, or any partial area, under the associated AFROC or FROC curve. Calculation of observer performance for these <span class="hlt">ideal</span> observers is computationally quite complex. We can reduce this complexity by considering forms of these observers that use false positive reports derived from signal-absent images only. We also consider a Bayes risk analysis for the multiple-signal detection task with an appropriate definition of costs. A general decision strategy that minimizes Bayes risk is derived. With particular cost constraints, this general decision strategy reduces to the decision strategy associated with the <span class="hlt">ideal</span> AFROC or FROC observer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22590584-acoustic-beam-control-biomimetic-projector-via-velocity-gradient','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22590584-acoustic-beam-control-biomimetic-projector-via-velocity-gradient"><span>Acoustic beam control in biomimetic projector via velocity <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Gao, Xiaowei; Dong, Erqian; Song, Zhongchang</p> <p></p> <p>A biomimetic projector (BioP) based on computerized tomography of pygmy sperm whale's biosonar system has been designed using <span class="hlt">gradient</span>-index (GRIN) material. The directivity of this BioP device was investigated as function of frequency and the velocity <span class="hlt">gradient</span> of the GRIN material. A strong beam control over a broad bandwidth at the subwavelength scale has been achieved. Compared with a bare subwavelength source, the main lobe <span class="hlt">pressure</span> of the BioP is about five times as high and the angular resolution is one order of magnitude better. Our results indicate that this BioP has excellent application potential in miniaturized underwater sonars.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ApPhL.109a3505G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ApPhL.109a3505G"><span>Acoustic beam control in biomimetic projector via velocity <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gao, Xiaowei; Zhang, Yu; Cao, Wenwu; Dong, Erqian; Song, Zhongchang; Li, Songhai; Tang, Liguo; Zhang, Sai</p> <p>2016-07-01</p> <p>A biomimetic projector (BioP) based on computerized tomography of pygmy sperm whale's biosonar system has been designed using <span class="hlt">gradient</span>-index (GRIN) material. The directivity of this BioP device was investigated as function of frequency and the velocity <span class="hlt">gradient</span> of the GRIN material. A strong beam control over a broad bandwidth at the subwavelength scale has been achieved. Compared with a bare subwavelength source, the main lobe <span class="hlt">pressure</span> of the BioP is about five times as high and the angular resolution is one order of magnitude better. Our results indicate that this BioP has excellent application potential in miniaturized underwater sonars.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120001337','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120001337"><span>Asymmetric Uncertainty Expression for High <span class="hlt">Gradient</span> Aerodynamics</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pinier, Jeremy T</p> <p>2012-01-01</p> <p>When the physics of the flow around an aircraft changes very abruptly either in time or space (e.g., flow separation/reattachment, boundary layer transition, unsteadiness, shocks, etc), the measurements that are performed in a simulated environment like a wind tunnel test or a computational simulation will most likely incorrectly predict the exact location of where (or when) the change in physics happens. There are many reasons for this, includ- ing the error introduced by simulating a real system at a smaller scale and at non-<span class="hlt">ideal</span> conditions, or the error due to turbulence models in a computational simulation. The un- certainty analysis principles that have been developed and are being implemented today do not fully account for uncertainty in the knowledge of the location of abrupt physics changes or sharp <span class="hlt">gradients</span>, leading to a potentially underestimated uncertainty in those areas. To address this problem, a new asymmetric aerodynamic uncertainty expression containing an extra term to account for a phase-uncertainty, the magnitude of which is emphasized in the high-<span class="hlt">gradient</span> aerodynamic regions is proposed in this paper. Additionally, based on previous work, a method for dispersing aerodynamic data within asymmetric uncer- tainty bounds in a more realistic way has been developed for use within Monte Carlo-type analyses.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15138658','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15138658"><span>[Resistance to <span class="hlt">pressure</span> of bronchial closures. Comparison of <span class="hlt">pressure</span> resistance of manual and stapler bronchial closures depending on the angle to the cartilaginous rings].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ludwig, C; Behrend, M; Hoffarth, U; Schüttler, W; Stoelben, E</p> <p>2004-09-01</p> <p>This study was aimed to determine the resistance to <span class="hlt">pressure</span> of manual and stapled bronchial closures under <span class="hlt">ideal</span> conditions (90 degrees to the bronchial tree) and parallel to the trachea (45 degrees). An experimental study was done on 60 explanted pig tracheae which were alternatively closed with either double-layer, running sutures angled 90 degrees to the cartilaginous rings or an automatic stapling device. The closure line was placed exactly 90 degrees to the bronchial tree in 30 cases and parallel to the trachea (45 degrees) in 30. The sutures were placed under <span class="hlt">pressure</span> until air leakage was observed. The leakage <span class="hlt">pressure</span> was digitally recorded. A statistically significant difference existed between the two groups. Mechanical sutures proved more resistant to <span class="hlt">pressure</span> (P=0.011). Under <span class="hlt">ideal</span> conditions, the resistance to <span class="hlt">pressure</span> of mechanical sutures is equal to if not better than that of manual sutures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGeod.tmp...24L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGeod.tmp...24L"><span>Refined discrete and empirical horizontal <span class="hlt">gradients</span> in VLBI analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Landskron, Daniel; Böhm, Johannes</p> <p>2018-02-01</p> <p>Missing or incorrect consideration of azimuthal asymmetry of troposphere delays is a considerable error source in space geodetic techniques such as Global Navigation Satellite Systems (GNSS) or Very Long Baseline Interferometry (VLBI). So-called horizontal troposphere <span class="hlt">gradients</span> are generally utilized for modeling such azimuthal variations and are particularly required for observations at low elevation angles. Apart from estimating the <span class="hlt">gradients</span> within the data analysis, which has become common practice in space geodetic techniques, there is also the possibility to determine the <span class="hlt">gradients</span> beforehand from different data sources than the actual observations. Using ray-tracing through Numerical Weather Models (NWMs), we determined discrete <span class="hlt">gradient</span> values referred to as GRAD for VLBI observations, based on the standard <span class="hlt">gradient</span> model by Chen and Herring (J Geophys Res 102(B9):20489-20502, 1997. https://doi.org/10.1029/97JB01739) and also for new, higher-order <span class="hlt">gradient</span> models. These <span class="hlt">gradients</span> are produced on the same data basis as the Vienna Mapping Functions 3 (VMF3) (Landskron and Böhm in J Geod, 2017.https://doi.org/10.1007/s00190-017-1066-2), so they can also be regarded as the VMF3 <span class="hlt">gradients</span> as they are fully consistent with each other. From VLBI analyses of the Vienna VLBI and Satellite Software (VieVS), it becomes evident that baseline length repeatabilities (BLRs) are improved on average by 5% when using a priori <span class="hlt">gradients</span> GRAD instead of estimating the <span class="hlt">gradients</span>. The reason for this improvement is that the <span class="hlt">gradient</span> estimation yields poor results for VLBI sessions with a small number of observations, while the GRAD a priori <span class="hlt">gradients</span> are unaffected from this. We also developed a new empirical <span class="hlt">gradient</span> model applicable for any time and location on Earth, which is included in the Global <span class="hlt">Pressure</span> and Temperature 3 (GPT3) model. Although being able to describe only the systematic component of azimuthal asymmetry and no short-term variations at all, even these</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26518496','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26518496"><span>Simple equations to simulate closed-loop recycling liquid-liquid chromatography: <span class="hlt">Ideal</span> and non-<span class="hlt">ideal</span> recycling models.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kostanyan, Artak E</p> <p>2015-12-04</p> <p>The <span class="hlt">ideal</span> (the column outlet is directly connected to the column inlet) and non-<span class="hlt">ideal</span> (includes the effects of extra-column dispersion) recycling equilibrium-cell models are used to simulate closed-loop recycling counter-current chromatography (CLR CCC). Simple chromatogram equations for the individual cycles and equations describing the transport and broadening of single peaks and complex chromatograms inside the recycling closed-loop column for <span class="hlt">ideal</span> and non-<span class="hlt">ideal</span> recycling models are presented. The extra-column dispersion is included in the theoretical analysis, by replacing the recycling system (connecting lines, pump and valving) by a cascade of Nec perfectly mixed cells. To evaluate extra-column contribution to band broadening, two limiting regimes of recycling are analyzed: plug-flow, Nec→∞, and maximum extra-column dispersion, Nec=1. Comparative analysis of <span class="hlt">ideal</span> and non-<span class="hlt">ideal</span> models has shown that when the volume of the recycling system is less than one percent of the column volume, the influence of the extra-column processes on the CLR CCC separation may be neglected. Copyright © 2015 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29510468','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29510468"><span>Using geometric morphometric visualizations of directional selection <span class="hlt">gradients</span> to investigate morphological differentiation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Weaver, Timothy D; Gunz, Philipp</p> <p>2018-04-01</p> <p>Researchers studying extant and extinct taxa are often interested in identifying the evolutionary processes that have lead to the morphological differences among the taxa. <span class="hlt">Ideally</span>, one could distinguish the influences of neutral evolutionary processes (genetic drift, mutation) from natural selection, and in situations for which selection is implicated, identify the targets of selection. The directional selection <span class="hlt">gradient</span> is an effective tool for investigating evolutionary process, because it can relate form (size and shape) differences between taxa to the variation and covariation found within taxa. However, although most modern morphometric analyses use the tools of geometric morphometrics (GM) to analyze landmark data, to date, selection <span class="hlt">gradients</span> have mainly been calculated from linear measurements. To address this methodological gap, here we present a GM approach for visualizing and comparing between-taxon selection <span class="hlt">gradients</span> with each other, associated difference vectors, and "selection" <span class="hlt">gradients</span> from neutral simulations. To exemplify our approach, we use a dataset of 347 three-dimensional landmarks and semilandmarks recorded on the crania of 260 primate specimens (112 humans, 67 common chimpanzees, 36 bonobos, 45 gorillas). Results on this example dataset show how incorporating geometric information can provide important insights into the evolution of the human braincase, and serve to demonstrate the utility of our approach for understanding morphological evolution. © 2018 The Author(s). Evolution © 2018 The Society for the Study of Evolution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23988512','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23988512"><span>Adoption of American Heart Association 2020 <span class="hlt">ideal</span> healthy diet recommendations prevents weight gain in young adults.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Forget, Geneviève; Doyon, Myriam; Lacerte, Guillaume; Labonté, Mélissa; Brown, Christine; Carpentier, André C; Langlois, Marie-France; Hivert, Marie-France</p> <p>2013-11-01</p> <p>In 2010, the American Heart Association established the concept of <span class="hlt">ideal</span> cardiovascular health. Nationally representative data estimated that <1% of Americans meet the seven health metrics required for achieving <span class="hlt">ideal</span> cardiovascular health, with the main challenge residing in meeting the criteria for an <span class="hlt">ideal</span> Healthy Diet Score. In a cohort of young adults (N=196), we aimed to investigate the prevalence of <span class="hlt">ideal</span> cardiovascular health and <span class="hlt">ideal</span> Healthy Diet Score and its association to weight gain over a 4-year follow-up period. Anthropometric measures, blood <span class="hlt">pressure</span>, and blood samples were taken according to standardized procedures. Dietary intake was measured by a 3-day food diary and verified by a registered dietitian. We observed that only 0.5% of our sample met the criteria for <span class="hlt">ideal</span> cardiovascular health and only 4.1% met the criteria for an <span class="hlt">ideal</span> Healthy Diet Score. The components of the Healthy Diet Score with the lowest observance were consumption of fruits and vegetables (9.7%) and whole grains (14.8%). Meeting zero or one out of five of the Healthy Diet Score components was associated with increased risk of weight gain over 4 years compared with meeting at least two components (P=0.03). With the exception of dietary criteria, prevalence was high for achieving <span class="hlt">ideal</span> levels of the remaining six cardiovascular health metrics. In conclusion, in this sample of young adults, a very low prevalence of <span class="hlt">ideal</span> overall cardiovascular health was observed, mainly driven by poor dietary habits, and a poor Healthy Diet Score was associated with increased weight gain. Copyright © 2013 Academy of Nutrition and Dietetics. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003JChPh.119.1897T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003JChPh.119.1897T"><span><span class="hlt">Ideal</span> glass transitions in thin films: An energy landscape perspective</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Truskett, Thomas M.; Ganesan, Venkat</p> <p>2003-07-01</p> <p>We introduce a mean-field model for the potential energy landscape of a thin fluid film confined between parallel substrates. The model predicts how the number of accessible basins on the energy landscape and, consequently, the film's <span class="hlt">ideal</span> glass transition temperature depend on bulk <span class="hlt">pressure</span>, film thickness, and the strength of the fluid-fluid and fluid-substrate interactions. The predictions are in qualitative agreement with the experimental trends for the kinetic glass transition temperature of thin films, suggesting the utility of landscape-based approaches for studying the behavior of confined fluids.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1375953-pattern-parallel-edge-plasma-flows-due-pressure-gradients-recycling-resonant-magnetic-perturbations-diii','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1375953-pattern-parallel-edge-plasma-flows-due-pressure-gradients-recycling-resonant-magnetic-perturbations-diii"><span>The pattern of parallel edge plasma flows due to <span class="hlt">pressure</span> <span class="hlt">gradients</span>, recycling, and resonant magnetic perturbations in DIII-D</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Frerichs, H.; Schmitz, Oliver; Evans, Todd; ...</p> <p>2015-07-13</p> <p>High resolution plasma transport simulations with the EMC3-EIRENE code have been performed to address the parallel plasma flow structure in the boundary of a poloidal divertor configuration with non-axisymmetric perturbations at DIII-D. Simulation results show that a checkerboard pattern of flows with alternating direction is generated inside the separatrix. This pattern is aligned with the position of the main resonances (i.e. where the safety factor is equal to rational values q = m/n for a perturbation field with base mode number n): m pairs of alternating forward and backward flow channel exist for each resonance. The poloidal oscillations are alignedmore » with the subharmonic Melnikov function, which indicates that the plasma flow is generated by parallel <span class="hlt">pressure</span> <span class="hlt">gradients</span> along perturbed field lines. Lastly, an additional scrape-off layer-like domain is introduced by the perturbed separatrix which guides field lines from the interior to the divertor targets, resulting in an enhanced outward flow that is consistent with the experimentally observed particle pump-out effect. However, while the lobe structure of the perturbed separatrix is very well reflected in the temperature profile, the same lobes can appear to be smaller in the flow profile due to a competition between high upstream <span class="hlt">pressure</span> and downstream particle sources driving flows in opposite directions.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/EJ795292.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/EJ795292.pdf"><span>Teaching with Vision: How One Teacher Negotiates the Tension between High <span class="hlt">Ideals</span> and Standardized Testing</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Hammerness, Karen</p> <p>2004-01-01</p> <p>These are challenging times for teachers. Mixed messages, conflicting demands, and increasing needs on all fronts surround them. Each day, teachers face increasing requirements and significant <span class="hlt">pressures</span> on their daily practice from administrators and policymakers. It is hard to be, or remain, a teacher of quality committed to one's <span class="hlt">ideals</span>. In this…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ShWav..28..765S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ShWav..28..765S"><span>Supersonic flow <span class="hlt">gradients</span> at an overexpanded nozzle lip</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Silnikov, M. V.; Chernyshov, M. V.</p> <p>2018-07-01</p> <p>The flowfield of a planar, overexpanded jet flow and an axisymmetric one are analyzed theoretically for a wide range of governing flow parameters (such as the nozzle divergence angle, the initial flow Mach number, the jet expansion ratio, and the ratio of specific heats). Significant differences are discovered between these parameters of the incident shock and the downstream flow for a planar jet and for an axisymmetric overexpanded jet flow. Incident shock curvature, shock strength variation, the geometrical curvature of the jet boundary, <span class="hlt">gradients</span> of total and static <span class="hlt">pressure</span> and Mach number, and flow vorticity parameters in post-shock flow are studied theoretically for non-separated nozzle flows. Flow parameters indicating zero and extrema values of these <span class="hlt">gradients</span> are reported. Some theoretical results (such as concavities of incident shock and jet boundary, local decreases in the incident shock strength, increases and decreases in the static <span class="hlt">pressure</span>, and the Mach number downstream of the incident shock) seem rather specific and non-evident at first sight. The theoretical results, achieved while using an inviscid flow model, are compared and confirmed with experimental data obtained by other authors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhCS.991a2053L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS.991a2053L"><span>A stationary bulk planar <span class="hlt">ideal</span> flow solution for the double shearing model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lyamina, E. A.; Kalenova, N. V.; Date, P. P.</p> <p>2018-04-01</p> <p>This paper provides a general <span class="hlt">ideal</span> flow solution for the double shearing model of <span class="hlt">pressure</span>-dependent plasticity. This new solution is restricted to a special class of stationary planar flows. A distinguished feature of this class of solutions is that one family of characteristic lines is straight. The solution is analytic. The mapping between Cartesian and principal lines based coordinate systems is given in parametric form with characteristic coordinates being the parameters. A simple relation that connects the scale factor for one family of coordinate curves of the principal lines based coordinate system and the magnitude of velocity is derived. The original <span class="hlt">ideal</span> flow theory is widely used as the basis for inverse methods for the preliminary design of metal forming processes driven by minimum plastic work. The new theory extends this area of application to granular materials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11270555','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11270555"><span>A spinal thecal sac constriction model supports the theory that induced <span class="hlt">pressure</span> <span class="hlt">gradients</span> in the cord cause edema and cyst formation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Josephson, A; Greitz, D; Klason, T; Olson, L; Spenger, C</p> <p>2001-03-01</p> <p>Spinal cord cysts are a devastating condition that occur secondary to obstructions of the spinal canal, which may be caused by congenital malformations, trauma, spinal canal stenosis, tumors, meningitis, or arachnoiditis. A hypothesis that could explain how spinal cord cysts form in these situations has been presented recently. Therefore, a novel spinal thecal sac constriction model was implemented to test various aspects of this hypothesis. Thecal sac constriction was achieved by subjecting rats to an extradural silk ligature at the T8 spinal cord level. Rats with complete spinal cord transection served as a second model for comparison. The animals underwent high-resolution magnetic resonance imaging and histological analysis. Thecal sac constriction caused edema cranial and caudal to the ligation within 3 weeks, and cysts developed after 8 to 13 weeks. In contrast, cysts in rats with spinal cord transection were located predominantly in the cranial spinal cord. Histological sections of spinal cords confirmed the magnetic resonance imaging results. Magnetic resonance imaging provided the specific advantage of enabling characterization of events as they occurred repeatedly over time in the spinal cords of individual living animals. The spinal thecal sac constriction model proved useful for investigation of features of the cerebrospinal fluid pulse <span class="hlt">pressure</span> theory. Edema and cyst distributions were in accordance with this theory. We conclude that induced intramedullary <span class="hlt">pressure</span> <span class="hlt">gradients</span> originating from the cerebrospinal fluid pulse <span class="hlt">pressure</span> may underlie cyst formation in the vicinity of spinal canal obstructions and that cysts are preceded by edema.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11568078','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11568078"><span>Relationship between early diastolic intraventricular <span class="hlt">pressure</span> <span class="hlt">gradients</span>, an index of elastic recoil, and improvements in systolic and diastolic function.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Firstenberg, M S; Smedira, N G; Greenberg, N L; Prior, D L; McCarthy, P M; Garcia, M J; Thomas, J D</p> <p>2001-09-18</p> <p>Early diastolic intraventricular <span class="hlt">pressure</span> <span class="hlt">gradients</span> (IVPGs) have been proposed to relate to left ventricular (LV) elastic recoil and early ventricular "suction." Animal studies have demonstrated relationships between IVPGs and systolic and diastolic indices during acute ischemia. However, data on the effects of improvements in LV function in humans and the relationship to IVPGs are lacking. Eight patients undergoing CABG and/or infarct exclusion surgery had a triple-sensor high-fidelity catheter placed across the mitral valve intraoperatively for simultaneous recording of left atrial (LA), basal LV, and apical LV <span class="hlt">pressures</span>. Hemodynamic data obtained before bypass were compared with those with similar LA <span class="hlt">pressures</span> and heart rates obtained after bypass. From each LV waveform, the time constant of LV relaxation (tau), +dP/dt(max), and -dP/dt(max) were determined. Transesophageal echocardiography was used to determined end-diastolic (EDV) and end-systolic (ESV) volumes and ejection fractions (EF). At similar LA <span class="hlt">pressures</span> and heart rates, IVPG increased after bypass (before bypass 1.64+/-0.79 mm Hg; after bypass 2.67+/-1.25 mm Hg; P<0.01). Significant improvements were observed in ESV, as well as in apical and basal +dP/dt(max), -dP/dt(max), and tau (each P<0.05). Overall, IVPGs correlated inversely with both ESV (IVPG=-0.027[ESV]+3.46, r=-0.64) and EDV (IVPG=-0.027[EDV]+4.30, r=-0.70). Improvements in IVPGs correlated with improvements in apical tau (Deltatau =5.93[DeltaIVPG]+4.76, r=0.91) and basal tau (Deltatau =2.41[DeltaIVPG]+5.13, r=-0.67). Relative changes in IVPGs correlated with changes in ESV (DeltaESV=-0.97[%DeltaIVPG]+23.34, r=-0.79), EDV (DeltaEDV=-1.16[%DeltaIVPG]+34.92, r=-0.84), and EF (DeltaEF=0.38[%DeltaIVPG]-8.39, r=0.85). Improvements in LV function also increase IVPGs. These changes in IVPGs, suggestive of increases in LV suction and elastic recoil, correlate directly with improvements in LV relaxation and ESV.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MS%26E..219a2047Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MS%26E..219a2047Y"><span><span class="hlt">Gradient</span> microstructure and microhardness in a nitrided 18CrNiMo7-6 gear steel</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, R.; Wu, G. L.; Zhang, X.; Fu, W. T.; Huang, X.</p> <p>2017-07-01</p> <p>A commercial gear steel (18CrNiMo7-6) containing a tempered martensite structure was nitrided using a <span class="hlt">pressurized</span> gas nitriding process under a <span class="hlt">pressure</span> of 5 atm at 530 °C for 5 hours. The mechanical properties and microstructure of the nitrided sample were characterized by Vickers hardness measurements, X-ray diffraction, and backscatter electron imaging in a scanning electron microscope. A micro-hardness <span class="hlt">gradient</span> was identified over a distance of 500 μm with hardness values of 900 HV at the top surface and 300 HV in the core. This micro-hardness <span class="hlt">gradient</span> corresponds to a <span class="hlt">gradient</span> in the microstructure that changes from a nitride compound layer at the top surface (∼ 20 μm thick) to a diffusion zone with a decreasing nitrogen concentration and precipitate density with distance from the surface, finally reaching the core matrix layer with a recovered martensite structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22929732','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22929732"><span>Superiority of desflurane over sevoflurane and isoflurane in the presence of <span class="hlt">pressure</span>-overload right ventricle hypertrophy in rats.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Blaudszun, Grégoire; Morel, Denis R</p> <p>2012-11-01</p> <p>Pulmonary hypertension and associated <span class="hlt">pressure</span>-overload right ventricular (RV) hypertrophy represent a tremendous challenge for the anesthesiologist, as optimal perioperative management is mandatory. However, the <span class="hlt">ideal</span> anesthetic agent remains unknown because scientific evidence is lacking. Twenty-eight rats were randomly assigned to a control or a monocrotaline group (60 mg kg). Four weeks later, animals were anesthetized, instrumented with a RV conductance catheter, and underwent well-controlled dose-responses to isoflurane, desflurane, and sevoflurane inhalation (minimum alveolar concentrations 0.5, 1.0, 1.5). Compared with controls, rats injected with monocrotaline presented with RV hypertrophy, increased afterload, and contractility, without change in cardiac output. The ratio of <span class="hlt">pressures</span> in the right over the left circulation increased. The halogenated volatiles differently altered hemodynamics. Sevoflurane reduced RV contractility (more than 50%) and the right over left <span class="hlt">pressures</span> ratio increased (from 0.41 ± 0.08 [SD] to 0.82 ± 0.14; P < 0.0001) secondary to profound concomitant systemic vasodilation, demonstrating a critical <span class="hlt">pressure</span> <span class="hlt">gradient</span> between right and left circulations. Despite significantly higher RV systolic <span class="hlt">pressures</span> and afterload, desflurane decreased RV contractility much less (<10%; P < 0.0001 vs. sevoflurane) and maintained the right over left <span class="hlt">pressures</span> ratio at more favorable values (0.47 ± 0.07; P < 0.0001 vs. sevoflurane). Isoflurane presented intermediate effects. In the presence of <span class="hlt">pressure</span>-overload RV hypertrophy, hemodynamics are better preserved under desflurane inhalation, whereas sevoflurane-and to a lesser extent isoflurane-cause large discrepancies on the left and right circulations, raising the right over left <span class="hlt">pressures</span> ratio to critical levels despite a conserved cardiac output.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_18 --> <div id="page_19" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="361"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JBO....23c6005H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JBO....23c6005H"><span>In vivo photoacoustic imaging of chorioretinal oxygen <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hariri, Ali; Wang, Junxin; Kim, Yeji; Jhunjhunwala, Anamik; Chao, Daniel L.; Jokerst, Jesse V.</p> <p>2018-03-01</p> <p>Chorioretinal imaging has a crucial role for the patients with chorioretinal vascular diseases, such as neovascular age-related macular degeneration. Imaging oxygen <span class="hlt">gradients</span> in the eye could better diagnose and treat ocular diseases. Here, we describe the use of photoacoustic ocular imaging (PAOI) in measuring chorioretinal oxygen saturation (CR - sO2) <span class="hlt">gradients</span> in New Zealand white rabbits (n = 5) with ocular ischemia. We observed good correlation (R2 = 0.98) between pulse oximetry and PAOI as a function of different oxygen percentages in inhaled air. We then used an established ocular ischemia model in which intraocular <span class="hlt">pressure</span> is elevated to constrict ocular blood flow, and notice a positive correlation (R2 = 0.92) between the injected volume of phosphate buffered saline (PBS) and intraocular <span class="hlt">pressure</span> (IOP) as well as a negative correlation (R2 = 0.98) between CR - sO2 and injected volume of PBS. The CR - sO2 was measured before (baseline), during (ischemia), and after the infusion (600-μL PBS). The ischemia-reperfusion model did not affect the measurement of the sO2 using a pulse oximeter on the animal's paw, but the chorioretinal PAOI signal showed a nearly sixfold decrease in CR - sO2 (n = 5, p = 0.00001). We also observe a sixfold decrease in CR - sO2 after significant elevation of IOP during ischemia, with an increase close to baseline during reperfusion. These data suggest that PAOI can detect changes in chorioretinal oxygenation and may be useful for application to imaging oxygen <span class="hlt">gradients</span> in ocular disease.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..MAR.T1383K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..MAR.T1383K"><span>Study of the <span class="hlt">Pressure</span> and Velocity Across the Aortic Valve</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kyung, Seo Young; Chung, Erica Soyun; Lee, Joo Hee; Kyung, Hayoung; Choi, Si Young</p> <p></p> <p>Biomechanics of the heart, requiring an extensive understanding of the complexity of the heart, have become the interests of many biomedical engineers in cardiology today. In order to study aortic valve disease, engineers have focused on the data obtained through bio-fluid flow analysis. To further this study, physical and computational analysis on the biomechanical determinants of blood flow in the stenosed aortic valve have been examined. These observations, along with the principles of cardiovascular physiology, confirm that when blood flows through the valve opening, <span class="hlt">pressure</span> <span class="hlt">gradient</span> across the valve is produced as a result of stenosis of the aortic valve. The aortic valve <span class="hlt">gradient</span> is used to interpret the increase and decrease on each side of the defective valve. To compute different <span class="hlt">pressure</span> <span class="hlt">gradients</span> across the aortic valve, this paper analyzes Aortic Valve Areas (AVA) using simulations based on the continuity equation and Gorlin equation. The data obtained from such analysis consist of patients in the AS category that display mild Aortic Valve Velocity (AVV) and <span class="hlt">pressure</span> <span class="hlt">gradient</span>. Such correlation results in the construction of a dependent relationship between severe AS causing LV systolic dysfunction and the transaortic velocity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27859549','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27859549"><span>On the accurate analysis of vibroacoustics in head insert <span class="hlt">gradient</span> coils.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Winkler, Simone A; Alejski, Andrew; Wade, Trevor; McKenzie, Charles A; Rutt, Brian K</p> <p>2017-10-01</p> <p>To accurately analyze vibroacoustics in MR head <span class="hlt">gradient</span> coils. A detailed theoretical model for <span class="hlt">gradient</span> coil vibroacoustics, including the first description and modeling of Lorentz damping, is introduced and implemented in a multiphysics software package. Numerical finite-element method simulations were used to establish a highly accurate vibroacoustic model in head <span class="hlt">gradient</span> coils in detail, including the newly introduced Lorentz damping effect. Vibroacoustic coupling was examined through an additional modal analysis. Thorough experimental studies were used to validate simulations. Average experimental sound <span class="hlt">pressure</span> levels (SPLs) and accelerations over the 0-3000 Hz frequency range were 97.6 dB, 98.7 dB, and 95.4 dB, as well as 20.6 g, 8.7 g, and 15.6 g for the X-, Y-, and Z-<span class="hlt">gradients</span>, respectively. A reasonable agreement between simulations and measurements was achieved. Vibroacoustic coupling showed a coupled resonance at 2300 Hz for the Z-<span class="hlt">gradient</span> that is responsible for a sharp peak and the highest SPL value in the acoustic spectrum. We have developed and used more realistic multiphysics simulation methods to gain novel insights into the underlying concepts for vibroacoustics in head <span class="hlt">gradient</span> coils, which will permit improved analyses of existing <span class="hlt">gradient</span> coils and novel SPL reduction strategies for future <span class="hlt">gradient</span> coil designs. Magn Reson Med 78:1635-1645, 2017. © 2016 International Society for Magnetic Resonance in Medicine. © 2016 International Society for Magnetic Resonance in Medicine.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70190419','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70190419"><span>Understanding differences between DELFT3D and empirical predictions of alongshore sediment transport <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>List, Jeffrey; Benedet, Lindino; Hanes, Daniel M.; Ruggiero, Peter</p> <p>2009-01-01</p> <p>Predictions of alongshore transport <span class="hlt">gradients</span> are critical for forecasting shoreline change. At the previous ICCE conference, it was demonstrated that alongshore transport <span class="hlt">gradients</span> predicted by the empirical CERC equation can differ substantially from predictions made by the hydrodynamics-based model Delft3D in the case of a simulated borrow pit on the shoreface. Here we use the Delft3D momentum balance to examine the reason for this difference. Alongshore advective flow accelerations in our Delft3D simulation are mainly driven by <span class="hlt">pressure</span> <span class="hlt">gradients</span> resulting from alongshore variations in wave height and setup, and Delft3D transport <span class="hlt">gradients</span> are controlled by these flow accelerations. The CERC equation does not take this process into account, and for this reason a second empirical transport term is sometimes added when alongshore <span class="hlt">gradients</span> in wave height are thought to be significant. However, our test case indicates that this second term does not properly predict alongshore transport <span class="hlt">gradients</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16960297','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16960297"><span>Erroneous intracranial <span class="hlt">pressure</span> measurements from simultaneous <span class="hlt">pressure</span> monitoring and ventricular drainage catheters.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Birch, A A; Eynon, C A; Schley, D</p> <p>2006-01-01</p> <p>The objective of this report is to highlight the potential for false <span class="hlt">pressure</span> measurements from systems that combine intracranial <span class="hlt">pressure</span> (ICP) measurement and ventricular drainage. If the ports of the drain become blocked to the extent that they present a high resistance to cerebrospinal fluid flow, then a significant <span class="hlt">pressure</span> <span class="hlt">gradient</span> between the inside and outside of the catheter may be established. Thus, any intracatheter transducer will faithfully record a <span class="hlt">pressure</span> much lower than true ICP. This holds true for catheter-tip transducers when the transducer lies inside the catheter. In the absence of flow, however, <span class="hlt">pressures</span> will equalize; therefore, accurate measurements may be taken if the drain is temporarily closed. We model this situation and provide simulations of expected measurements in such situations; these compare well to observed clinical readings.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26141912','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26141912"><span>Association of <span class="hlt">Ideal</span> Cardiovascular Health and Long-term Healthcare Costs.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Willis, Benjamin L; DeFina, Laura F; Bachmann, Justin M; Franzini, Luisa; Shay, Christina M; Gao, Ang; Leonard, David; Berry, Jarett D</p> <p>2015-11-01</p> <p>The American Heart Association's (AHA's) 2020 Strategic Impact Goals introduced the concept of <span class="hlt">ideal</span> cardiovascular (CV) health based on seven health factors and behaviors associated with lower CV disease (CVD) risk. The association between CV health and healthcare costs has not been reported; therefore, we evaluated the association between CV health profile and later-life healthcare costs. Cooper Center Longitudinal Study participants (N=4,906; mean age, 56 years) receiving Medicare coverage from 1999 to 2009 were included. CV health behaviors (diet, physical activity, BMI, smoking) and CV health factors (blood <span class="hlt">pressure</span>, total cholesterol, blood glucose) were categorized as unfavorable (zero to two <span class="hlt">ideal</span> components); intermediate (two to four); and favorable (five to seven). Healthcare costs were cumulated from Medicare claims data, adjusted for inflation. Associations between midlife CV health status and non-CVD and CVD-related costs were estimated using multivariable quantile regression. Analyses were conducted in 2013 and 2014. Favorable CV health was prevalent in 14.8% of men and 30.1% of women, with <1% having <span class="hlt">ideal</span> levels of all health metrics. After 31,945 person-years of Medicare follow-up, individuals with favorable CV health exhibited 24.9% (95% CI=11.7%, 36.0%) lower median annual non-CVD costs and 74.5% (57.5%, 84.7%) lower median CVD costs than those with unfavorable CV health. Annualized differences were greater for non-CVD costs than for CVD costs ($1,175 vs $566). Having more <span class="hlt">ideal</span> CV health components in middle age, as outlined by the AHA 2020 Goals, is associated with lower non-CVD and CVD healthcare costs in later life. Copyright © 2015 American Journal of Preventive Medicine. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24834936','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24834936"><span><span class="hlt">Pressure</span> chamber tests of eustachian tube function document lower efficiency in adults with colds when compared to without colds.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Doyle, William J; Singla, Alok; Banks, Juliane; El-Wagaa, Jenna; Swarts, J Douglas</p> <p>2014-07-01</p> <p>Fractional <span class="hlt">gradient</span> equilibrated (FGE) for ears with applied positive but not negative middle ear (ME)-ambient <span class="hlt">pressure</span> <span class="hlt">gradients</span> is highly sensitive to a cold-like illness (CLI). The sequential development of eustachian tube (ET) dysfunction, ME under-<span class="hlt">pressure</span>, and otitis media (OM) characterizes many children during a CLI. If linked, OM burden would be lessened by interventions that promote/preserve good ET function during a CLI. Evaluating this requires a quantitative ET function test for MEs with an intact tympanic membrane responsive to a CLI. <span class="hlt">Pressure</span> chamber testing of ET function was performed at +200 and -200 daPa in 3 groups of adults: group I, 21 subjects with an extant CLI and groups II and III, 14 and 57 adults, respectively, without a CLI. ME-chamber <span class="hlt">pressure</span> <span class="hlt">gradient</span> was recorded by tympanometry before and after the subject swallowed twice. ET functional efficiency was quantified as the FGE, which was then compared among groups using a Mann-Whitney U test. At chamber <span class="hlt">pressures</span> of 200 daPa, the ME-chamber <span class="hlt">pressure</span> <span class="hlt">gradient</span> was negative, and FGE was low and not different among groups. At chamber <span class="hlt">pressures</span> of -200 daPa that <span class="hlt">gradient</span> was positive, and FGE was significantly higher in groups II and III when compared with group I.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27545828','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27545828"><span>Airway driving <span class="hlt">pressure</span> and lung stress in ARDS patients.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chiumello, Davide; Carlesso, Eleonora; Brioni, Matteo; Cressoni, Massimo</p> <p>2016-08-22</p> <p>Lung-protective ventilation strategy suggests the use of low tidal volume, depending on <span class="hlt">ideal</span> body weight, and adequate levels of PEEP. However, reducing tidal volume according to <span class="hlt">ideal</span> body weight does not always prevent overstress and overstrain. On the contrary, titrating mechanical ventilation on airway driving <span class="hlt">pressure</span>, computed as airway <span class="hlt">pressure</span> changes from PEEP to end-inspiratory plateau <span class="hlt">pressure</span>, equivalent to the ratio between the tidal volume and compliance of respiratory system, should better reflect lung injury. However, possible changes in chest wall elastance could affect the reliability of airway driving <span class="hlt">pressure</span>. The aim of this study was to evaluate if airway driving <span class="hlt">pressure</span> could accurately predict lung stress (the <span class="hlt">pressure</span> generated into the lung due to PEEP and tidal volume). One hundred and fifty ARDS patients were enrolled. At 5 and 15 cmH2O of PEEP, lung stress, driving <span class="hlt">pressure</span>, lung and chest wall elastance were measured. The applied tidal volume (mL/kg of <span class="hlt">ideal</span> body weight) was not related to lung gas volume (r (2) = 0.0005 p = 0.772). Patients were divided according to an airway driving <span class="hlt">pressure</span> lower and equal/higher than 15 cmH2O (the lower and higher airway driving <span class="hlt">pressure</span> groups). At both PEEP levels, the higher airway driving <span class="hlt">pressure</span> group had a significantly higher lung stress, respiratory system and lung elastance compared to the lower airway driving <span class="hlt">pressure</span> group. Airway driving <span class="hlt">pressure</span> was significantly related to lung stress (r (2) = 0.581 p < 0.0001 and r (2) = 0.353 p < 0.0001 at 5 and 15 cmH2O of PEEP). For a lung stress of 24 and 26 cmH2O, the optimal cutoff value for the airway driving <span class="hlt">pressure</span> were 15.0 cmH2O (ROC AUC 0.85, 95 % CI = 0.782-0.922); and 16.7 (ROC AUC 0.84, 95 % CI = 0.742-0.936). Airway driving <span class="hlt">pressure</span> can detect lung overstress with an acceptable accuracy. However, further studies are needed to establish if these limits could be used for ventilator settings.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730009903','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730009903"><span>Objective sea level <span class="hlt">pressure</span> analysis for sparse data areas</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Druyan, L. M.</p> <p>1972-01-01</p> <p>A computer procedure was used to analyze the <span class="hlt">pressure</span> distribution over the North Pacific Ocean for eleven synoptic times in February, 1967. Independent knowledge of the central <span class="hlt">pressures</span> of lows is shown to reduce the analysis errors for very sparse data coverage. The application of planned remote sensing of sea-level wind speeds is shown to make a significant contribution to the quality of the analysis especially in the high <span class="hlt">gradient</span> mid-latitudes and for sparse coverage of conventional observations (such as over Southern Hemisphere oceans). Uniform distribution of the available observations of sea-level <span class="hlt">pressure</span> and wind velocity yields results far superior to those derived from a random distribution. A generalization of the results indicates that the average lower limit for analysis errors is between 2 and 2.5 mb based on the perfect specification of the magnitude of the sea-level <span class="hlt">pressure</span> <span class="hlt">gradient</span> from a known verification analysis. A less than perfect specification will derive from wind-<span class="hlt">pressure</span> relationships applied to satellite observed wind speeds.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23772898','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23772898"><span>Highly robust thin-film composite <span class="hlt">pressure</span> retarded osmosis (PRO) hollow fiber membranes with high power densities for renewable salinity-<span class="hlt">gradient</span> energy generation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Han, Gang; Wang, Peng; Chung, Tai-Shung</p> <p>2013-07-16</p> <p>The practical application of <span class="hlt">pressure</span> retarded osmosis (PRO) technology for renewable blue energy (i.e., osmotic power generation) from salinity <span class="hlt">gradient</span> is being hindered by the absence of effective membranes. Compared to flat-sheet membranes, membranes with a hollow fiber configuration are of great interest due to their high packing density and spacer-free module fabrication. However, the development of PRO hollow fiber membranes is still in its infancy. This study aims to open up new perspectives and design strategies to molecularly construct highly robust thin film composite (TFC) PRO hollow fiber membranes with high power densities. The newly developed TFC PRO membranes consist of a selective polyamide skin formed on the lumen side of well-constructed Matrimid hollow fiber supports via interfacial polymerization. For the first time, laboratory PRO power generation tests demonstrate that the newly developed PRO hollow fiber membranes can withstand trans-membrane <span class="hlt">pressures</span> up to 16 bar and exhibit a peak power density as high as 14 W/m(2) using seawater brine (1.0 M NaCl) as the draw solution and deionized water as the feed. We believe that the developed TFC PRO hollow fiber membranes have great potential for osmotic power harvesting.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27165887','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27165887"><span>Bernoulli's Principle Applied to Brain Fluids: Intracranial <span class="hlt">Pressure</span> Does Not Drive Cerebral Perfusion or CSF Flow.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Schmidt, Eric; Ros, Maxime; Moyse, Emmanuel; Lorthois, Sylvie; Swider, Pascal</p> <p>2016-01-01</p> <p>In line with the first law of thermodynamics, Bernoulli's principle states that the total energy in a fluid is the same at all points. We applied Bernoulli's principle to understand the relationship between intracranial <span class="hlt">pressure</span> (ICP) and intracranial fluids. We analyzed simple fluid physics along a tube to describe the interplay between <span class="hlt">pressure</span> and velocity. Bernoulli's equation demonstrates that a fluid does not flow along a <span class="hlt">gradient</span> of <span class="hlt">pressure</span> or velocity; a fluid flows along a <span class="hlt">gradient</span> of energy from a high-energy region to a low-energy region. A fluid can even flow against a <span class="hlt">pressure</span> <span class="hlt">gradient</span> or a velocity <span class="hlt">gradient</span>. <span class="hlt">Pressure</span> and velocity represent part of the total energy. Cerebral blood perfusion is not driven by <span class="hlt">pressure</span> but by energy: the blood flows from high-energy to lower-energy regions. Hydrocephalus is related to increased cerebrospinal fluid (CSF) resistance (i.e., energy transfer) at various points. Identification of the energy transfer within the CSF circuit is important in understanding and treating CSF-related disorders. Bernoulli's principle is not an abstract concept far from clinical practice. We should be aware that <span class="hlt">pressure</span> is easy to measure, but it does not induce resumption of fluid flow. Even at the bedside, energy is the key to understanding ICP and fluid dynamics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DPPU11048L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DPPU11048L"><span>The temporal evolution of the resistive <span class="hlt">pressure-gradient</span>-driven turbulence and anomalous transport in shear flow across the magnetic field</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, Hae June; Mikhailenko, Vladmir; Mikhailenko, Vladimir</p> <p>2017-10-01</p> <p>The temporal evolution of the resistive <span class="hlt">pressure-gradient</span>-driven mode in the sheared flow is investigated by employing the shearing modes approach. It reveals an essential difference in the processes, which occur in the case of the flows with velocity shearing rate less than the growth rate of the instability in the steady plasmas, and in the case of the flows with velocity shear larger than the instability growth rate in steady plasmas. It displays the physical content of the empirical ``quench rule'' which predicts the suppression of the turbulence in the sheared flows when the velocity shearing rate becomes larger than the maximum growth rate of the possible instability. We found that the distortion of the perturbations by the sheared flow with such velocity shear introduces the time dependencies into the governing equations, which prohibits the application of the eigenmodes formalism and requires the solution of the initial value problem.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DPPJ11118D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DPPJ11118D"><span>Density-<span class="hlt">Gradient</span>-Driven trapped-electron-modes in improved-confinement RFP plasmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Duff, James; Sarff, John; Ding, Weixing; Brower, David; Parke, Eli; Chapman, Brett; Terry, Paul; Pueschel, M. J.; Williams, Zach</p> <p>2017-10-01</p> <p>Short wavelength density fluctuations in improved-confinement MST plasmas exhibit multiple features characteristic of the trapped-electron-mode (TEM). Core transport in the RFP is normally governed by magnetic stochasticity stemming from long wavelength tearing modes that arise from current profile peaking, which are suppressed via inductive control for this work. The improved confinement is associated with an increase in the <span class="hlt">pressure</span> <span class="hlt">gradient</span> that can destabilize drift waves. The measured density fluctuations have f 50 kHz, kϕρs < 0.14 , and propagate in the electron drift direction. Their spectral emergence coincides with a sharp decrease in global tearing mode associated fluctuations, their amplitude increases with local density <span class="hlt">gradient</span>, and they exhibit a density-<span class="hlt">gradient</span> threshold at R /Ln 15 . The GENE code, modified for the RFP, predicts the onset of density-<span class="hlt">gradient</span>-driven TEM for these strong-<span class="hlt">gradient</span> plasma conditions. While nonlinear analysis shows a large Dimits shift associated with predicted strong zonal flows, the inclusion of residual magnetic fluctuations, comparable to experimental magnetic fluctuations, causes a collapse of the zonal flows and an increase in the predicted transport to a level close to the experimentally measured heat flux. Work supported by US DOE.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=433198','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=433198"><span>Thermal Motion and Forced Migration of Colloidal Particles Generate Hydrostatic <span class="hlt">Pressure</span> in Solvent</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Hammel, H. T.; Scholander, P. F.</p> <p>1973-01-01</p> <p>A colloidal solution of ferrite particles in an osmometer has been used to demonstrate that the property that propels water across the semipermeable membrane is the decrease in hydrostatic <span class="hlt">pressure</span> in the water of the solution. A magnetic field <span class="hlt">gradient</span> directed so as to force the ferrite particles away from the semipermeable membrane of the osmometer and toward the free surface of the solution enhanced the colloidal osmotic <span class="hlt">pressure</span>. The enhancement of this <span class="hlt">pressure</span> was always exactly equal to the augmentation of the <span class="hlt">pressure</span> as measured by the outward force of the particles, against the area of the free surface. Contrariwise, directing the magnetic field <span class="hlt">gradient</span> so as to force the ferrite particles away from the free surface and toward the semipermeable membrane diminished the colloidal osmotic <span class="hlt">pressure</span> of the solution. For a sufficiently forceful field <span class="hlt">gradient</span>, the initial colloidal osmotic <span class="hlt">pressure</span> could be negative, followed by an equilibrium <span class="hlt">pressure</span> approaching zero regardless of the force of the particles against the membrane. Thus, the osmotic <span class="hlt">pressure</span> of a solution is to be attributed to the <span class="hlt">pressure</span> in the solvent generated in opposition to the <span class="hlt">pressure</span> of the solute particles caused by their interaction with the free surface (Brownian motion and/or an external field force), or by their viscous shear when they migrate through the solvent, or both. PMID:16592046</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26716691','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26716691"><span>Effects of Hydrostatic <span class="hlt">Pressure</span> on Carcinogenic Properties of Epithelia.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tokuda, Shinsaku; Kim, Young Hak; Matsumoto, Hisako; Muro, Shigeo; Hirai, Toyohiro; Mishima, Michiaki; Furuse, Mikio</p> <p>2015-01-01</p> <p>The relationship between chronic inflammation and cancer is well known. The inflammation increases the permeability of blood vessels and consequently elevates <span class="hlt">pressure</span> in the interstitial tissues. However, there have been only a few reports on the effects of hydrostatic <span class="hlt">pressure</span> on cultured cells, and the relationship between elevated hydrostatic <span class="hlt">pressure</span> and cell properties related to malignant tumors is less well understood. Therefore, we investigated the effects of hydrostatic <span class="hlt">pressure</span> on the cultured epithelial cells seeded on permeable filters. Surprisingly, hydrostatic <span class="hlt">pressure</span> from basal to apical side induced epithelial stratification in Madin-Darby canine kidney (MDCK) I and Caco-2 cells, and cavities with microvilli and tight junctions around their surfaces were formed within the multi-layered epithelia. The hydrostatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> also promoted cell proliferation, suppressed cell apoptosis, and increased transepithelial ion permeability. The inhibition of protein kinase A (PKA) promoted epithelial stratification by the hydrostatic <span class="hlt">pressure</span> whereas the activation of PKA led to suppressed epithelial stratification. These results indicate the role of the hydrostatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> in the regulation of various epithelial cell functions. The findings in this study may provide clues for the development of a novel strategy for the treatment of the carcinoma.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4696811','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4696811"><span>Effects of Hydrostatic <span class="hlt">Pressure</span> on Carcinogenic Properties of Epithelia</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Tokuda, Shinsaku; Kim, Young Hak; Matsumoto, Hisako; Muro, Shigeo; Hirai, Toyohiro; Mishima, Michiaki; Furuse, Mikio</p> <p>2015-01-01</p> <p>The relationship between chronic inflammation and cancer is well known. The inflammation increases the permeability of blood vessels and consequently elevates <span class="hlt">pressure</span> in the interstitial tissues. However, there have been only a few reports on the effects of hydrostatic <span class="hlt">pressure</span> on cultured cells, and the relationship between elevated hydrostatic <span class="hlt">pressure</span> and cell properties related to malignant tumors is less well understood. Therefore, we investigated the effects of hydrostatic <span class="hlt">pressure</span> on the cultured epithelial cells seeded on permeable filters. Surprisingly, hydrostatic <span class="hlt">pressure</span> from basal to apical side induced epithelial stratification in Madin-Darby canine kidney (MDCK) I and Caco-2 cells, and cavities with microvilli and tight junctions around their surfaces were formed within the multi-layered epithelia. The hydrostatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> also promoted cell proliferation, suppressed cell apoptosis, and increased transepithelial ion permeability. The inhibition of protein kinase A (PKA) promoted epithelial stratification by the hydrostatic <span class="hlt">pressure</span> whereas the activation of PKA led to suppressed epithelial stratification. These results indicate the role of the hydrostatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> in the regulation of various epithelial cell functions. The findings in this study may provide clues for the development of a novel strategy for the treatment of the carcinoma. PMID:26716691</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25978093','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25978093"><span>Combining Step <span class="hlt">Gradients</span> and Linear <span class="hlt">Gradients</span> in Density.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kumar, Ashok A; Walz, Jenna A; Gonidec, Mathieu; Mace, Charles R; Whitesides, George M</p> <p>2015-06-16</p> <p>Combining aqueous multiphase systems (AMPS) and magnetic levitation (MagLev) provides a method to produce hybrid <span class="hlt">gradients</span> in apparent density. AMPS—solutions of different polymers, salts, or surfactants that spontaneously separate into immiscible but predominantly aqueous phases—offer thermodynamically stable steps in density that can be tuned by the concentration of solutes. MagLev—the levitation of diamagnetic objects in a paramagnetic fluid within a magnetic field gradient—can be arranged to provide a near-linear <span class="hlt">gradient</span> in effective density where the height of a levitating object above the surface of the magnet corresponds to its density; the strength of the <span class="hlt">gradient</span> in effective density can be tuned by the choice of paramagnetic salt and its concentrations and by the strength and <span class="hlt">gradient</span> in the magnetic field. Including paramagnetic salts (e.g., MnSO4 or MnCl2) in AMPS, and placing them in a magnetic field <span class="hlt">gradient</span>, enables their use as media for MagLev. The potential to create large steps in density with AMPS allows separations of objects across a range of densities. The <span class="hlt">gradients</span> produced by MagLev provide resolution over a continuous range of densities. By combining these approaches, mixtures of objects with large differences in density can be separated and analyzed simultaneously. Using MagLev to add an effective <span class="hlt">gradient</span> in density also enables tuning the range of densities captured at an interface of an AMPS by simply changing the position of the container in the magnetic field. Further, by creating AMPS in which phases have different concentrations of paramagnetic ions, the phases can provide different resolutions in density. These results suggest that combining steps in density with <span class="hlt">gradients</span> in density can enable new classes of separations based on density.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2869367','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2869367"><span>Kirkwood–Buff integrals for <span class="hlt">ideal</span> solutions</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ploetz, Elizabeth A.; Bentenitis, Nikolaos; Smith, Paul E.</p> <p>2010-01-01</p> <p>The Kirkwood–Buff (KB) theory of solutions is a rigorous theory of solution mixtures which relates the molecular distributions between the solution components to the thermodynamic properties of the mixture. <span class="hlt">Ideal</span> solutions represent a useful reference for understanding the properties of real solutions. Here, we derive expressions for the KB integrals, the central components of KB theory, in <span class="hlt">ideal</span> solutions of any number of components corresponding to the three main concentration scales. The results are illustrated by use of molecular dynamics simulations for two binary solutions mixtures, benzene with toluene, and methanethiol with dimethylsulfide, which closely approach <span class="hlt">ideal</span> behavior, and a binary mixture of benzene and methanol which is nonideal. Simulations of a quaternary mixture containing benzene, toluene, methanethiol, and dimethylsulfide suggest this system displays <span class="hlt">ideal</span> behavior and that <span class="hlt">ideal</span> behavior is not limited to mixtures containing a small number of components. PMID:20441282</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003JGRA..108.1331G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003JGRA..108.1331G"><span><span class="hlt">Pressure</span> balance inconsistency exhibited in a statistical model of magnetospheric plasma</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Garner, T. W.; Wolf, R. A.; Spiro, R. W.; Thomsen, M. F.; Korth, H.</p> <p>2003-08-01</p> <p>While quantitative theories of plasma flow from the magnetotail to the inner magnetosphere typically assume adiabatic convection, it has long been understood that these convection models tend to overestimate the plasma <span class="hlt">pressure</span> in the inner magnetosphere. This phenomenon is called the <span class="hlt">pressure</span> crisis or the <span class="hlt">pressure</span> balance inconsistency. In order to analyze it in a new and more detailed manner we utilize an empirical model of the proton and electron distribution functions in the near-Earth plasma sheet (-50 RE < X < -10 RE), which uses the [1989] magnetic field model and a plasma sheet representation based upon several previously published statistical studies. We compare our results to a statistically derived particle distribution function at geosynchronous orbit. In this analysis the particle distribution function is characterized by the isotropic energy invariant λ = EV2/3, where E is the particle's kinetic energy and V is the magnetic flux tube volume. The energy invariant is conserved in guiding center drift under the assumption of strong, elastic pitch angle scattering. If, in addition, loss is negligible, the phase space density f(λ) is also conserved along the same path. The statistical model indicates that f(λ, ?) is approximately independent of X for X ≤ -35 RE but decreases with increasing X for X ≥ -35 RE. The tailward <span class="hlt">gradient</span> of f(λ, ?) might be attributed to <span class="hlt">gradient</span>/curvature drift for large isotropic energy invariants but not for small invariants. The tailward <span class="hlt">gradient</span> of the distribution function indicates a violation of the adiabatic drift condition in the plasma sheet. It also confirms the existence of a "number crisis" in addition to the <span class="hlt">pressure</span> crisis. In addition, plasma sheet <span class="hlt">pressure</span> <span class="hlt">gradients</span>, when crossed with the <span class="hlt">gradient</span> of flux tube volume computed from the [1989] magnetic field model, indicate Region 1 currents on the dawn and dusk sides of the outer plasma sheet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JAMES...9.1431S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JAMES...9.1431S"><span><span class="hlt">Idealized</span> modeling of convective organization with changing sea surface temperatures using multiple equilibria in weak temperature <span class="hlt">gradient</span> simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sentić, Stipo; Sessions, Sharon L.</p> <p>2017-06-01</p> <p>The weak temperature <span class="hlt">gradient</span> (WTG) approximation is a method of parameterizing the influences of the large scale on local convection in limited domain simulations. WTG simulations exhibit multiple equilibria in precipitation; depending on the initial moisture content, simulations can precipitate or remain dry for otherwise identical boundary conditions. We use a hypothesized analogy between multiple equilibria in precipitation in WTG simulations, and dry and moist regions of organized convection to study tropical convective organization. We find that the range of wind speeds that support multiple equilibria depends on sea surface temperature (SST). Compared to the present SST, low SSTs support a narrower range of multiple equilibria at higher wind speeds. In contrast, high SSTs exhibit a narrower range of multiple equilibria at low wind speeds. This suggests that at high SSTs, organized convection might occur with lower surface forcing. To characterize convection at different SSTs, we analyze the change in relationships between precipitation rate, atmospheric stability, moisture content, and the large-scale transport of moist entropy and moisture with increasing SSTs. We find an increase in large-scale export of moisture and moist entropy from dry simulations with increasing SST, which is consistent with a strengthening of the up-<span class="hlt">gradient</span> transport of moisture from dry regions to moist regions in organized convection. Furthermore, the changes in diagnostic relationships with SST are consistent with more intense convection in precipitating regions of organized convection for higher SSTs.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_19 --> <div id="page_20" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="381"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18510603','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18510603"><span>Gastroesophageal <span class="hlt">pressure</span> <span class="hlt">gradients</span> in gastroesophageal reflux disease: relations with hiatal hernia, body mass index, and esophageal acid exposure.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>de Vries, Durk R; van Herwaarden, Margot A; Smout, André J P M; Samsom, Melvin</p> <p>2008-06-01</p> <p>The roles of intragastric <span class="hlt">pressure</span> (IGP), intraesophageal <span class="hlt">pressure</span> (IEP), gastroesophageal <span class="hlt">pressure</span> <span class="hlt">gradient</span> (GEPG), and body mass index (BMI) in the pathophysiology of gastroesophageal reflux disease (GERD) and hiatal hernia (HH) are only partly understood. In total, 149 GERD patients underwent stationary esophageal manometry, 24-h pH-metry, and endoscopy. One hundred three patients had HH. Linear regression analysis showed that each kilogram per square meter of BMI caused a 0.047-kPa increase in inspiratory IGP (95% confidence interval [CI] 0.026-0.067) and a 0.031-kPa increase in inspiratory GEPG (95% CI 0.007-0.055). Each kilogram per square meter of BMI caused expiratory IGP to increase with 0.043 kPa (95% CI 0.025-0.060) and expiratory IEP with 0.052 kPa (95% CI 0.027-0.077). Each added year of age caused inspiratory IEP to decrease by 0.008 kPa (95% CI -0.015-0.001) and inspiratory GEPG to increase by 0.008 kPa (95% CI 0.000-0.015). In binary logistic regression analysis, HH was predicted by inspiratory and expiratory IGP (odds ratio [OR] 2.93 and 2.62, respectively), inspiratory and expiratory GEPG (OR 3.19 and 2.68, respectively), and BMI (OR 1.72/5 kg/m(2)). In linear regression analysis, HH caused an average 5.09% increase in supine acid exposure (95% CI 0.96-9.22) and an average 3.46% increase in total acid exposure (95% CI 0.82-6.09). Each added year of age caused an average 0.10% increase in upright acid exposure and a 0.09% increase in total acid exposure (95% CI 0.00-0.20 and 0.00-0.18). BMI predicts IGP, inspiratory GEPG, and expiratory IEP. Age predicts inspiratory IEP and GEPG. Presence of HH is predicted by IGP, GEPG, and BMI. GEPG is not associated with acid exposure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21373963','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21373963"><span>Water flux through human aquaporin 1: inhibition by intracellular furosemide and maximal response with high osmotic <span class="hlt">gradients</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ozu, Marcelo; Dorr, Ricardo A; Teresa Politi, M; Parisi, Mario; Toriano, Roxana</p> <p>2011-06-01</p> <p>This work studies water permeability properties of human aquaporin 1 (hAQP1) expressed in Xenopus laevis oocyte membranes, applying a technique where cellular content is replaced with a known medium, with the possibility of measuring intracellular <span class="hlt">pressure</span>. Consequences on water transport-produced by well-known anisotonic <span class="hlt">gradients</span> and by the intracellular effect of probable aquaporin inhibitors-were tested. In this way, the specific intracellular inhibition of hAQP1 by the diuretic drug furosemide was demonstrated. In addition, experiments imposing anisotonic mannitol <span class="hlt">gradients</span> with a constant ionic strength showed that the relationship between water flux and the applied mannitol <span class="hlt">gradient</span> deflects from a perfect osmometer response when the <span class="hlt">gradient</span> is higher than 150 mosmol kg (W) (-1) . These results would indicate that the passage of water molecules through hAQP1 may have a maximum rate. As a whole, this work demonstrates the technical advantage of controlling both intracellular <span class="hlt">pressure</span> and medium composition in order to study biophysical properties of hAQP1, and contributes information on water channel behavior under osmotic challenges and the discovery of new inhibitors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29115059','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29115059"><span>Universal field matching in craniospinal irradiation by a background-dose <span class="hlt">gradient</span>-optimized method.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Traneus, Erik; Bizzocchi, Nicola; Fellin, Francesco; Rombi, Barbara; Farace, Paolo</p> <p>2018-01-01</p> <p>The <span class="hlt">gradient</span>-optimized methods are overcoming the traditional feathering methods to plan field junctions in craniospinal irradiation. In this note, a new <span class="hlt">gradient</span>-optimized technique, based on the use of a background dose, is described. Treatment planning was performed by RayStation (RaySearch Laboratories, Stockholm, Sweden) on the CT scans of a pediatric patient. Both proton (by pencil beam scanning) and photon (by volumetric modulated arc therapy) treatments were planned with three isocenters. An 'in silico' <span class="hlt">ideal</span> background dose was created first to cover the upper-spinal target and to produce a perfect dose <span class="hlt">gradient</span> along the upper and lower junction regions. Using it as background, the cranial and the lower-spinal beams were planned by inverse optimization to obtain dose coverage of their relevant targets and of the junction volumes. Finally, the upper-spinal beam was inversely planned after removal of the background dose and with the previously optimized beams switched on. In both proton and photon plans, the optimized cranial and the lower-spinal beams produced a perfect linear <span class="hlt">gradient</span> in the junction regions, complementary to that produced by the optimized upper-spinal beam. The final dose distributions showed a homogeneous coverage of the targets. Our simple technique allowed to obtain high-quality <span class="hlt">gradients</span> in the junction region. Such technique universally works for photons as well as protons and could be applicable to the TPSs that allow to manage a background dose. © 2017 The Authors. Journal of Applied Clinical Medical Physics published by Wiley Periodicals, Inc. on behalf of American Association of Physicists in Medicine.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28413417','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28413417"><span>The Dialysis Sodium <span class="hlt">Gradient</span>: A Modifiable Risk Factor for Fluid Overload.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Trinh, Emilie; Weber, Catherine</p> <p>2017-01-01</p> <p>Fluid overload in patients on conventional hemodialysis is a frequent complication, associated with increased cardiovascular morbidity and mortality. The dialysate sodium prescription is a potential modifiable risk factor. Our primary objective was to describe associations between dialysate-to-serum sodium <span class="hlt">gradient</span> and parameters of fluid status. A secondary objective was to evaluate the 6-month risk of hospitalization and mortality in relation to sodium <span class="hlt">gradient</span>. We performed a cross-sectional study of 110 prevalent conventional hemodialysis patients at a single center. The associations of sodium <span class="hlt">gradient</span> with interdialytic weight gain index (IDWG%), ultrafiltration (UF) rate, and blood <span class="hlt">pressure</span> (BP) were analyzed. The mean serum sodium <span class="hlt">gradient</span> was 4.6 ± 3.6 mEq/L. There was a direct correlation between sodium <span class="hlt">gradient</span> and IDWG% ( r = 0.48, p < 0.01) as well as UF rate ( r = 0.44, p < 0.01). In a logistic regression model, a 1 mEq/L higher sodium <span class="hlt">gradient</span> was associated with increased risk of IDWG% >3% (OR 1.33, p < 0.01) and increased risk of UF rate >10 mL/kg/h (OR 1.16, p = 0.03), but there were no associations with intradialytic hypotension, intradialytic hypertension or BP. No significant differences were found with 6-month hospitalization or mortality risk in relation to sodium <span class="hlt">gradient</span>. A higher sodium <span class="hlt">gradient</span> was associated with significant increases in IDWG and UF rates, known to be associated with poor outcomes, but was not associated with intradialytic hypotension. Individualizing the dialysate sodium prescription to minimize sodium gap may lead to less fluid overload in conventional hemodialysis patients.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24824969','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24824969"><span><span class="hlt">Ideal</span> regularization for learning kernels from labels.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pan, Binbin; Lai, Jianhuang; Shen, Lixin</p> <p>2014-08-01</p> <p>In this paper, we propose a new form of regularization that is able to utilize the label information of a data set for learning kernels. The proposed regularization, referred to as <span class="hlt">ideal</span> regularization, is a linear function of the kernel matrix to be learned. The <span class="hlt">ideal</span> regularization allows us to develop efficient algorithms to exploit labels. Three applications of the <span class="hlt">ideal</span> regularization are considered. Firstly, we use the <span class="hlt">ideal</span> regularization to incorporate the labels into a standard kernel, making the resulting kernel more appropriate for learning tasks. Next, we employ the <span class="hlt">ideal</span> regularization to learn a data-dependent kernel matrix from an initial kernel matrix (which contains prior similarity information, geometric structures, and labels of the data). Finally, we incorporate the <span class="hlt">ideal</span> regularization to some state-of-the-art kernel learning problems. With this regularization, these learning problems can be formulated as simpler ones which permit more efficient solvers. Empirical results show that the <span class="hlt">ideal</span> regularization exploits the labels effectively and efficiently. Copyright © 2014 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhCS1003a2064M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS1003a2064M"><span>Intuitionistic fuzzy n-fold KU-<span class="hlt">ideal</span> of KU-algebra</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mostafa, Samy M.; Kareem, Fatema F.</p> <p>2018-05-01</p> <p>In this paper, we apply the notion of intuitionistic fuzzy n-fold KU-<span class="hlt">ideal</span> of KU-algebra. Some types of <span class="hlt">ideals</span> such as intuitionistic fuzzy KU-<span class="hlt">ideal</span>, intuitionistic fuzzy closed <span class="hlt">ideal</span> and intuitionistic fuzzy n-fold KU-<span class="hlt">ideal</span> are studied. Also, the relations between intuitionistic fuzzy n-fold KU-<span class="hlt">ideal</span> and intuitionistic fuzzy KU-<span class="hlt">ideal</span> are discussed. Furthermore, a few results of intuitionistic fuzzy n-fold KU-<span class="hlt">ideals</span> of a KU-algebra under homomorphism are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4696945','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4696945"><span>Hepatic Venous <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> Predicts Long-Term Mortality in Patients with Decompensated Cirrhosis</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kim, Tae Yeob; Lee, Jae Gon; Kim, Ji Yeoun; Kim, Sun Min; Kim, Jinoo; Jeong, Woo Kyoung</p> <p>2016-01-01</p> <p>Purpose The present study aimed to investigate the role of hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> (HVPG) for prediction of long-term mortality in patients with decompensated cirrhosis. Materials and Methods Clinical data from 97 non-critically-ill cirrhotic patients with HVPG measurements were retrospectively and consecutively collected between 2009 and 2012. Patients were classified according to clinical stages and presence of ascites. The prognostic accuracy of HVPG for death, survival curves, and hazard ratios were analyzed. Results During a median follow-up of 24 (interquartile range, 13-36) months, 22 patients (22.7%) died. The area under the receiver operating characteristics curves of HVPG for predicting 1-year, 2-year, and overall mortality were 0.801, 0.737, and 0.687, respectively (all p<0.01). The best cut-off value of HVPG for predicting long-term overall mortality in all patients was 17 mm Hg. The mortality rates at 1 and 2 years were 8.9% and 19.2%, respectively: 1.9% and 11.9% with HVPG ≤17 mm Hg and 16.2% and 29.4% with HVPG >17 mm Hg, respectively (p=0.015). In the ascites group, the mortality rates at 1 and 2 years were 3.9% and 17.6% with HVPG ≤17 mm Hg and 17.5% and 35.2% with HVPG >17 mm Hg, respectively (p=0.044). Regarding the risk factors for mortality, both HVPG and model for end-stage liver disease were positively related with long-term mortality in all patients. Particularly, for the patients with ascites, both prothrombin time and HVPG were independent risk factors for predicting poor outcomes. Conclusion HVPG is useful for predicting the long-term mortality in patients with decompensated cirrhosis, especially in the presence of ascites. PMID:26632394</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=%22thermodynamics+examples%22&id=EJ717199','ERIC'); return false;" href="https://eric.ed.gov/?q=%22thermodynamics+examples%22&id=EJ717199"><span>Examples for Non-<span class="hlt">Ideal</span> Solution Thermodynamics Study</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>David, Carl W.</p> <p>2004-01-01</p> <p>A mathematical model of a non-<span class="hlt">ideal</span> solution is presented, where it is shown how and where the non-<span class="hlt">ideality</span> manifests itself in the standard thermodynamics tableau. Examples related to the non-<span class="hlt">ideal</span> solution thermodynamics study are also included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27866688','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27866688"><span>Optimal mixing rate in linear solvent strength <span class="hlt">gradient</span> liquid chromatography. Balanced mixing program.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Blumberg, Leonid M; Desmet, Gert</p> <p>2016-12-09</p> <p>The mixing rate (R ϕ ) is the temporal rate of increase in the solvent strength in <span class="hlt">gradient</span> LC. The optimal R ϕ (R ϕ ,Opt ) is the one at which a required peak capacity of <span class="hlt">gradient</span> LC analysis is obtained in the shortest time. The balanced mixing program is a one where, for better separation of early eluting solutes, the mixing ramp is preceded by a balanced isocratic hold of the duration depending on R ϕ . The improvement in the separation of the earlier eluites due to the balanced programming has been evaluated. The value of R ϕ ,Opt depends on the solvent composition range covered by the mixing ramp and on the column <span class="hlt">pressure</span> conditions. The R ϕ ,Opt for a column operating at maximum instrumental <span class="hlt">pressure</span> is different from R ϕ ,Opt for a column operating below the instrumental <span class="hlt">pressure</span> limit. On the other hand, it has been shown that the difference in the R ϕ ,Opt values under different conditions is not very large so that a single default R ϕ previously recommended for <span class="hlt">gradient</span> analyses without the isocratic hold also yields a good approximation to the shortest analysis time for all conditions in the balanced analyses. With or without the initial balance isocratic hold, the recommended default R ϕ is about 5%/t 0 (5% increase in the solvent strength per each t 0 -long increment in time) for small-molecule samples, and about an order of magnitude slower (0.5%/t 0 ) for protein samples. A discussion illustrating the use of the optimization criteria employed here for the techniques other than LSS <span class="hlt">gradient</span> LC is included. Copyright © 2016 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvL.118q3901F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvL.118q3901F"><span><span class="hlt">Ideal</span> Magnetic Dipole Scattering</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Feng, Tianhua; Xu, Yi; Zhang, Wei; Miroshnichenko, Andrey E.</p> <p>2017-04-01</p> <p>We introduce the concept of tunable <span class="hlt">ideal</span> magnetic dipole scattering, where a nonmagnetic nanoparticle scatters light as a pure magnetic dipole. High refractive index subwavelength nanoparticles usually support both electric and magnetic dipole responses. Thus, to achieve <span class="hlt">ideal</span> magnetic dipole scattering one has to suppress the electric dipole response. Such a possibility was recently demonstrated for the so-called anapole mode, which is associated with zero electric dipole scattering. By spectrally overlapping the magnetic dipole resonance with the anapole mode, we achieve <span class="hlt">ideal</span> magnetic dipole scattering in the far field with tunable strong scattering resonances in the near infrared spectrum. We demonstrate that such a condition can be realized at least for two subwavelength geometries. One of them is a core-shell nanosphere consisting of a Au core and silicon shell. It can be also achieved in other geometries, including nanodisks, which are compatible with current nanofabrication technology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JFM...843..244S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JFM...843..244S"><span>Compressible flow at high <span class="hlt">pressure</span> with linear equation of state</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sirignano, William A.</p> <p>2018-05-01</p> <p>Compressible flow varies from <span class="hlt">ideal</span>-gas behavior at high <span class="hlt">pressures</span> where molecular interactions become important. Density is described through a cubic equation of state while enthalpy and sound speed are functions of both temperature and <span class="hlt">pressure</span>, based on two parameters, A and B, related to intermolecular attraction and repulsion, respectively. Assuming small variations from <span class="hlt">ideal</span>-gas behavior, a closed-form solution is obtained that is valid over a wide range of conditions. An expansion in these molecular-interaction parameters simplifies relations for flow variables, elucidating the role of molecular repulsion and attraction in variations from <span class="hlt">ideal</span>-gas behavior. Real-gas modifications in density, enthalpy, and sound speed for a given <span class="hlt">pressure</span> and temperature lead to variations in many basic compressible flow configurations. Sometimes, the variations can be substantial in quantitative or qualitative terms. The new approach is applied to choked-nozzle flow, isentropic flow, nonlinear-wave propagation, and flow across a shock wave, all for the real gas. Modifications are obtained for allowable mass-flow through a choked nozzle, nozzle thrust, sonic wave speed, Riemann invariants, Prandtl's shock relation, and the Rankine-Hugoniot relations. Forced acoustic oscillations can show substantial augmentation of <span class="hlt">pressure</span> amplitudes when real-gas effects are taken into account. Shocks at higher temperatures and <span class="hlt">pressures</span> can have larger <span class="hlt">pressure</span> jumps with real-gas effects. Weak shocks decay to zero strength at sonic speed. The proposed framework can rely on any cubic equation of state and be applied to multicomponent flows or to more-complex flow configurations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/14705056','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/14705056"><span>Momentum-weighted conjugate <span class="hlt">gradient</span> descent algorithm for <span class="hlt">gradient</span> coil optimization.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lu, Hanbing; Jesmanowicz, Andrzej; Li, Shi-Jiang; Hyde, James S</p> <p>2004-01-01</p> <p>MRI <span class="hlt">gradient</span> coil design is a type of nonlinear constrained optimization. A practical problem in transverse <span class="hlt">gradient</span> coil design using the conjugate <span class="hlt">gradient</span> descent (CGD) method is that wire elements move at different rates along orthogonal directions (r, phi, z), and tend to cross, breaking the constraints. A momentum-weighted conjugate <span class="hlt">gradient</span> descent (MW-CGD) method is presented to overcome this problem. This method takes advantage of the efficiency of the CGD method combined with momentum weighting, which is also an intrinsic property of the Levenberg-Marquardt algorithm, to adjust step sizes along the three orthogonal directions. A water-cooled, 12.8 cm inner diameter, three axis torque-balanced <span class="hlt">gradient</span> coil for rat imaging was developed based on this method, with an efficiency of 2.13, 2.08, and 4.12 mT.m(-1).A(-1) along X, Y, and Z, respectively. Experimental data demonstrate that this method can improve efficiency by 40% and field uniformity by 27%. This method has also been applied to the design of a <span class="hlt">gradient</span> coil for the human brain, employing remote current return paths. The benefits of this design include improved <span class="hlt">gradient</span> field uniformity and efficiency, with a shorter length than <span class="hlt">gradient</span> coil designs using coaxial return paths. Copyright 2003 Wiley-Liss, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25984898','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25984898"><span>Association between cumulative social risk and <span class="hlt">ideal</span> cardiovascular health in US adults: NHANES 1999-2006.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Caleyachetty, Rishi; Echouffo-Tcheugui, Justin B; Muennig, Peter; Zhu, Wenyi; Muntner, Paul; Shimbo, Daichi</p> <p>2015-07-15</p> <p>The American Heart Association developed the Life's Simple 7 metric for defining cardiovascular health. Little is known about the association of co-occurring social risk factors on <span class="hlt">ideal</span> cardiovascular health. Using data on 11,467 adults aged ≥25 years from the National Health and Nutrition Examination Survey 1999-2006, we examined the association between cumulative social risk and <span class="hlt">ideal</span> cardiovascular health in US adults. A cumulative risk score (range 0 to 3 or 4) was created by summing four social risk factors (low family income, low education level, minority race, and single-living status). <span class="hlt">Ideal</span> levels for each component in Life's Simple 7 (blood <span class="hlt">pressure</span>, cholesterol, glucose, BMI, smoking, physical activity, and diet) were used to create an <span class="hlt">ideal</span> Life's Simple 7 score [0-1 (low), 2, 3, 4, and 5-7 (high)]. Adults with low income (odds ratio [OR]=0.30 [95% CI 0.23-0.39]), low education [0.22 (0.16-0.28)], who are non-white (0.44 [0.36-0.54]) and single-living [0.79 (0.67-0.95)] were less likely to have 5-7 versus 0 <span class="hlt">ideal</span> Life's Simple 7 scores after adjustment for age and sex. Adults were less likely to attain 5-7 versus 0 <span class="hlt">ideal</span> Life's Simple 7 scores as exposure to the number of social risk factors increased [OR (95% CI) of 0.58 (0.49-0.68); 0.27 (0.21-0.35); and 0.19 (0.14-0.27) for cumulative social risk scores of 1, 2, and 3 or 4, respectively, each versus 0]. US adults with an increasing number of socially risk factors, were progressively less likely to attain <span class="hlt">ideal</span> levels of cardiovascular health factors. Copyright © 2015 Elsevier Ireland Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29245862','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29245862"><span>Non-destructive residual <span class="hlt">pressure</span> self-measurement method for the sensing chip of optical Fabry-Perot <span class="hlt">pressure</span> sensor.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Xue; Wang, Shuang; Jiang, Junfeng; Liu, Kun; Zhang, Xuezhi; Xiao, Mengnan; Xiao, Hai; Liu, Tiegen</p> <p>2017-12-11</p> <p>We introduce a simple residual <span class="hlt">pressure</span> self-measurement method for the Fabry-Perot (F-P) cavity of optical MEMS <span class="hlt">pressure</span> sensor. No extra installation is required and the structure of the sensor is unchanged. In the method, the relationship between residual <span class="hlt">pressure</span> and external <span class="hlt">pressure</span> under the same diaphragm deflection condition at different temperatures is analyzed by using the deflection formula of the circular plate with clamped edges and the <span class="hlt">ideal</span> gas law. Based on this, the residual <span class="hlt">pressure</span> under the flat condition can be obtained by <span class="hlt">pressure</span> scanning process and calculation process. We carried out the experiment to compare the residual <span class="hlt">pressures</span> of two batches MEMS sensors fabricated by two kinds of bonding process. The measurement result indicates that our approach is reliable enough for the measurement.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1850c0030K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1850c0030K"><span><span class="hlt">Ideal</span> heat transfer conditions for tubular solar receivers with different design constraints</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, Jin-Soo; Potter, Daniel; Gardner, Wilson; Too, Yen Chean Soo; Padilla, Ricardo Vasquez</p> <p>2017-06-01</p> <p>The optimum heat transfer condition for a tubular type solar receiver was investigated for various receiver pipe size, heat transfer fluid, and design requirement and constraint(s). Heat transfer of a single plain receiver pipe exposed to concentrated solar energy was modelled along the flow path of the heat transfer fluid. Three different working fluids, molten salt, sodium, and supercritical carbon dioxide (sCO2) were considered in the case studies with different design conditions. The optimized <span class="hlt">ideal</span> heat transfer condition was identified through fast iterative heat transfer calculations solving for all relevant radiation, conduction and convection heat transfers throughout the entire discretized tubular receiver. The <span class="hlt">ideal</span> condition giving the best performance was obtained by finding the highest acceptable solar energy flux optimally distributed to meet different constraint(s), such as maximum allowable material temperature of receiver, maximum allowable film temperature of heat transfer fluid, and maximum allowable stress of receiver pipe material. The level of fluid side turbulence (represented by <span class="hlt">pressure</span> drop in this study) was also optimized to give the highest net power production. As the outcome of the study gives information on the most <span class="hlt">ideal</span> heat transfer condition, it can be used as a useful guideline for optimal design of a real receiver and solar field in a combined manner. The <span class="hlt">ideal</span> heat transfer condition is especially important for high temperature tubular receivers (e.g. for supplying heat to high efficiency Brayton cycle turbines) where the system design and performance is tightly constrained by the receiver pipe material strength.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28026771','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28026771"><span>Prescribed Velocity <span class="hlt">Gradients</span> for Highly Viscous SPH Fluids with Vorticity Diffusion.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Peer, Andreas; Teschner, Matthias</p> <p>2017-12-01</p> <p>Working with prescribed velocity <span class="hlt">gradients</span> is a promising approach to efficiently and robustly simulate highly viscous SPH fluids. Such approaches allow to explicitly and independently process shear rate, spin, and expansion rate. This can be used to, e.g., avoid interferences between <span class="hlt">pressure</span> and viscosity solvers. Another interesting aspect is the possibility to explicitly process the vorticity, e.g., to preserve the vorticity. In this context, this paper proposes a novel variant of the prescribed-<span class="hlt">gradient</span> idea that handles vorticity in a physically motivated way. In contrast to a less appropriate vorticity preservation that has been used in a previous approach, vorticity is diffused. The paper illustrates the utility of the vorticity diffusion. Therefore, comparisons of the proposed vorticity diffusion with vorticity preservation and additionally with vorticity damping are presented. The paper further discusses the relation between prescribed velocity <span class="hlt">gradients</span> and prescribed velocity Laplacians which improves the intuition behind the prescribed-<span class="hlt">gradient</span> method for highly viscous SPH fluids. Finally, the paper discusses the relation of the proposed method to a physically correct implicit viscosity formulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000HyPr...14..155C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000HyPr...14..155C"><span>Influence of aspect and slope <span class="hlt">gradient</span> on hydraulic conductivity measured by tension infiltrometer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Casanova, Manuel; Messing, Ingmar; Joel, Abraham</p> <p>2000-01-01</p> <p>A tension infiltrometer technique was used to characterize differences in hydraulic conductivity (K) in two rain-fed hillsides (north-facing and south-facing) in central Chile. For the north-facing locations, smaller values of K (at a range of supply water <span class="hlt">pressure</span> heads ) compared with south-facing locations were found, with accentuated differences close to saturation (zero <span class="hlt">pressure</span> head). The differences were attributed to differences in texture and organic matter contents observed for the two sites. Furthermore, K() had a tendency to increase with increasing slope <span class="hlt">gradient</span>. This tendency was to an extent explained by the deviation from requirements of measurements on level ground. The differences found in K() between different slope <span class="hlt">gradients</span> were explained by the differences in the vertical and lateral hydraulic conductivity and by the occurrence of surface sealing in low slope plots.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040088758&hterms=APICAL&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DAPICAL','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040088758&hterms=APICAL&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DAPICAL"><span>Relationship between early diastolic intraventricular <span class="hlt">pressure</span> <span class="hlt">gradients</span>, an index of elastic recoil, and improvements in systolic and diastolic function</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Firstenberg, M. S.; Smedira, N. G.; Greenberg, N. L.; Prior, D. L.; McCarthy, P. M.; Garcia, M. J.; Thomas, J. D.</p> <p>2001-01-01</p> <p>BACKGROUND: Early diastolic intraventricular <span class="hlt">pressure</span> <span class="hlt">gradients</span> (IVPGs) have been proposed to relate to left ventricular (LV) elastic recoil and early ventricular "suction." Animal studies have demonstrated relationships between IVPGs and systolic and diastolic indices during acute ischemia. However, data on the effects of improvements in LV function in humans and the relationship to IVPGs are lacking. METHODS AND RESULTS: Eight patients undergoing CABG and/or infarct exclusion surgery had a triple-sensor high-fidelity catheter placed across the mitral valve intraoperatively for simultaneous recording of left atrial (LA), basal LV, and apical LV <span class="hlt">pressures</span>. Hemodynamic data obtained before bypass were compared with those with similar LA <span class="hlt">pressures</span> and heart rates obtained after bypass. From each LV waveform, the time constant of LV relaxation (tau), +dP/dt(max), and -dP/dt(max) were determined. Transesophageal echocardiography was used to determined end-diastolic (EDV) and end-systolic (ESV) volumes and ejection fractions (EF). At similar LA <span class="hlt">pressures</span> and heart rates, IVPG increased after bypass (before bypass 1.64+/-0.79 mm Hg; after bypass 2.67+/-1.25 mm Hg; P<0.01). Significant improvements were observed in ESV, as well as in apical and basal +dP/dt(max), -dP/dt(max), and tau (each P<0.05). Overall, IVPGs correlated inversely with both ESV (IVPG=-0.027[ESV]+3.46, r=-0.64) and EDV (IVPG=-0.027[EDV]+4.30, r=-0.70). Improvements in IVPGs correlated with improvements in apical tau (Deltatau =5.93[DeltaIVPG]+4.76, r=0.91) and basal tau (Deltatau =2.41[DeltaIVPG]+5.13, r=-0.67). Relative changes in IVPGs correlated with changes in ESV (DeltaESV=-0.97[%DeltaIVPG]+23.34, r=-0.79), EDV (DeltaEDV=-1.16[%DeltaIVPG]+34.92, r=-0.84), and EF (DeltaEF=0.38[%DeltaIVPG]-8.39, r=0.85). CONCLUSIONS: Improvements in LV function also increase IVPGs. These changes in IVPGs, suggestive of increases in LV suction and elastic recoil, correlate directly with improvements in LV relaxation</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/2000753','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/2000753"><span>Noninvasive estimation of left atrial <span class="hlt">pressure</span> in patients with congestive heart failure and mitral regurgitation by Doppler echocardiography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gorcsan, J; Snow, F R; Paulsen, W; Nixon, J V</p> <p>1991-03-01</p> <p>A completely noninvasive method for estimating left atrial <span class="hlt">pressure</span> in patients with congestive heart failure and mitral regurgitation has been devised with the use of continuous-wave Doppler echocardiography and brachial sphygmomanometry. Of 46 patients studied with mitral regurgitation, 35 (76%) had jets with distinct Doppler spectral envelopes recorded. The peak ventriculoatrial <span class="hlt">gradient</span> was obtained by measuring peak mitral regurgitant velocity in systole and using the modified Bernoulli equation. This <span class="hlt">gradient</span> was then subtracted from peak brachial systolic blood <span class="hlt">pressure</span>, an estimate of left ventricular systolic <span class="hlt">pressure</span>, to yield left atrial <span class="hlt">pressure</span> (left atrial <span class="hlt">pressure</span> = systolic blood <span class="hlt">pressure</span> - mitral regurgitant <span class="hlt">pressure</span> <span class="hlt">gradient</span>). Noninvasive estimates of left atrial <span class="hlt">pressure</span> from 35 patients were plotted against simultaneous recordings of mean pulmonary capillary wedge <span class="hlt">pressure</span> resulting in the correlation y = 0.88x + 3.3, r = 0.88, standard error of estimate = +/- 4 mm Hg (p less than 0.001). Therefore, continuous-wave Doppler echocardiography and sphygmomanometry may be used in selected patients with congestive heart failure and mitral regurgitation for noninvasive estimation of left atrial <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27585698','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27585698"><span><span class="hlt">Ideal</span> Cardiovascular Health and Subclinical Markers of Carotid Structure and Function: The Paris Prospective Study III.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gaye, Bamba; Mustafic, Hazrije; Laurent, Stéphane; Perier, Marie-Cécile; Thomas, Frédérique; Guibout, Catherine; Tafflet, Muriel; Pannier, Bruno; Boutouyrie, Pierre; Jouven, Xavier; Empana, Jean-Philippe</p> <p>2016-10-01</p> <p>We hypothesized that subclinical markers of vascular structure and function, which are independent predictors of cardiovascular disease, would be less frequent in subjects with <span class="hlt">ideal</span> than poor cardiovascular health (CVH) as defined by the American Heart Association (AHA). Carotid parameters were measured using high-precision echotracking device in 9155 nonreferred participants attending a health checkup in a large health center in Paris (France) between 2008 and 2012. According to the AHA, participants with 0 to 2, 3 to 4, and 5 to 7 metrics (smoking, physical activity, body mass index, diet, blood glucose and total cholesterol, blood <span class="hlt">pressure</span>) at the <span class="hlt">ideal</span> level were categorized as having poor, intermediate, and <span class="hlt">ideal</span> CVH. Carotid parameters were dichotomized according to their median value, and multivariable logistic regression analysis was performed. Mean age was 59.5 (SD 6.3) years; 39% were females, and <span class="hlt">ideal</span> CVH was present in 10.11% of the study participants. After adjustment for age, sex, education, and living alone and compared with a poor CVH, an <span class="hlt">ideal</span> CVH was associated with lower common carotid artery intima-media thickness (odds ratio=1.64; 95% confidence interval 1.40, 1.93), absence of carotid plaques (odds ratio=2.14; 95% confidence interval 1.60, 2.87), lower Young's elastic modulus (odds ratio=2.43; 95% confidence interval 2.07, 2.84), and higher carotid distensibility coefficient (odds ratio=2.90; 95% confidence interval 2.47, 3.41). In community subjects aged 50 to 75 years, <span class="hlt">ideal</span> CVH was associated with substantially less arterial stiffness and thickness. These associations might contribute to the lower risk of cardiovascular diseases in subjects with <span class="hlt">ideal</span> CVH. © 2016 American Heart Association, Inc.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_20 --> <div id="page_21" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="401"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010071251','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010071251"><span>A Performance Map for <span class="hlt">Ideal</span> Air Breathing Pulse Detonation Engines</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Paxson, Daniel E.</p> <p>2001-01-01</p> <p>The performance of an <span class="hlt">ideal</span>, air breathing Pulse Detonation Engine is described in a manner that is useful for application studies (e.g., as a stand-alone, propulsion system, in combined cycles, or in hybrid turbomachinery cycles). It is shown that the Pulse Detonation Engine may be characterized by an averaged total <span class="hlt">pressure</span> ratio, which is a unique function of the inlet temperature, the fraction of the inlet flow containing a reacting mixture, and the stoichiometry of the mixture. The inlet temperature and stoichiometry (equivalence ratio) may in turn be combined to form a nondimensional heat addition parameter. For each value of this parameter, the average total enthalpy ratio and total <span class="hlt">pressure</span> ratio across the device are functions of only the reactant fill fraction. Performance over the entire operating envelope can thus be presented on a single plot of total <span class="hlt">pressure</span> ratio versus total enthalpy ratio for families of the heat addition parameter. Total <span class="hlt">pressure</span> ratios are derived from thrust calculations obtained from an experimentally validated, reactive Euler code capable of computing complete Pulse Detonation Engine limit cycles. Results are presented which demonstrate the utility of the described method for assessing performance of the Pulse Detonation Engine in several potential applications. Limitations and assumptions of the analysis are discussed. Details of the particular detonative cycle used for the computations are described.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26754123','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26754123"><span>Trends in <span class="hlt">Ideal</span> Cardiovascular Health Metrics Among Employees of a Large Healthcare Organization (from the Baptist Health South Florida Employee Study).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ogunmoroti, Oluseye; Utuama, Ovie; Spatz, Erica S; Rouseff, Maribeth; Parris, Don; Das, Sankalp; Younus, Adnan; Guzman, Henry; Tran, Thinh; Agatston, Arthur; Feldman, Theodore; Virani, Salim S; Maziak, Wasim; Veledar, Emir; Nasir, Khurram</p> <p>2016-03-01</p> <p>The American Heart Association (AHA)'s 2020 goal is to improve the cardiovascular health (CVH) of people living in the United States (US) by 20% and reduce mortality from cardiovascular diseases and stroke by 20%. Given that 155 million adults are in the US workforce, and >60% have employee-based insurance, workplace studies provide an important opportunity to assess and potentially advance CVH through the use of comprehensive workplace wellness programs. Among a cohort of employees of the Baptist Health System, CVH was assessed annually during voluntary health fairs and health risk assessments (HRA) from 2011 to 2014 using the AHA's 7 CVH metrics: smoking, body mass index (BMI), physical activity, diet, blood <span class="hlt">pressure</span>, total cholesterol, and blood glucose. Each metric was categorized as <span class="hlt">ideal</span>, intermediate, or poor according to the AHA criteria. Cochrane-Armitage test was used to detect trends in CVH by year. <span class="hlt">Ideal</span> CVH, defined as meeting <span class="hlt">ideal</span> criteria for all 7 metrics, was assessed and compared across years. The overall cohort was 34,746 with 4,895 employees in 2011, 10,724 in 2012, 9,763 in 2013, and 9,364 in 2014. Mean age (SD) was between 43 (±12) and 46 years (±12). Female to male ratio was 3:1. The prevalence of study participants who met the <span class="hlt">ideal</span> criteria for diet, physical activity, and blood <span class="hlt">pressure</span> increased significantly from 2011 to 2014 but for BMI, total cholesterol, and blood glucose, a significant decrease was noticed. In addition, the prevalence of study participants in <span class="hlt">ideal</span> CVH although low, increased significantly over time (0.3% to 0.6%, p <0.0001). In conclusion, this study shows the trends of the AHA's CVH metrics in a large health care organization. The positive findings noted for the metrics of smoking, physical activity, total cholesterol, and blood glucose should be reinforced. However, the metrics of diet, BMI, and blood <span class="hlt">pressure</span> need more attention. Copyright © 2016 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28597898','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28597898"><span>Maxwell-Stefan diffusion coefficient estimation for ternary systems: an <span class="hlt">ideal</span> ternary alcohol system.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Allie-Ebrahim, Tariq; Zhu, Qingyu; Bräuer, Pierre; Moggridge, Geoff D; D'Agostino, Carmine</p> <p>2017-06-21</p> <p>The Maxwell-Stefan model is a popular diffusion model originally developed to model diffusion of gases, which can be considered thermodynamically <span class="hlt">ideal</span> mixtures, although its application has been extended to model diffusion in non-<span class="hlt">ideal</span> liquid mixtures as well. A drawback of the model is that it requires the Maxwell-Stefan diffusion coefficients, which are not based on measurable quantities but they have to be estimated. As a result, numerous estimation methods, such as the Darken model, have been proposed to estimate these diffusion coefficients. However, the Darken model was derived, and is only well defined, for binary systems. This model has been extended to ternary systems according to two proposed forms, one by R. Krishna and J. M. van Baten, Ind. Eng. Chem. Res., 2005, 44, 6939-6947 and the other by X. Liu, T. J. H. Vlugt and A. Bardow, Ind. Eng. Chem. Res., 2011, 50, 10350-10358. In this paper, the two forms have been analysed against the <span class="hlt">ideal</span> ternary system of methanol/butan-1-ol/propan-1-ol and using experimental values of self-diffusion coefficients. In particular, using pulsed <span class="hlt">gradient</span> stimulated echo nuclear magnetic resonance (PGSTE-NMR) we have measured the self-diffusion coefficients in various methanol/butan-1-ol/propan-1-ol mixtures. The experimental values of self-diffusion coefficients were then used as the input data required for the Darken model. The predictions of the two proposed multicomponent forms of this model were then compared to experimental values of mutual diffusion coefficients for the <span class="hlt">ideal</span> alcohol ternary system. This experimental-based approach showed that the Liu's model gives better predictions compared to that of Krishna and van Baten, although it was only accurate to within 26%. Nonetheless, the multicomponent Darken model in conjunction with self-diffusion measurements from PGSTE-NMR represents an attractive method for a rapid estimation of mutual diffusion in multicomponent systems, especially when compared to exhaustive</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1345540-models-sol-transport-relation-scaling-divertor-heat-flux-width-diii','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1345540-models-sol-transport-relation-scaling-divertor-heat-flux-width-diii"><span>Models of SOL transport and their relation to scaling of the divertor heat flux width in DIII-D</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Makowski, M. A.; Lasnier, C. J.; Leonard, A. W.; ...</p> <p>2014-10-06</p> <p>Strong support for the critical <span class="hlt">pressure</span> <span class="hlt">gradient</span> model for the heat flux width has been obtained, in that the measured separatrix <span class="hlt">pressure</span> <span class="hlt">gradient</span> lies below and scales similarly to the <span class="hlt">pressure</span> <span class="hlt">gradient</span> limit obtained from the <span class="hlt">ideal</span>, infinite-n stability codes, BALOO and 2DX, in all cases that have been examined. Predictions of a heuristic drift model for the heat flux width are also in qualitative agreement with the measurements. We obtained these results by using an improved high rep-rate and higher edge spatial resolution Thomson scattering system on DIII-D to measure the upstream electron temperature and density profiles. In ordermore » to compare theory and experiment, profiles of density, temperature, and <span class="hlt">pressure</span> for both electrons and ions are needed as well values of these quantitities at the separatrix. We also developed a simple method to identify a proxy for the separatrix.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22599996-causal-relation-between-turbulent-particle-flux-density-gradient','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22599996-causal-relation-between-turbulent-particle-flux-density-gradient"><span>The causal relation between turbulent particle flux and density <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Milligen, B. Ph. van; Martín de Aguilera, A.; Hidalgo, C.</p> <p></p> <p>A technique for detecting the causal relationship between fluctuating signals is used to investigate the relation between flux and <span class="hlt">gradient</span> in fusion plasmas. Both a resistive <span class="hlt">pressure</span> <span class="hlt">gradient</span> driven turbulence model and experimental Langmuir probe data from the TJ-II stellarator are studied. It is found that the maximum influence occurs at a finite time lag (non-instantaneous response) and that quasi-periodicities exist. Furthermore, the model results show very long range radial influences, extending over most of the investigated regions, possibly related to coupling effects associated with plasma self-organization. These results clearly show that transport in fusion plasmas is not local andmore » instantaneous, as is sometimes assumed.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005PhDT.......141M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005PhDT.......141M"><span>High-<span class="hlt">pressure</span> nuclear magnetic resonance studies of fuel cell membranes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mananga, Eugene Stephane</p> <p></p> <p>This thesis focuses on the use of high <span class="hlt">pressure</span> NMR to study transport properties in electrolyte membranes used for fuel cells. The main concern is in studying the self-diffusion coefficients of ions and molecules in membranes and solutions, which can be used to characterize electrolytes in fuel cells. For this purpose, a high-<span class="hlt">pressure</span> fringe field NMR method to study transport properties in material systems useful for fuel cell and battery electrolytes, was designed, developed, and implemented. In this investigation, <span class="hlt">pressure</span> is the thermodynamic variable to obtain additional information about the ionic transport process, which could yield the crucial parameter, activation volume. Most of the work involves proton NMR, with additional investigations of others nuclei, such as fluorine, phosphorus and lithium. Using the FFG method, two fuel cell membrane types (NAFION-117, SPTES), and different dilutions of phosphoric acid were investigated, as was LiTf salt in Diglyme solution, which is used as a lithium battery electrolyte. In addition to high-<span class="hlt">pressure</span> NMR diffusion measurements carried out in the fringe field <span class="hlt">gradient</span> for the investigation of SPTES, pulse field <span class="hlt">gradient</span> spin echo NMR was also used to characterize the water diffusion, in addition to measuring diffusion rates as a function of temperature. This second method allows us to measure distinct diffusion coefficients in cases where the different nuclear (proton) environments can be resolved in the NMR spectrum. Polymer electrolyte systems, in which the mobility of both cations and anions is probed by NMR self-diffusion measurements using standard pulsed field <span class="hlt">gradient</span> methods and static <span class="hlt">gradient</span> measurements as a function of applied hydrostatic <span class="hlt">pressure</span>, were also investigated. The material investigated is the low molecular weight liquid diglyme/LiCF3SO3 (LiTf) complexes which can be used as electrolytes in lithium batteries. Finally, high-<span class="hlt">pressure</span> diffusion coefficient measurements of phosphoric acid in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4061707','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4061707"><span>Improved Classification of Mammograms Following <span class="hlt">Idealized</span> Training</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Hornsby, Adam N.; Love, Bradley C.</p> <p>2014-01-01</p> <p>People often make decisions by stochastically retrieving a small set of relevant memories. This limited retrieval implies that human performance can be improved by training on <span class="hlt">idealized</span> category distributions (Giguère & Love, 2013). Here, we evaluate whether the benefits of <span class="hlt">idealized</span> training extend to categorization of real-world stimuli, namely classifying mammograms as normal or tumorous. Participants in the <span class="hlt">idealized</span> condition were trained exclusively on items that, according to a norming study, were relatively unambiguous. Participants in the actual condition were trained on a representative range of items. Despite being exclusively trained on easy items, <span class="hlt">idealized</span>-condition participants were more accurate than those in the actual condition when tested on a range of item types. However, <span class="hlt">idealized</span> participants experienced difficulties when test items were very dissimilar from training cases. The benefits of <span class="hlt">idealization</span>, attributable to reducing noise arising from cognitive limitations in memory retrieval, suggest ways to improve real-world decision making. PMID:24955325</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24955325','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24955325"><span>Improved Classification of Mammograms Following <span class="hlt">Idealized</span> Training.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hornsby, Adam N; Love, Bradley C</p> <p>2014-06-01</p> <p>People often make decisions by stochastically retrieving a small set of relevant memories. This limited retrieval implies that human performance can be improved by training on <span class="hlt">idealized</span> category distributions (Giguère & Love, 2013). Here, we evaluate whether the benefits of <span class="hlt">idealized</span> training extend to categorization of real-world stimuli, namely classifying mammograms as normal or tumorous. Participants in the <span class="hlt">idealized</span> condition were trained exclusively on items that, according to a norming study, were relatively unambiguous. Participants in the actual condition were trained on a representative range of items. Despite being exclusively trained on easy items, <span class="hlt">idealized</span>-condition participants were more accurate than those in the actual condition when tested on a range of item types. However, <span class="hlt">idealized</span> participants experienced difficulties when test items were very dissimilar from training cases. The benefits of <span class="hlt">idealization</span>, attributable to reducing noise arising from cognitive limitations in memory retrieval, suggest ways to improve real-world decision making.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014HMT....50..737Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014HMT....50..737Y"><span>Experimental investigation on circumferential and axial temperature <span class="hlt">gradient</span> over fuel channel under LOCA</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yadav, Ashwini Kumar; kumar, Ravi; Gupta, Akhilesh; Chatterjee, Barun; Mukhopadhyay, Deb; Lele, H. G.</p> <p>2014-06-01</p> <p>In a nuclear reactor temperature rises drastically in fuel channels under loss of coolant accident due to failure of primary heat transportation system. Present investigation has been carried out to capture circumferential and axial temperature <span class="hlt">gradients</span> during fully and partially voiding conditions in a fuel channel using 19 pin fuel element simulator. A series of experiments were carried out by supplying power to outer, middle and center rods of 19 pin fuel simulator in ratio of 1.4:1.1:1. The temperature at upper periphery of <span class="hlt">pressure</span> tube (PT) was slightly higher than at bottom due to increase in local equivalent thermal conductivity from top to bottom of PT. To simulate fully voided conditions PT was <span class="hlt">pressurized</span> at 2.0 MPa <span class="hlt">pressure</span> with 17.5 kW power injection. Ballooning initiated from center and then propagates towards the ends and hence axial temperature difference has been observed along the length of PT. For asymmetric heating, upper eight rods of fuel simulator were activated and temperature difference up-to 250 °C has been observed from top to bottom periphery of PT. Such situation creates steep circumferential temperature <span class="hlt">gradient</span> over PT and could lead to breaching of PT under high <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920034389&hterms=BALANCE+SHEET&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DBALANCE%2BSHEET','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920034389&hterms=BALANCE+SHEET&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DBALANCE%2BSHEET"><span><span class="hlt">Pressure</span> anisotropy and radial stress balance in the Jovian neutral sheet</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Paranicas, C. P.; Mauk, B. H.; Krimigis, S. M.</p> <p>1991-01-01</p> <p>By examining particle and magnetic field data from the Voyager 1 and 2 spacecraft, signatures were found indicating that the (greater than about 28 keV) particle <span class="hlt">pressure</span> parallel to the magnetic field is greater than the <span class="hlt">pressure</span> perpendicular to the field within the nightside neutral sheet (three nightside neutral sheet crossings, with favorable experimental conditions, were used). By incorporating the <span class="hlt">pressure</span> anisotropy into the calculation of radial forces within the hightside neutral sheet, it is found that (1) force balance is approximately achieved and (2) the anisotropy force term provides the largest contribution of the other particle forces considered (<span class="hlt">pressure</span> <span class="hlt">gradients</span> and the corotation centrifugal force). With regard to the problem of understanding the balance of radial forces within the dayside neutral sheet (McNutt, 1984; Mauk and Krimigis, 1987), the nightside <span class="hlt">pressure</span> anisotropy force is larger than the dayside <span class="hlt">pressure</span> <span class="hlt">gradient</span> forces at equivalent radial distances; however, a full accounting of the dayside regions remains to be achieved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EJPh...38a4002D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EJPh...38a4002D"><span>An <span class="hlt">ideal</span> free-kick</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>De Luca, R.; Faella, O.</p> <p>2017-01-01</p> <p>The kinematics of a free-kick is studied. As in projectile motion, the free-kick is <span class="hlt">ideal</span> since we assume that a point-like ball moves in the absence of air resistance. We have experienced the fortunate conjuncture of a classical mechanics lecture taught right before an important football game. These types of sports events might trigger a great deal of attention from the classroom. The <span class="hlt">idealized</span> problem is devised in such a way that students are eager to come to the end of the whole story.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28009240','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28009240"><span>Venous sinus stenting for reduction of intracranial <span class="hlt">pressure</span> in IIH: a prospective pilot study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Kenneth C; Starke, Robert M; Durst, Christopher R; Wang, Tony R; Ding, Dale; Crowley, R Webster; Newman, Steven A</p> <p>2017-11-01</p> <p>OBJECTIVE Idiopathic intracranial hypertension (IIH) may cause blindness due to elevated intracranial <span class="hlt">pressure</span> (ICP). Venous sinus stenosis has been identified in select patients, leading to stenting as a potential treatment, but its effects on global ICP have not been completely defined. The purpose of this pilot study was to assess the effects of venous sinus stenting on ICP in a small group of patients with IIH. METHODS Ten patients for whom medical therapy had failed were prospectively followed. Ophthalmological examinations were assessed, and patients with venous sinus stenosis on MR angiography proceeded to catheter angiography, venography with assessment of <span class="hlt">pressure</span> <span class="hlt">gradient</span>, and ICP monitoring. Patients with elevated ICP measurements and an elevated <span class="hlt">pressure</span> <span class="hlt">gradient</span> across the stenosis were treated with stent placement. RESULTS All patients had elevated venous <span class="hlt">pressure</span> (mean 39.5 ± 14.9 mm Hg), an elevated <span class="hlt">gradient</span> across the venous sinus stenosis (30.0 ± 13.2 mm Hg), and elevated ICP (42.2 ± 15.9 mm Hg). Following stent placement, all patients had resolution of the stenosis and <span class="hlt">gradient</span> (1 ± 1 mm Hg). The ICP values showed an immediate decrease (to a mean of 17.0 ± 8.3 mm Hg), and further decreased overnight (to a mean of 8 ± 4.2 mm Hg). All patients had subjective and objective improvement, and all but one improved during follow-up (median 23.4 months; range 15.7-31.6 months). Two patients developed stent-adjacent stenosis; retreatment abolished the stenosis and <span class="hlt">gradient</span> in both cases. Patients presenting with papilledema had resolution on follow-up funduscopic imaging and optical coherence tomography (OCT) and improvement on visual field testing. Patients presenting with optic atrophy had optic nerve thinning on follow-up OCT, but improved visual fields. CONCLUSIONS For selected patients with IIH and venous sinus stenosis with an elevated <span class="hlt">pressure</span> <span class="hlt">gradient</span> and elevated ICP, venous sinus stenting results in resolution of the venous <span class="hlt">pressure</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910000032&hterms=fermentation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dfermentation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910000032&hterms=fermentation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dfermentation"><span>Membrane Bioreactor With <span class="hlt">Pressure</span> Cycle</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Efthymiou, George S.; Shuler, Michael L.</p> <p>1991-01-01</p> <p>Improved class of multilayer membrane bioreactors uses convention forced by differences in <span class="hlt">pressure</span> to overcome some of diffusional limitations of prior bioreactors. In reactor of new class, flow of nutrient solution reduces adverse <span class="hlt">gradients</span> of concentration, keeps cells supplied with fresh nutrient, and sweeps away products faster than diffusion alone. As result, overall yield and rate of reaction increased. <span class="hlt">Pressures</span> in sweeping gas and nutrient alternated to force nutrient liquid into and out of biocatalyst layer through hyrophilic membrane.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050182917','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050182917"><span>On controlling nonlinear dissipation in high order filter methods for <span class="hlt">ideal</span> and non-<span class="hlt">ideal</span> MHD</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yee, H. C.; Sjogreen, B.</p> <p>2004-01-01</p> <p>The newly developed adaptive numerical dissipation control in spatially high order filter schemes for the compressible Euler and Navier-Stokes equations has been recently extended to the <span class="hlt">ideal</span> and non-<span class="hlt">ideal</span> magnetohydrodynamics (MHD) equations. These filter schemes are applicable to complex unsteady MHD high-speed shock/shear/turbulence problems. They also provide a natural and efficient way for the minimization of Div(B) numerical error. The adaptive numerical dissipation mechanism consists of automatic detection of different flow features as distinct sensors to signal the appropriate type and amount of numerical dissipation/filter where needed and leave the rest of the region free from numerical dissipation contamination. The numerical dissipation considered consists of high order linear dissipation for the suppression of high frequency oscillation and the nonlinear dissipative portion of high-resolution shock-capturing methods for discontinuity capturing. The applicable nonlinear dissipative portion of high-resolution shock-capturing methods is very general. The objective of this paper is to investigate the performance of three commonly used types of nonlinear numerical dissipation for both the <span class="hlt">ideal</span> and non-<span class="hlt">ideal</span> MHD.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MS%26E..311a2013A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MS%26E..311a2013A"><span><span class="hlt">Ideal</span> flow theory for the double - shearing model as a basis for metal forming design</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Alexandrov, S.; Trung, N. T.</p> <p>2018-02-01</p> <p>In the case of Tresca’ solids (i.e. solids obeying the Tresca yield criterion and its associated flow rule) <span class="hlt">ideal</span> flows have been defined elsewhere as solenoidal smooth deformations in which an eigenvector field associated everywhere with the greatest principal stress (and strain rate) is fixed in the material. Under such conditions all material elements undergo paths of minimum plastic work, a condition which is often advantageous for metal forming processes. Therefore, the <span class="hlt">ideal</span> flow theory is used as the basis of a procedure for the preliminary design of such processes. The present paper extends the theory of stationary planar <span class="hlt">ideal</span> flow to <span class="hlt">pressure</span> dependent materials obeying the double shearing model and the double slip and rotation model. It is shown that the original problem of plasticity reduces to a purely geometric problem. The corresponding system of equations is hyperbolic. The characteristic relations are integrated in elementary functions. In regions where one family of characteristics is straight, mapping between the principal lines and Cartesian coordinates is determined by linear ordinary differential equations. An illustrative example is provided.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27119471','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27119471"><span><span class="hlt">Pressure</span> profiles of sport compression stockings.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Reich-Schupke, Stefanie; Surhoff, Stefan; Stücker, Markus</p> <p>2016-05-01</p> <p>While sport compression stockings (SCS) have become increasingly popular, there is no regulatory norm as exists for medical compression stockings (MCS). The objective of this pilot study was to compare five SCS with respect to their <span class="hlt">pressure</span> profiles ex vivo and in vivo, and in relation to German standards for MCS (RAL norm). In vivo (10 competitive athletes; standardized procedure using the Kikuhime <span class="hlt">pressure</span> monitor) and ex vivo (tested at the Hohenstein Institute) <span class="hlt">pressure</span> profiles were tested for the following products: CEP Running Progressive Socks, Falke Running Energizing, Sigvaris Performance, X-Socks Speed Metal Energizer, and 2XU Compression Race Socks. Ex vivo ankle <span class="hlt">pressures</span> of CEP (25.6 mmHg) and 2XU (23.2 mmHg) corresponded to class 2 MCS; that of Sigvaris (20.8 mmHg), to class 1 MCS. The remaining SCS achieved lower <span class="hlt">pressure</span> values. The <span class="hlt">pressure</span> <span class="hlt">gradients</span> showed marked differences, and did not meet MCS standards. Average in vivo <span class="hlt">pressures</span> were higher for 2XU, CEP, and Sigvaris than for Falke and X-Socks. However, in vivo values for all SCS were below those of class 1 MCS. None of the SCS showed the decreasing <span class="hlt">pressure</span> <span class="hlt">gradient</span> (from distal to proximal) required for MCS. In vivo and ex vivo <span class="hlt">pressure</span> profiles of all SCS examined showed marked heterogeneity, and did not meet MCS standards. Consequently, the clinical and practical effects of SCS cannot be compared, either. It would therefore be desirable to establish a classification that allows for the categorization and comparison of various SCS as well as their selection based on individual preferences and needs (high vs. low <span class="hlt">pressure</span>, progressive vs. degressive profile). © 2016 Deutsche Dermatologische Gesellschaft (DDG). Published by John Wiley & Sons Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=vitamin+AND+c&id=EJ949386','ERIC'); return false;" href="https://eric.ed.gov/?q=vitamin+AND+c&id=EJ949386"><span>Recharging Our Sense of <span class="hlt">Idealism</span>: Concluding Thoughts</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>D'Andrea, Michael; Dollarhide, Colette T.</p> <p>2011-01-01</p> <p>In this article, the authors aim to recharge one's sense of <span class="hlt">idealism</span>. They argue that <span class="hlt">idealism</span> is the Vitamin C that sustains one's commitment to implementing humanistic principles and social justice practices in the work of counselors and educators. The <span class="hlt">idealism</span> that characterizes counselors and educators who are humanistic and social justice…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27718544','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27718544"><span>Salinity <span class="hlt">Gradients</span> for Sustainable Energy: Primer, Progress, and Prospects.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yip, Ngai Yin; Brogioli, Doriano; Hamelers, Hubertus V M; Nijmeijer, Kitty</p> <p>2016-11-15</p> <p>Combining two solutions of different composition releases the Gibbs free energy of mixing. By using engineered processes to control the mixing, chemical energy stored in salinity <span class="hlt">gradients</span> can be harnessed for useful work. In this critical review, we present an overview of the current progress in salinity <span class="hlt">gradient</span> power generation, discuss the prospects and challenges of the foremost technologies - <span class="hlt">pressure</span> retarded osmosis (PRO), reverse electrodialysis (RED), and capacitive mixing (CapMix) and provide perspectives on the outlook of salinity <span class="hlt">gradient</span> power generation. Momentous strides have been made in technical development of salinity <span class="hlt">gradient</span> technologies and field demonstrations with natural and anthropogenic salinity <span class="hlt">gradients</span> (for example, seawater-river water and desalination brine-wastewater, respectively), but fouling persists to be a pivotal operational challenge that can significantly ebb away cost-competitiveness. Natural hypersaline sources (e.g., hypersaline lakes and salt domes) can achieve greater concentration difference and, thus, offer opportunities to overcome some of the limitations inherent to seawater-river water. Technological advances needed to fully exploit the larger salinity <span class="hlt">gradients</span> are identified. While seawater desalination brine is a seemingly attractive high salinity anthropogenic stream that is otherwise wasted, actual feasibility hinges on the appropriate pairing with a suitable low salinity stream. Engineered solutions are foulant-free and can be thermally regenerative for application in low-temperature heat utilization. Alternatively, PRO, RED, and CapMix can be coupled with their analog separation process (reverse osmosis, electrodialysis, and capacitive deionization, respectively) in salinity <span class="hlt">gradient</span> flow batteries for energy storage in chemical potential of the engineered solutions. Rigorous techno-economic assessments can more clearly identify the prospects of low-grade heat conversion and large-scale energy storage</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvE..97c3204S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvE..97c3204S"><span>Fully kinetic Biermann battery and associated generation of <span class="hlt">pressure</span> anisotropy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schoeffler, K. M.; Loureiro, N. F.; Silva, L. O.</p> <p>2018-03-01</p> <p>The dynamical evolution of a fully kinetic, collisionless system with imposed background density and temperature <span class="hlt">gradients</span> is investigated analytically. The temperature <span class="hlt">gradient</span> leads to the generation of temperature anisotropy, with the temperature along the <span class="hlt">gradient</span> becoming larger than that in the direction perpendicular to it. This causes the system to become unstable to <span class="hlt">pressure</span> anisotropy driven instabilities, dominantly to the electron Weibel instability. When both density and temperature <span class="hlt">gradients</span> are present and nonparallel to each other, we obtain a Biermann-like linear-in-time magnetic field growth. Accompanying particle-in-cell numerical simulations are shown to confirm our analytical results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28864136','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28864136"><span>Severe aortic stenosis patients with preserved ejection fraction according to flow and <span class="hlt">gradient</span> classification: Prevalence and outcomes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>González Gómez, Ariana; Fernández-Golfín, Covadonga; Monteagudo, Juan Manuel; Izurieta, Carlos; Hinojar, Rocío; García, Ana; Casas, Eduardo; Jiménez-Nacher, José Julio; Moya, José Luis; Ruiz, Soledad; Zamorano, José Luis</p> <p>2017-12-01</p> <p>Clinicians often encounter patients with apparently discordant echocardiographic findings, severe aortic stenosis (SAS) defined by aortic valve area (AVA) despite a low mean <span class="hlt">gradient</span>. A new classification according to flow state and <span class="hlt">pressure</span> <span class="hlt">gradient</span> has been proposed. We sought to assess the prevalence, characteristics and outcomes of patients with asymptomatic SAS with preserved left-ventricular ejection fraction (LVEF) according to flow and <span class="hlt">gradient</span>. In total 442 patients with SAS (AVAi<0.6 cm2/m2) and LVEF ≥50% (mean age 80+11years, 54,5% female) were included. Patients were classified according to flow state (≥ or <35ml/m 2 ) and mean <span class="hlt">pressure</span> <span class="hlt">gradient</span> (≥ or <40mmHg): Low Flow/Low <span class="hlt">Gradient</span> (LF/LG): 21.3%(n=94); Normal Flow/Low <span class="hlt">Gradient</span> (NF/LG): 32.1%(n=142); Low Flow/High <span class="hlt">Gradient</span> (LF/HG): 6.8%(n=30); Normal Flow/High <span class="hlt">Gradient</span> (NF/HG): 39,8%(n=176). Mean follow-up time was 20.5months (SD=10.3). Primary combined endpoint was cardiovascular mortality and hospital admission for SAS related symptom, secondary endpoint was aortic valve replacement (AVR), comparing HG group to LF/LG group. During follow-up 17 (18%) of LF/LG patients and 21 (10.2%) of HG patients met the primary endpoint. A lower free of event survival (cardiovascular mortality and hospital admission) was observed in patients with LF/LG AS (Breslow, p=0.002). Significant differences were noted between groups with a lower AVR free survival in the LF/LG group compared to HG groups (Breslow, p=0.002). Our study confirms the high prevalence and worse prognosis of LF/LG SAS. Clinicians must be aware of this entity to ensure appropriate patient management. Copyright © 2017 Elsevier Ireland Ltd. All rights reserved.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_21 --> <div id="page_22" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="421"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ApGeo..12..283L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ApGeo..12..283L"><span>Full magnetic <span class="hlt">gradient</span> tensor from triaxial aeromagnetic <span class="hlt">gradient</span> measurements: Calculation and application</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Luo, Yao; Wu, Mei-Ping; Wang, Ping; Duan, Shu-Ling; Liu, Hao-Jun; Wang, Jin-Long; An, Zhan-Feng</p> <p>2015-09-01</p> <p>The full magnetic <span class="hlt">gradient</span> tensor (MGT) refers to the spatial change rate of the three field components of the geomagnetic field vector along three mutually orthogonal axes. The tensor is of use to geological mapping, resources exploration, magnetic navigation, and others. However, it is very difficult to measure the full magnetic tensor <span class="hlt">gradient</span> using existing engineering technology. We present a method to use triaxial aeromagnetic <span class="hlt">gradient</span> measurements for deriving the full MGT. The method uses the triaxial <span class="hlt">gradient</span> data and makes full use of the variation of the magnetic anomaly modulus in three dimensions to obtain a self-consistent magnetic tensor <span class="hlt">gradient</span>. Numerical simulations show that the full MGT data obtained with the proposed method are of high precision and satisfy the requirements of data processing. We selected triaxial aeromagnetic <span class="hlt">gradient</span> data from the Hebei Province for calculating the full MGT. Data processing shows that using triaxial tensor <span class="hlt">gradient</span> data allows to take advantage of the spatial rate of change of the total field in three dimensions and suppresses part of the independent noise in the aeromagnetic <span class="hlt">gradient</span>. The calculated tensor components have improved resolution, and the transformed full tensor <span class="hlt">gradient</span> satisfies the requirement of geological mapping and interpretation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ExFl...54.1581K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ExFl...54.1581K"><span>Experimental characterization of powered Fontan hemodynamics in an <span class="hlt">idealized</span> total cavopulmonary connection model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kerlo, Anna-Elodie M.; Delorme, Yann T.; Xu, Duo; Frankel, Steven H.; Giridharan, Guruprasad A.; Rodefeld, Mark D.; Chen, Jun</p> <p>2013-08-01</p> <p>A viscous impeller pump (VIP) based on the Von Karman viscous pump is specifically designed to provide cavopulmonary assist in a univentricular Fontan circulation. The technology will make it possible to biventricularize the univentricular Fontan circulation. <span class="hlt">Ideally</span>, it will reduce the number of surgeries required for Fontan conversion from three to one early in life, while simultaneously improving physiological conditions. Later in life, it will provide a currently unavailable means of chronic support for adolescent and adult patients with failing Fontan circulations. Computational fluid dynamics simulations demonstrate that the VIP can satisfactorily augment cavopulmonary blood flow in an <span class="hlt">idealized</span> total cavopulmonary connection (TCPC). When the VIP is deployed at the TCPC intersection as a static device, it stabilizes the four-way flow pattern and is not obstructive to the flow. Experimental studies are carried out to assess performance, hemodynamic characteristics, and flow structures of the VIP in an <span class="hlt">idealized</span> TCPC model. Stereoscopic particle image velocimetry is applied using index-matched blood analog. Results show excellent performance of the VIP without cavitation and with reduction of the energy losses. The non-rotating VIP smoothes and accelerates flow, and decreases stresses and turbulence in the TCPC. The rotating VIP generates the desired low-<span class="hlt">pressure</span> Fontan flow augmentation (0-10 mmHg) while maintaining acceptable stress thresholds.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23034902','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23034902"><span>Genetic and environmental influences on thin-<span class="hlt">ideal</span> internalization.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Suisman, Jessica L; O'Connor, Shannon M; Sperry, Steffanie; Thompson, J Kevin; Keel, Pamela K; Burt, S Alexandra; Neale, Michael; Boker, Steven; Sisk, Cheryl; Klump, Kelly L</p> <p>2012-12-01</p> <p>Current research on the etiology of thin-<span class="hlt">ideal</span> internalization focuses on psychosocial influences (e.g., media exposure). The possibility that genetic influences also account for variance in thin-<span class="hlt">ideal</span> internalization has never been directly examined. This study used a twin design to estimate genetic effects on thin-<span class="hlt">ideal</span> internalization and examine if environmental influences are primarily shared or nonshared in origin. Participants were 343 postpubertal female twins (ages: 12-22 years; M = 17.61) from the Michigan State University Twin Registry. Thin-<span class="hlt">ideal</span> internalization was assessed using the Sociocultural Attitudes toward Appearance Questionnaire-3. Twin modeling suggested significant additive genetic and nonshared environmental influences on thin-<span class="hlt">ideal</span> internalization. Shared environmental influences were small and non-significant. Although prior research focused on psychosocial factors, genetic influences on thin-<span class="hlt">ideal</span> internalization were significant and moderate in magnitude. Research is needed to investigate possible interplay between genetic and nonshared environmental factors in the development of thin-<span class="hlt">ideal</span> internalization. Copyright © 2012 Wiley Periodicals, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25781166','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25781166"><span>Quantifying patterns of change in marine ecosystem response to multiple <span class="hlt">pressures</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Large, Scott I; Fay, Gavin; Friedland, Kevin D; Link, Jason S</p> <p>2015-01-01</p> <p>The ability to understand and ultimately predict ecosystem response to multiple <span class="hlt">pressures</span> is paramount to successfully implement ecosystem-based management. Thresholds shifts and nonlinear patterns in ecosystem responses can be used to determine reference points that identify levels of a <span class="hlt">pressure</span> that may drastically alter ecosystem status, which can inform management action. However, quantifying ecosystem reference points has proven elusive due in large part to the multi-dimensional nature of both ecosystem <span class="hlt">pressures</span> and ecosystem responses. We used ecological indicators, synthetic measures of ecosystem status and functioning, to enumerate important ecosystem attributes and to reduce the complexity of the Northeast Shelf Large Marine Ecosystem (NES LME). Random forests were used to quantify the importance of four environmental and four anthropogenic <span class="hlt">pressure</span> variables to the value of ecological indicators, and to quantify shifts in aggregate ecological indicator response along <span class="hlt">pressure</span> <span class="hlt">gradients</span>. Anthropogenic <span class="hlt">pressure</span> variables were critical defining features and were able to predict an average of 8-13% (up to 25-66% for individual ecological indicators) of the variation in ecological indicator values, whereas environmental <span class="hlt">pressures</span> were able to predict an average of 1-5 % (up to 9-26% for individual ecological indicators) of ecological indicator variation. Each <span class="hlt">pressure</span> variable predicted a different suite of ecological indicator's variation and the shapes of ecological indicator responses along <span class="hlt">pressure</span> <span class="hlt">gradients</span> were generally nonlinear. Threshold shifts in ecosystem response to exploitation, the most important <span class="hlt">pressure</span> variable, occurred when commercial landings were 20 and 60% of total surveyed biomass. Although present, threshold shifts in ecosystem response to environmental <span class="hlt">pressures</span> were much less important, which suggests that anthropogenic <span class="hlt">pressures</span> have significantly altered the ecosystem structure and functioning of the NES LME. <span class="hlt">Gradient</span> response</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12231794','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12231794"><span>Direct Demonstration of a Growth-Induced Water Potential <span class="hlt">Gradient</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nonami, H.; Boyer, J. S.</p> <p>1993-05-01</p> <p>When transpiration is negligible, water potentials in growing tissues are less than those in mature tissues and have been predicted to form <span class="hlt">gradients</span> that move water into the enlarging cells. To determine directly whether the <span class="hlt">gradients</span> exist, we measured water potentials along the radius of stems of intact soybean (Glycine max [L.] Merr.) seedlings growing in vermiculite in a water-saturated atmosphere. The measurements were made in individual cells by first determining the turgor with a miniature <span class="hlt">pressure</span> probe, then determining the osmotic potential of solution from the same cell, and finally summing the two potentials. The osmotic potentials were corrected for sample mixing in the probe. The measurements were checked with a thermocouple psychrometer that gave average tissue water potentials. In the elongating region, the water potential was highest near the xylem and lowest near the epidermis and in the center of the pith. In the basal, more mature region of the same stems, water potentials were near zero next to the xylem and throughout the tissue. These basal potentials reflected mostly the potential of the xylem, which extended into the elongating tissues. Thus, the high basal potential confirmed the high potential near the xylem in the elongating tissues. The psychrometer measurements for each tissue gave average potentials that agreed with the average of the cell potentials from the <span class="hlt">pressure</span> probe. We conclude that a radial <span class="hlt">gradient</span> was present in the elongating region that formed a water potential field in three dimensions around the xylem and that confirmed the predictions of Molz and Boyer (F.J. Molz and J.S. Boyer [1978] Plant Physiol 62: 423-429).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=158741','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=158741"><span>Direct Demonstration of a Growth-Induced Water Potential <span class="hlt">Gradient</span>.</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Nonami, H.; Boyer, J. S.</p> <p>1993-01-01</p> <p>When transpiration is negligible, water potentials in growing tissues are less than those in mature tissues and have been predicted to form <span class="hlt">gradients</span> that move water into the enlarging cells. To determine directly whether the <span class="hlt">gradients</span> exist, we measured water potentials along the radius of stems of intact soybean (Glycine max [L.] Merr.) seedlings growing in vermiculite in a water-saturated atmosphere. The measurements were made in individual cells by first determining the turgor with a miniature <span class="hlt">pressure</span> probe, then determining the osmotic potential of solution from the same cell, and finally summing the two potentials. The osmotic potentials were corrected for sample mixing in the probe. The measurements were checked with a thermocouple psychrometer that gave average tissue water potentials. In the elongating region, the water potential was highest near the xylem and lowest near the epidermis and in the center of the pith. In the basal, more mature region of the same stems, water potentials were near zero next to the xylem and throughout the tissue. These basal potentials reflected mostly the potential of the xylem, which extended into the elongating tissues. Thus, the high basal potential confirmed the high potential near the xylem in the elongating tissues. The psychrometer measurements for each tissue gave average potentials that agreed with the average of the cell potentials from the <span class="hlt">pressure</span> probe. We conclude that a radial <span class="hlt">gradient</span> was present in the elongating region that formed a water potential field in three dimensions around the xylem and that confirmed the predictions of Molz and Boyer (F.J. Molz and J.S. Boyer [1978] Plant Physiol 62: 423-429). PMID:12231794</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18515203','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18515203"><span>Calculation of <span class="hlt">pressure</span> half-time.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Oyama, Mark A; Weidman, Jess A; Cole, Steven G</p> <p>2008-06-01</p> <p>Doppler echocardiography is useful in assessing the severity of obstructive cardiac lesions, such as mitral valve stenosis. The Doppler study can be used to calculate <span class="hlt">pressure</span> half-time (PHT), which is defined as the time required for the <span class="hlt">pressure</span> <span class="hlt">gradient</span> across an obstruction to decrease to half of its maximal value. Thus, PHT increases as the severity of stenosis increases. In this report, we describe the methodology involved in measuring PHT in a dog with mitral valve stenosis before and after balloon valvuloplasty.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3430141','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3430141"><span>Family Life and Developmental <span class="hlt">Idealism</span> in Yazd, Iran</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Abbasi-Shavazi, Mohammad Jalal; Askari-Nodoushan, Abbas</p> <p>2012-01-01</p> <p>BACKGROUND This paper is motivated by the theory that developmental <span class="hlt">idealism</span> has been disseminated globally and has become an international force for family and demographic change. Developmental <span class="hlt">idealism</span> is a set of cultural beliefs and values about development and how development relates to family and demographic behavior. It holds that modern societies are causal forces producing modern families, that modern families help to produce modern societies, and that modern family change is to be expected. OBJECTIVE We examine the extent to which developmental <span class="hlt">idealism</span> has been disseminated in Iran. We also investigate predictors of the dissemination of developmental <span class="hlt">idealism</span>. METHODS We use survey data collected in 2007 from a sample of women in Yazd, a city in Iran. We examine the distribution of developmental <span class="hlt">idealism</span> in the sample and the multivariate predictors of developmental <span class="hlt">idealism</span>. RESULTS We find considerable support for the expectation that many elements of developmental <span class="hlt">idealism</span> have been widely disseminated. Statistically significant majorities associate development with particular family attributes, believe that development causes change in families, believe that fertility reductions and age-at-marriage increases help foster development, and perceive family trends in Iran headed toward modernity. As predicted, parental education, respondent education, and income affect adherence to developmental <span class="hlt">idealism</span>. CONCLUSIONS Developmental <span class="hlt">idealism</span> has been widely disseminated in Yazd, Iran and is related to social and demographic factors in predicted ways. COMMENTS Although our data come from only one city, we expect that developmental <span class="hlt">idealism</span> has been widely distributed in Iran, with important implications for family and demographic behavior. PMID:22942772</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28093205','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28093205"><span>Characterization of peak capacity of microbore liquid chromatography columns using <span class="hlt">gradient</span> kinetic plots.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hetzel, Terence; Blaesing, Christina; Jaeger, Martin; Teutenberg, Thorsten; Schmidt, Torsten C</p> <p>2017-02-17</p> <p>The performance of micro-liquid chromatography columns with an inner diameter of 0.3mm was investigated on a dedicated micro-LC system for <span class="hlt">gradient</span> elution. Core-shell as well as fully porous particle packed columns were compared on the basis of peak capacity and <span class="hlt">gradient</span> kinetic plot limits. The results for peak capacity showed the superior performance of columns packed with sub-2μm fully porous particles compared to 3.0μm fully porous and 2.7μm core-shell particles within a range of different <span class="hlt">gradient</span> time to column void time ratios. For ultra-fast chromatography a maximum peak capacity of 16 can be obtained using a 30s <span class="hlt">gradient</span> for the sub-2μm fully porous particle packed column. A maximum peak capacity of 121 can be achieved using a 5min <span class="hlt">gradient</span>. In addition, the influence of an alternative detector cell on the basis of optical waveguide technology and contributing less to system variance was investigated showing an increased peak capacity for all applied <span class="hlt">gradient</span> time/column void time ratios. Finally, the influence of <span class="hlt">pressure</span> was evaluated indicating increased peak capacity for maximum performance whereas a limited benefit for ultra-fast chromatography with <span class="hlt">gradient</span> times below 30s was observed. Copyright © 2017 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S23C0825P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S23C0825P"><span>Geothermal <span class="hlt">Gradient</span> impact on Induced Seismicity in Raton Basin, Colorado and New Mexico</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pfeiffer, K.; Ge, S.</p> <p>2017-12-01</p> <p>Since 1999, Raton Basin, located in southeastern Colorado and northern New Mexico, is the site of wastewater injection for disposing a byproduct of coal bed methane production. During 1999-2016, 29 wastewater injection wells were active in Raton Basin. Induced seismicity began in 2001 and the largest recorded earthquake, an M5.3, occurred in August 2011. Although most injection occurs in the Dakota Formation, the majority of the seismicity has been located in the crystalline basement. Previous studies involving Raton Basin focused on high injection rates and high volume wells to determine their effect on increased pore <span class="hlt">pressure</span>. However, the geothermal <span class="hlt">gradient</span> has yet to be studied as a potential catalyst of seismicity. Enhanced Geothermal Systems throughout the world have experienced similar seismicity problems due to water injection. Raton's geothermal <span class="hlt">gradient</span>, which averages 49± 12°C/km, is much higher then other areas experiencing seismicity. Thermal differences between the hot subsurface and cooler wastewater injection have the potential to affect the strength of the rock and allow for failure. Therefore, we hypothesis that wells in high geothermal <span class="hlt">gradient</span> areas will produce more frequent earthquakes due to thermal contrast from relatively cold wastewater injection. We model the geothermal <span class="hlt">gradient</span> in the surrounding areas of the injection sites in Raton Basin to assess potential spatial relationship between high geothermal <span class="hlt">gradient</span> and earthquakes. Preliminary results show that the fluid <span class="hlt">pressure</span> increase from injecting cool water is above the threshold of 0.1MPa, which has been shown to induce earthquakes. In addition, temperatures in the subsurface could decrease up to 2°C at approximately 80 m from the injection well, with a temperature effect reaching up to 100 m away from the injection well.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5715107','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5715107"><span>Tree Leaf Bacterial Community Structure and Diversity Differ along a <span class="hlt">Gradient</span> of Urban Intensity</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Messier, Christian; Kembel, Steven W.</p> <p>2017-01-01</p> <p>ABSTRACT Tree leaf-associated microbiota have been studied in natural ecosystems but less so in urban settings, where anthropogenic <span class="hlt">pressures</span> on trees could impact microbial communities and modify their interaction with their hosts. Additionally, trees act as vectors spreading bacterial cells in the air in urban environments due to the density of microbial cells on aerial plant surfaces. Characterizing tree leaf bacterial communities along an urban <span class="hlt">gradient</span> is thus key to understand the impact of anthropogenic <span class="hlt">pressures</span> on urban tree-bacterium interactions and on the overall urban microbiome. In this study, we aimed (i) to characterize phyllosphere bacterial communities of seven tree species in urban environments and (ii) to describe the changes in tree phyllosphere bacterial community structure and diversity along a <span class="hlt">gradient</span> of increasing urban intensity and at two degrees of tree isolation. Our results indicate that, as anthropogenic <span class="hlt">pressures</span> increase, urban leaf bacterial communities show a reduction in the abundance of the dominant class in the natural plant microbiome, the Alphaproteobacteria. Our work in the urban environment here reveals that the structures of leaf bacterial communities differ along the <span class="hlt">gradient</span> of urban intensity. The diversity of phyllosphere microbial communities increases at higher urban intensity, also displaying a greater number and variety of associated indicator taxa than the low and medium urban <span class="hlt">gradient</span> sites. In conclusion, we find that urban environments influence tree bacterial community composition, and our results suggest that feedback between human activity and plant microbiomes could shape urban microbiomes. IMPORTANCE In natural forests, tree leaf surfaces host diverse bacterial communities whose structure and composition are primarily driven by host species identity. Tree leaf bacterial diversity has also been shown to influence tree community productivity, a key function of terrestrial ecosystems. However, most urban</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29238751','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29238751"><span>Tree Leaf Bacterial Community Structure and Diversity Differ along a <span class="hlt">Gradient</span> of Urban Intensity.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Laforest-Lapointe, Isabelle; Messier, Christian; Kembel, Steven W</p> <p>2017-01-01</p> <p>Tree leaf-associated microbiota have been studied in natural ecosystems but less so in urban settings, where anthropogenic <span class="hlt">pressures</span> on trees could impact microbial communities and modify their interaction with their hosts. Additionally, trees act as vectors spreading bacterial cells in the air in urban environments due to the density of microbial cells on aerial plant surfaces. Characterizing tree leaf bacterial communities along an urban <span class="hlt">gradient</span> is thus key to understand the impact of anthropogenic <span class="hlt">pressures</span> on urban tree-bacterium interactions and on the overall urban microbiome. In this study, we aimed (i) to characterize phyllosphere bacterial communities of seven tree species in urban environments and (ii) to describe the changes in tree phyllosphere bacterial community structure and diversity along a <span class="hlt">gradient</span> of increasing urban intensity and at two degrees of tree isolation. Our results indicate that, as anthropogenic <span class="hlt">pressures</span> increase, urban leaf bacterial communities show a reduction in the abundance of the dominant class in the natural plant microbiome, the Alphaproteobacteria . Our work in the urban environment here reveals that the structures of leaf bacterial communities differ along the <span class="hlt">gradient</span> of urban intensity. The diversity of phyllosphere microbial communities increases at higher urban intensity, also displaying a greater number and variety of associated indicator taxa than the low and medium urban <span class="hlt">gradient</span> sites. In conclusion, we find that urban environments influence tree bacterial community composition, and our results suggest that feedback between human activity and plant microbiomes could shape urban microbiomes. IMPORTANCE In natural forests, tree leaf surfaces host diverse bacterial communities whose structure and composition are primarily driven by host species identity. Tree leaf bacterial diversity has also been shown to influence tree community productivity, a key function of terrestrial ecosystems. However, most urban microbiome</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920041973&hterms=conjugate+gradient&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dconjugate%2Bgradient','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920041973&hterms=conjugate+gradient&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dconjugate%2Bgradient"><span>Natural convection in binary gases driven by combined horizontal thermal and vertical solutal <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Weaver, J. A.; Viskanta, Raymond</p> <p>1992-01-01</p> <p>An investigation of natural convection is presented to examine the influence of a horizontal temperature <span class="hlt">gradient</span> and a concentration <span class="hlt">gradient</span> occurring from the bottom to the cold wall in a cavity. As the solutal buoyancy force changes from augmenting to opposing the thermal buoyancy force, the fluid motion switches from unicellular to multicellular flow (fluid motion is up the cold wall and down the hot wall for the bottom counterrotating flow cell). Qualitatively, the agreement between predicted streamlines and smoke flow patterns is generally good. In contrast, agreement between measured and predicted temperature and concentration distributions ranges from fair to poor. Part of the discrepancy can be attributed to experimental error. However, there remains considerable discrepancy between data and predictions due to the <span class="hlt">idealizations</span> of the mathematical model, which examines only first-order physical effects. An unsteady flow, variable thermophysical properties, conjugate effects, species interdiffusion, and radiation were not accounted for in the model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/897958','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/897958"><span>Behavior of Explosives Under <span class="hlt">Pressure</span> in a Diamond Anvil Cell</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Foltz, M F</p> <p>2006-06-20</p> <p>Diamond anvil cell (DAC) studies can yield information about the <span class="hlt">pressure</span> dependence of materials and reactions under conditions comparable to shock loading. The <span class="hlt">pressure</span> <span class="hlt">gradient</span> across the face of the diamonds is often deliberately minimized to create uniform <span class="hlt">pressure</span> over much of the sample and a simplified data set. To reach very high <span class="hlt">pressures</span> (30-40 GPa), however, it may be necessary to use ''softer'', high nitrogen content diamonds that are more susceptible to bending under <span class="hlt">pressure</span>. The resulting enhanced <span class="hlt">pressure</span> <span class="hlt">gradient</span> then provides a view of high-<span class="hlt">pressure</span> behavior under anisotropic conditions similar to those found at the burn front inmore » a bulk sample. We discuss visual observations of <span class="hlt">pressure</span>-induced changes relative to variations in burn rate of several explosives (Triaminotrinitrobenzene, Nitromethane, CL-20) in the DAC. The burn rate behavior of both Nitromethane (NM) and Triaminotrinitrobenzene (TATB) were previously reported for <span class="hlt">pressures</span> up to {approx}40 GPa. Nitromethane showed a near monotonic increase in burn rate to a maximum at {approx}30 GPa after which the burn rate decreased, all without color change. At higher <span class="hlt">pressures</span>, the TATB samples had shiny (metallic) polycrystalline zones or inclusions where the <span class="hlt">pressure</span> was highest in the sample. Around the shiny zones was a gradation of color (red to yellow) that appeared to follow the <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The color changes are believed related to disturbances in the resonance structure of this explosive as the intermolecular separations decrease with <span class="hlt">pressure</span>. The color and type of residue found in unvented gaskets after the burn was complete also varied with <span class="hlt">pressure</span>. The four polymorphs of CL-20 ({alpha}, {beta}, {gamma}, {var_epsilon}-Hexanitrohexaazaisowurtzitane, HNIW) did not change color up to the highest <span class="hlt">pressure</span> applied ({approx}30 GPa), and each polymorph demonstrated a distinctly different burn rate signature. One polymorph {beta} was so sensitive to laser ignition over a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050082147','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050082147"><span><span class="hlt">Gradient</span> Driven Fluctuations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cannell, David</p> <p>2005-01-01</p> <p>We have worked with our collaborators at the University of Milan (Professor Marzio Giglio and his group-supported by ASI) to define the science required to measure <span class="hlt">gradient</span> driven fluctuations in the microgravity environment. Such a study would provide an accurate test of the extent to which the theory of fluctuating hydrodynamics can be used to predict the properties of fluids maintained in a stressed, non-equilibrium state. As mentioned above, the results should also provide direct visual insight into the behavior of a variety of fluid systems containing <span class="hlt">gradients</span> or interfaces, when placed in the microgravity environment. With support from the current grant, we have identified three key systems for detailed investigation. These three systems are: 1) A single-component fluid to be studied in the presence of a temperature <span class="hlt">gradient</span>; 2) A mixture of two organic liquids to be studied both in the presence of a temperature <span class="hlt">gradient</span>, which induces a steady-state concentration <span class="hlt">gradient</span>, and with the temperature <span class="hlt">gradient</span> removed, but while the concentration <span class="hlt">gradient</span> is dying by means of diffusion; 3) Various pairs of liquids undergoing free diffusion, including a proteidbuffer solution and pairs of mixtures having different concentrations, to allow us to vary the differences in fluid properties in a controlled manner.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29067687','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29067687"><span>Relationship Between <span class="hlt">Ideal</span> Cardiovascular Health and Disability in Older Adults: The Chilean National Health Survey (2009-10).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>García-Hermoso, Antonio; Ramírez-Vélez, Robinson; Ramirez-Campillo, Rodrigo; Izquierdo, Mikel</p> <p>2017-12-01</p> <p>This study aimed to examine the relationship between disability and the American Heart Association metric of <span class="hlt">ideal</span> cardiovascular health (CVH) in older adults from the 2009-10 Chilean National Health Survey. Data from 460 older adults were analyzed. All subjects were interviewed using the standardized World Health Survey, which includes 16 health-related questions and assesses the domains of mobility, self-care, pain and discomfort, cognition, interpersonal activities, vision, sleep and energy, and affect. A person who responds with a difficulty rating of severe, extreme, or unable to do in at least one of these eight functioning domains is considered to have a disability. <span class="hlt">Ideal</span> CVH was defined as meeting the <span class="hlt">ideal</span> levels of four behaviors (smoking, body mass index, physical activity, diet adherence) and three factors (total cholesterol, fasting glucose, blood <span class="hlt">pressure</span>). Logistic regression analysis suggested that <span class="hlt">ideal</span> physical activity reduces the odds of disability (odds ratio (OR) = 0.55, 95% confidence interval (CI) = 0.36-0.85). Moreover, participants with intermediate (3-4 metrics) (OR = 0.63, 95% CI = 0.41-0.97) and <span class="hlt">ideal</span> (5-7 metrics) (OR = 0.51, 95% CI = 0.24-0.97) CVH profiles had lower odds of disability independent of history of vascular events and arthritis disease than those with a poor profile (0-2 metrics). In conclusion, despite the cross-sectional design, this study suggests the importance of promoting <span class="hlt">ideal</span> CVH because of their relationship with disability. © 2017, Copyright the Authors Journal compilation © 2017, The American Geriatrics Society.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23384051','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23384051"><span>Purification of white spot syndrome virus by iodixanol density <span class="hlt">gradient</span> centrifugation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dantas-Lima, J J; Corteel, M; Cornelissen, M; Bossier, P; Sorgeloos, P; Nauwynck, H J</p> <p>2013-10-01</p> <p>Up to now, only a few brief procedures for purifying white spot syndrome virus (WSSV) have been described. They were mainly based on sucrose, NaBr and CsCl density <span class="hlt">gradient</span> centrifugation. This work describes for the first time the purification of WSSV through iodixanol density <span class="hlt">gradients</span>, using virus isolated from infected tissues and haemolymph of Penaeus vannamei (Boone). The purification from tissues included a concentration step by centrifugation (2.5 h at 60,000 g) onto a 50% iodixanol cushion and a purification step by centrifugation (3 h at 80,000 g) through a discontinuous iodixanol <span class="hlt">gradient</span> (phosphate-buffered saline, 5%, 10%, 15% and 20%). The purification from infected haemolymph enclosed a dialysis step with a membrane of 1,000 kDa (18 h) and a purification step through the earlier iodixanol <span class="hlt">gradient</span>. The <span class="hlt">gradients</span> were collected in fractions and analysed. The number of particles, infectivity titre (in vivo), total protein and viral protein content were evaluated. The purification from infected tissues gave WSSV suspensions with a very high infectivity and an acceptable purity, while virus purified from haemolymph had a high infectivity and a very high purity. Additionally, it was observed that WSSV has an unusually low buoyant density and that it is very sensitive to high external <span class="hlt">pressures</span>. © 2013 John Wiley & Sons Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMOS51A1148G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMOS51A1148G"><span>Resolving the Role of the Dynamic <span class="hlt">Pressure</span> in the Burial, Exposure, Scour, and Mobility of Underwater Munitions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gilooly, S.; Foster, D. L.</p> <p>2017-12-01</p> <p>In nearshore environments, the motion of munitions results from a mixture of sediment transport conditions including sheet flow, scour, bedform migration, and momentary liquefaction. Incipient motion can be caused by disruptive shear stresses and <span class="hlt">pressure</span> <span class="hlt">gradients</span>. Foster et al. (2006) incorporated both processes into a single parameter, indicating incipient motion as a function of the bed state. This research looks to evaluate the role of the <span class="hlt">pressure</span> <span class="hlt">gradient</span> in positional state changes such as burial, exposure, and mobility. In the case of munitions, this may include <span class="hlt">pressure</span> <span class="hlt">gradients</span> induced by vortex shedding or the passing wave. <span class="hlt">Pressure</span>-mapped model munitions are being developed to measure the orientation, rotation, and surface <span class="hlt">pressure</span> of the munitions during threshold events leading to a new positional state. These munitions will be deployed in inner surf zone and estuary environments along with acoustic Doppler velocimeters (ADVs), pore water <span class="hlt">pressure</span> sensors, a laser grid, and a pencil beam sonar with an azimuth drive. The additional instruments allow for near bed and far field water column and sediment bed sampling. Currently preliminary assessments of various <span class="hlt">pressure</span> sensors and munition designs are underway. Two <span class="hlt">pressure</span> sensors were selected; the thin FlexiForce A201 sensors will be used to indicate munition rolling during threshold events and diaphragm sensors will be used to understand changes in surrounding pore water <span class="hlt">pressure</span> as the munition begins to bury/unbury. Both sensors are expected to give quantitative measurements of dynamic <span class="hlt">pressure</span> <span class="hlt">gradients</span> in the flow field surrounding the munition. Resolving the role of this process will give insight to an improved incipient motion parameter and allow for better munition motion predictions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26ES..155a2001M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26ES..155a2001M"><span>An analytical model of SAGD process considering the effect of threshold <span class="hlt">pressure</span> <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Morozov, P.; Abdullin, A.; Khairullin, M.</p> <p>2018-05-01</p> <p>An analytical model is proposed for the development of super-viscous oil deposits by the method of steam-assisted gravity drainage, taking into account the nonlinear filtration law with the limiting <span class="hlt">gradient</span>. The influence of non-Newtonian properties of oil on the productivity of a horizontal well and the cumulative steam-oil ratio are studied. Verification of the proposed model based on the results of physical modeling of the SAGD process was carried out.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27748008','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27748008"><span>Determinants and prognostic implications of the negative diastolic pulmonary <span class="hlt">pressure</span> <span class="hlt">gradient</span> in patients with pulmonary hypertension due to left heart disease.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nagy, Anikó Ilona; Venkateshvaran, Ashwin; Merkely, Béla; Lund, Lars H; Manouras, Aristomenis</p> <p>2017-01-01</p> <p>The diastolic pulmonary <span class="hlt">pressure</span> <span class="hlt">gradient</span> (DPG) has recently been introduced as a specific marker of combined pre-capillary pulmonary hypertension (Cpc-PH) in left heart disease (LHD). However, its diagnostic and prognostic superiority compared with traditional haemodynamic indices has been challenged lately. Current recommendations explicitly denote that in the normal heart, DPG values are greater than zero, with DPG ≥7 mmHg indicating Cpc-PH. However, clinicians are perplexed by the frequent observation of DPG <0 mmHg (DPG NEG ), as its physiological explanation and clinical impact are unclear to date. We hypothesized that large V-waves in the pulmonary artery wedge <span class="hlt">pressure</span> (PAWP) curve yielding asymmetric <span class="hlt">pressure</span> transmission might account for DPG NEG and undertook this study to clarify the physiological and prognostic implications of DPG NEG . Right heart catheterization and echocardiography were performed in 316 patients with LHD due to primary myocardial dysfunction or valvular disease. A total of 256 patients had PH-LHD, of whom 48% demonstrated DPG NEG . The V-wave amplitude inversely correlated with DPG (r = -0.45, P < 0.001) in patients with low pulmonary vascular resistance (PVR), but not in those with elevated PVR (P > 0.05). Patients with large V-waves had negative and lower DPG than those without augmented V-waves (P < 0.001) despite similar PVR (P >0.05). Positive, but normal DPG (0-6 mmHg) carried a worse 2-year prognosis for death and/or heart transplantation than DPG NEG (hazard ratio 2.97; P < 0.05). Our results advocate against DPG NEG constituting a measurement error. We propose that DPG NEG can partially be ascribed to large V-waves and carries a better prognosis than DPG within the normal positive range. © 2016 The Authors. European Journal of Heart Failure © 2016 European Society of Cardiology.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_22 --> <div id="page_23" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="441"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999PhDT........45K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999PhDT........45K"><span>Identifying and addressing student difficulties with the <span class="hlt">ideal</span> gas law</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kautz, Christian Hans</p> <p></p> <p>This dissertation reports on an in-depth investigation of student understanding of the <span class="hlt">ideal</span> gas law. The research and curriculum development were mostly conducted in the context of algebra- and calculus-based introductory physics courses and a sophomore-level thermal physics course. Research methods included individual demonstration interviews and written questions. Student difficulties with the quantities: <span class="hlt">pressure</span>, volume, temperature, and the number of moles were identified. Data suggest that students' incorrect and incomplete microscopic models about gases contribute to the difficulties they have in answering questions posed in macroscopic terms. In addition, evidence for general reasoning difficulties is presented. These research results have guided the development of curriculum to address the student difficulties that have been identified.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/5093919','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/5093919"><span>Determination of <span class="hlt">ideal</span>-gas enthalpies of formation for key compounds:</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Steele, W.V.; Chirico, R.D.; Nguyen, A.</p> <p>1991-10-01</p> <p>The results of a study aimed at improvement of group-contribution methodology for estimation of thermodynamic properties of organic and organosilicon substances are reported. Specific weaknesses where particular group-contribution terms were unknown, or estimated because of lack of experimental data, are addressed by experimental studies of enthalpies of combustion in the condensed phase, vapor-<span class="hlt">pressure</span> measurements, and differential scanning calorimetric (d.s.c.) heat-capacity measurements. <span class="hlt">Ideal</span>-gas enthalpies of formation of ({plus minus})-butan-2-ol, tetradecan-1-ol, hexan-1,6-diol, methacrylamide, benzoyl formic acid, naphthalene-2,6-dicarboxylic acid dimethyl ester, and tetraethylsilane are reported. A crystalline-phase enthalpy of formation at 298.15 K was determined for naphthalene-2,6-dicarboxylic acid, which decomposed at 695 Kmore » before melting. The combustion calorimetry of tetraethylsilane used the proven fluorine-additivity methodology. Critical temperature and critical density were determined for tetraethylsilane with differential scanning calorimeter and the critical <span class="hlt">pressure</span> was derived. Group-additivity parameters useful in the application of group- contribution correlations are derived. 112 refs., 13 figs., 19 tabs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/7163071','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/7163071"><span>Oxygen partial <span class="hlt">pressure</span> sensor</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Dees, D.W.</p> <p>1994-09-06</p> <p>A method for detecting oxygen partial <span class="hlt">pressure</span> and an oxygen partial <span class="hlt">pressure</span> sensor are provided. The method for measuring oxygen partial <span class="hlt">pressure</span> includes contacting oxygen to a solid oxide electrolyte and measuring the subsequent change in electrical conductivity of the solid oxide electrolyte. A solid oxide electrolyte is utilized that contacts both a porous electrode and a nonporous electrode. The electrical conductivity of the solid oxide electrolyte is affected when oxygen from an exhaust stream permeates through the porous electrode to establish an equilibrium of oxygen anions in the electrolyte, thereby displacing electrons throughout the electrolyte to form an electron <span class="hlt">gradient</span>. By adapting the two electrodes to sense a voltage potential between them, the change in electrolyte conductivity due to oxygen presence can be measured. 1 fig.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/869477','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/869477"><span>Oxygen partial <span class="hlt">pressure</span> sensor</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Dees, Dennis W.</p> <p>1994-01-01</p> <p>A method for detecting oxygen partial <span class="hlt">pressure</span> and an oxygen partial <span class="hlt">pressure</span> sensor are provided. The method for measuring oxygen partial <span class="hlt">pressure</span> includes contacting oxygen to a solid oxide electrolyte and measuring the subsequent change in electrical conductivity of the solid oxide electrolyte. A solid oxide electrolyte is utilized that contacts both a porous electrode and a nonporous electrode. The electrical conductivity of the solid oxide electrolyte is affected when oxygen from an exhaust stream permeates through the porous electrode to establish an equilibrium of oxygen anions in the electrolyte, thereby displacing electrons throughout the electrolyte to form an electron <span class="hlt">gradient</span>. By adapting the two electrodes to sense a voltage potential between them, the change in electrolyte conductivity due to oxygen presence can be measured.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28588196','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28588196"><span>Direct measurement of optical trapping force <span class="hlt">gradient</span> on polystyrene microspheres using a carbon nanotube mechanical resonator.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yasuda, Masaaki; Takei, Kuniharu; Arie, Takayuki; Akita, Seiji</p> <p>2017-06-06</p> <p>Optical tweezers based on optical radiation <span class="hlt">pressure</span> are widely used to manipulate nanoscale to microscale particles. This study demonstrates direct measurement of the optical force <span class="hlt">gradient</span> distribution acting on a polystyrene (PS) microsphere using a carbon nanotube (CNT) mechanical resonator, where a PS microsphere with 3 μm diameter is welded at the CNT tip using laser heating. With the CNT mechanical resonator with PS microsphere, we measured the distribution of optical force <span class="hlt">gradient</span> with resolution near the thermal noise limit of 0.02 pN/μm in vacuum, in which condition enables us to high accuracy measurement using the CNT mechanical resonator because of reduced mechanical damping from surrounding fluid. The obtained force <span class="hlt">gradient</span> and the force <span class="hlt">gradient</span> distribution agree well with theoretical values calculated using Lorenz-Mie theory.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4254567','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4254567"><span>“Measure Your Gradient”: A New Way to Measure <span class="hlt">Gradients</span> in High Performance Liquid Chromatography by Mass Spectrometric or Absorbance Detection</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Magee, Megan H.; Manulik, Joseph C.; Barnes, Brian B.; Abate-Pella, Daniel; Hewitt, Joshua T.; Boswell, Paul G.</p> <p>2014-01-01</p> <p>The <span class="hlt">gradient</span> produced by an HPLC is never the same as the one it is programmed to produce, but non-<span class="hlt">idealities</span> in the <span class="hlt">gradient</span> can be taken into account if they are measured. Such measurements are routine, yet only one general approach has been described to make them: both HPLC solvents are replaced with water, solvent B is spiked with 0.1% acetone, and the <span class="hlt">gradient</span> is measured by UV absorbance. Despite the widespread use of this procedure, we found a number of problems and complications with it, mostly stemming from the fact that it measures the <span class="hlt">gradient</span> under abnormal conditions (e.g. both solvents are water). It is also generally not amenable to MS detection, leaving those with only an MS detector no way to accurately measure their <span class="hlt">gradients</span>. We describe a new approach called “Measure Your Gradient” that potentially solves these problems. One runs a test mixture containing 20 standards on a standard stationary phase and enters their <span class="hlt">gradient</span> retention times into open-source software available at www.measureyourgradient.org. The software uses the retention times to back-calculate the <span class="hlt">gradient</span> that was truly produced by the HPLC. Here we present a preliminary investigation of the new approach. We found that <span class="hlt">gradients</span> measured this way are comparable to those measured by a more accurate, albeit impractical, version of the conventional approach. The new procedure worked with different <span class="hlt">gradients</span>, flow rates, column lengths, inner diameters, on two different HPLCs, and with six different batches of the standard stationary phase. PMID:25441073</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110002689','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110002689"><span>The Statistical Mechanics of <span class="hlt">Ideal</span> MHD Turbulence</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shebalin, John V.</p> <p>2003-01-01</p> <p>Turbulence is a universal, nonlinear phenomenon found in all energetic fluid and plasma motion. In particular. understanding magneto hydrodynamic (MHD) turbulence and incorporating its effects in the computation and prediction of the flow of ionized gases in space, for example, are great challenges that must be met if such computations and predictions are to be meaningful. Although a general solution to the "problem of turbulence" does not exist in closed form, numerical integrations allow us to explore the phase space of solutions for both <span class="hlt">ideal</span> and dissipative flows. For homogeneous, incompressible turbulence, Fourier methods are appropriate, and phase space is defined by the Fourier coefficients of the physical fields. In the case of <span class="hlt">ideal</span> MHD flows, a fairly robust statistical mechanics has been developed, in which the symmetry and ergodic properties of phase space is understood. A discussion of these properties will illuminate our principal discovery: Coherent structure and randomness co-exist in <span class="hlt">ideal</span> MHD turbulence. For dissipative flows, as opposed to <span class="hlt">ideal</span> flows, progress beyond the dimensional analysis of Kolmogorov has been difficult. Here, some possible future directions that draw on the <span class="hlt">ideal</span> results will also be discussed. Our conclusion will be that while <span class="hlt">ideal</span> turbulence is now well understood, real turbulence still presents great challenges.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999SPIE.3591...82J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999SPIE.3591...82J"><span>Importance of intraocular <span class="hlt">pressure</span> in glaucoma</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Joos, Karen M.</p> <p>1999-06-01</p> <p>Glaucoma results in permanent vision loss and affects the peripheral vision initially. It is presented in 22.5 million people worldwide and is the 3rd cause of blindness. Present tonometers are not <span class="hlt">ideal</span> for intraocular <span class="hlt">pressure</span> measurements in all eyes. Of concern, PRK and LASIK may result in lower intraocular <span class="hlt">pressure</span> readings. A challenges now exists for the development of a tonometer which can easily compensate for corneas with many parameters to avoid a future increase in normal-tension glaucoma or glaucoma which is advanced.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70020226','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70020226"><span>Abnormal <span class="hlt">pressure</span> in hydrocarbon environments</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Law, B.E.; Spencer, C.W.</p> <p>1998-01-01</p> <p>Abnormal <span class="hlt">pressures</span>, <span class="hlt">pressures</span> above or below hydrostatic <span class="hlt">pressures</span>, occur on all continents in a wide range of geological conditions. According to a survey of published literature on abnormal <span class="hlt">pressures</span>, compaction disequilibrium and hydrocarbon generation are the two most commonly cited causes of abnormally high <span class="hlt">pressure</span> in petroleum provinces. In young (Tertiary) deltaic sequences, compaction disequilibrium is the dominant cause of abnormal <span class="hlt">pressure</span>. In older (pre-Tertiary) lithified rocks, hydrocarbon generation, aquathermal expansion, and tectonics are most often cited as the causes of abnormal <span class="hlt">pressure</span>. The association of abnormal <span class="hlt">pressures</span> with hydrocarbon accumulations is statistically significant. Within abnormally <span class="hlt">pressured</span> reservoirs, empirical evidence indicates that the bulk of economically recoverable oil and gas occurs in reservoirs with <span class="hlt">pressure</span> <span class="hlt">gradients</span> less than 0.75 psi/ft (17.4 kPa/m) and there is very little production potential from reservoirs that exceed 0.85 psi/ft (19.6 kPa/m). Abnormally <span class="hlt">pressured</span> rocks are also commonly associated with unconventional gas accumulations where the <span class="hlt">pressuring</span> phase is gas of either a thermal or microbial origin. In underpressured, thermally mature rocks, the affected reservoirs have most often experienced a significant cooling history and probably evolved from an originally overpressured system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3573840','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3573840"><span>Predicting Film Genres with Implicit <span class="hlt">Ideals</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Olney, Andrew McGregor</p> <p>2013-01-01</p> <p>We present a new approach to defining film genre based on implicit <span class="hlt">ideals</span>. When viewers rate the likability of a film, they indirectly express their <span class="hlt">ideal</span> of what a film should be. Across six studies we investigate the category structure that emerges from likability ratings and the category structure that emerges from the features of film. We further compare these data-driven category structures with human annotated film genres. We conclude that film genres are structured more around <span class="hlt">ideals</span> than around features of film. This finding lends experimental support to the notion that film genres are set of shifting, fuzzy, and highly contextualized psychological categories. PMID:23423823</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23423823','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23423823"><span>Predicting film genres with implicit <span class="hlt">ideals</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Olney, Andrew McGregor</p> <p>2012-01-01</p> <p>We present a new approach to defining film genre based on implicit <span class="hlt">ideals</span>. When viewers rate the likability of a film, they indirectly express their <span class="hlt">ideal</span> of what a film should be. Across six studies we investigate the category structure that emerges from likability ratings and the category structure that emerges from the features of film. We further compare these data-driven category structures with human annotated film genres. We conclude that film genres are structured more around <span class="hlt">ideals</span> than around features of film. This finding lends experimental support to the notion that film genres are set of shifting, fuzzy, and highly contextualized psychological categories.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27312889','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27312889"><span>Microbial community diversity, structure and assembly across oxygen <span class="hlt">gradients</span> in meromictic marine lakes, Palau.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Meyerhof, Matthew S; Wilson, Jesse M; Dawson, Michael N; Michael Beman, J</p> <p>2016-12-01</p> <p>Microbial communities consume oxygen, alter biogeochemistry and compress habitat in aquatic ecosystems, yet our understanding of these microbial-biogeochemical-ecological interactions is limited by a lack of systematic analyses of low-oxygen ecosystems. Marine lakes provide an <span class="hlt">ideal</span> comparative system, as they range from well-mixed holomictic lakes to stratified, anoxic, meromictic lakes that vary in their vertical extent of anoxia. We examined microbial communities inhabiting six marine lakes and one ocean site using pyrosequencing of 16S rRNA genes. Microbial richness and evenness was typically highest in the anoxic monimolimnion of meromictic lakes, with common marine bacteria present in mixolimnion communities replaced by anoxygenic phototrophs, sulfate-reducing bacteria and SAR406 in the monimolimnion. These sharp changes in community structure were linked to environmental <span class="hlt">gradients</span> (constrained variation in redundancy analysis = 68%-76%) - particularly oxygen and pH. However, in those lakes with the steepest oxygen <span class="hlt">gradients</span>, salinity and dissolved nutrients were important secondary constraining variables, indicating that subtle but substantive differences in microbial communities occur within similar low-oxygen habitats. Deterministic processes were a dominant influence on whole community assembly (all nearest taxon index values >4), demonstrating that the strong environmental <span class="hlt">gradients</span> present in meromictic marine lakes drive microbial community assembly. © 2016 Society for Applied Microbiology and John Wiley & Sons Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22685590','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22685590"><span>Size-frequency distributions along a latitudinal <span class="hlt">gradient</span> in Middle Permian fusulinoideans.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Yichun; Payne, Jonathan L</p> <p>2012-01-01</p> <p>Geographic <span class="hlt">gradients</span> in body size within and among living species are commonly used to identify controls on the long-term evolution of organism size. However, the persistence of these <span class="hlt">gradients</span> over evolutionary time remains largely unknown because ancient biogeographic variation in organism size is poorly documented. Middle Permian fusulinoidean foraminifera are <span class="hlt">ideal</span> for investigating the temporal persistence of geographic <span class="hlt">gradients</span> in organism size because they were diverse and abundant along a broad range of paleo-latitudes during this interval (~275-260 million years ago). In this study, we determined the sizes of Middle Permian fusulinoidean fossils from three different paleo-latitudinal zones in order to examine the relationship between the size of foraminifers and regional environment. We recovered the following results: keriothecal fusulinoideans are substantially larger than nonkeriothecal fusulinoideans; fusulinoideans from the equatorial zone are typically larger than those from the north and south transitional zones; neoschwagerinid specimens within a single species are generally larger in the equatorial zone than those in both transitional zones; and the nonkeriothecal fusulinoideans Staffellidae and Schubertellidae have smaller size in the north transitional zone. Fusulinoidean foraminifers differ from most other marine taxa in exhibiting larger sizes closer to the equator, contrary to Bergmann's rule. Meridional variation in seasonality, water temperature, nutrient availability, and carbonate saturation level are all likely to have favored or enabled larger sizes in equatorial regions. Temporal variation in atmospheric oxygen concentrations have been shown to account for temporal variation in fusulinoidean size during Carboniferous and Permian time, but oxygen availability appears unlikely to explain biogeographic variation in fusulinoidean sizes, because dissolved oxygen concentrations in seawater typically increase away from the equator due to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3369838','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3369838"><span>Size-Frequency Distributions along a Latitudinal <span class="hlt">Gradient</span> in Middle Permian Fusulinoideans</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Zhang, Yichun; Payne, Jonathan L.</p> <p>2012-01-01</p> <p>Geographic <span class="hlt">gradients</span> in body size within and among living species are commonly used to identify controls on the long-term evolution of organism size. However, the persistence of these <span class="hlt">gradients</span> over evolutionary time remains largely unknown because ancient biogeographic variation in organism size is poorly documented. Middle Permian fusulinoidean foraminifera are <span class="hlt">ideal</span> for investigating the temporal persistence of geographic <span class="hlt">gradients</span> in organism size because they were diverse and abundant along a broad range of paleo-latitudes during this interval (∼275–260 million years ago). In this study, we determined the sizes of Middle Permian fusulinoidean fossils from three different paleo-latitudinal zones in order to examine the relationship between the size of foraminifers and regional environment. We recovered the following results: keriothecal fusulinoideans are substantially larger than nonkeriothecal fusulinoideans; fusulinoideans from the equatorial zone are typically larger than those from the north and south transitional zones; neoschwagerinid specimens within a single species are generally larger in the equatorial zone than those in both transitional zones; and the nonkeriothecal fusulinoideans Staffellidae and Schubertellidae have smaller size in the north transitional zone. Fusulinoidean foraminifers differ from most other marine taxa in exhibiting larger sizes closer to the equator, contrary to Bergmann's rule. Meridional variation in seasonality, water temperature, nutrient availability, and carbonate saturation level are all likely to have favored or enabled larger sizes in equatorial regions. Temporal variation in atmospheric oxygen concentrations have been shown to account for temporal variation in fusulinoidean size during Carboniferous and Permian time, but oxygen availability appears unlikely to explain biogeographic variation in fusulinoidean sizes, because dissolved oxygen concentrations in seawater typically increase away from the equator due to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/897937','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/897937"><span>Kinetic Modeling of Slow Energy Release in Non-<span class="hlt">Ideal</span> Carbon Rich Explosives</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Vitello, P; Fried, L; Glaesemann, K</p> <p>2006-06-20</p> <p>We present here the first self-consistent kinetic based model for long time-scale energy release in detonation waves in the non-<span class="hlt">ideal</span> explosive LX-17. Non-<span class="hlt">ideal</span>, insensitive carbon rich explosives, such as those based on TATB, are believed to have significant late-time slow release in energy. One proposed source of this energy is diffusion-limited growth of carbon clusters. In this paper we consider the late-time energy release problem in detonation waves using the thermochemical code CHEETAH linked to a multidimensional ALE hydrodynamics model. The linked CHEETAH-ALE model dimensional treats slowly reacting chemical species using kinetic rate laws, with chemical equilibrium assumed for speciesmore » coupled via fast time-scale reactions. In the model presented here we include separate rate equations for the transformation of the un-reacted explosive to product gases and for the growth of a small particulate form of condensed graphite to a large particulate form. The small particulate graphite is assumed to be in chemical equilibrium with the gaseous species allowing for coupling between the instantaneous thermodynamic state and the production of graphite clusters. For the explosive burn rate a <span class="hlt">pressure</span> dependent rate law was used. Low <span class="hlt">pressure</span> freezing of the gas species mass fractions was also included to account for regions where the kinetic coupling rates become longer than the hydrodynamic time-scales. The model rate parameters were calibrated using cylinder and rate-stick experimental data. Excellent long time agreement and size effect results were achieved.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/6491066','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/6491066"><span>Extracardiac conduit obstruction: initial experience in the use of Doppler echocardiography for noninvasive estimation of <span class="hlt">pressure</span> <span class="hlt">gradient</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Reeder, G S; Currie, P J; Fyfe, D A; Hagler, D J; Seward, J B; Tajik, A J</p> <p>1984-11-01</p> <p>Extracardiac valved conduits are often employed in the repair of certain complex congenital heart defects; late obstruction is a well recognized problem that usually requires catheterization for definitive diagnosis. A reliable noninvasive method for detecting conduit stenosis would be clinically useful in identifying the small proportion of patients who develop this problem. Continuous wave Doppler echocardiography has been used successfully to estimate cardiac valvular obstructive lesions noninvasively. Twenty-three patients with prior extracardiac conduit placement for complex congenital heart disease underwent echocardiographic and continuous wave Doppler echocardiographic examinations to determine the presence and severity of conduit stenosis. In 20 of the 23 patients, an adequate conduit flow velocity profile was obtained, and in 10 an abnormally increased conduit flow velocity was present. All but one patient had significant obstruction proven at surgery and in one patient, surgery was planned. In three patients, an adequate conduit flow velocity profile could not be obtained but obstruction was still suspected based on high velocity tricuspid regurgitant Doppler signals. In these three patients, subsequent surgery also proved that conduit stenosis was present. Doppler-predicted <span class="hlt">gradients</span> and right ventricular <span class="hlt">pressures</span> showed an overall good correlation (r = 0.90) with measurements at subsequent cardiac catheterization. Continuous wave Doppler echocardiography appears to be a useful noninvasive tool for the detection and semiquantitation of extracardiac conduit stenosis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4094860','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4094860"><span><span class="hlt">Ideal</span> Theory in Semigroups Based on Intersectional Soft Sets</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Song, Seok Zun; Jun, Young Bae</p> <p>2014-01-01</p> <p>The notions of int-soft semigroups and int-soft left (resp., right) <span class="hlt">ideals</span> are introduced, and several properties are investigated. Using these notions and the notion of inclusive set, characterizations of subsemigroups and left (resp., right) <span class="hlt">ideals</span> are considered. Using the notion of int-soft products, characterizations of int-soft semigroups and int-soft left (resp., right) <span class="hlt">ideals</span> are discussed. We prove that the soft intersection of int-soft left (resp., right) <span class="hlt">ideals</span> (resp., int-soft semigroups) is also int-soft left (resp., right) <span class="hlt">ideals</span> (resp., int-soft semigroups). The concept of int-soft quasi-<span class="hlt">ideals</span> is also introduced, and characterization of a regular semigroup is discussed. PMID:25101310</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21775063','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21775063"><span>New calibration method for I-scan sensors to enable the precise measurement of <span class="hlt">pressures</span> delivered by '<span class="hlt">pressure</span> garments'.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Macintyre, Lisa</p> <p>2011-11-01</p> <p>Accurate measurement of the <span class="hlt">pressure</span> delivered by medical compression products is highly desirable both in monitoring treatment and in developing new <span class="hlt">pressure</span> inducing garments or products. There are several complications in measuring <span class="hlt">pressure</span> at the garment/body interface and at present no <span class="hlt">ideal</span> <span class="hlt">pressure</span> measurement tool exists for this purpose. This paper summarises a thorough evaluation of the accuracy and reproducibility of measurements taken following both of Tekscan Inc.'s recommended calibration procedures for I-scan sensors; and presents an improved method for calibrating and using I-scan <span class="hlt">pressure</span> sensors. The proposed calibration method enables accurate (±2.1 mmHg) measurement of <span class="hlt">pressures</span> delivered by <span class="hlt">pressure</span> garments to body parts with a circumference ≥30 cm. This method is too cumbersome for routine clinical use but is very useful, accurate and reproducible for product development or clinical evaluation purposes. Copyright © 2011 Elsevier Ltd and ISBI. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24671111','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24671111"><span>The values of wall shear stress, turbulence kinetic energy and blood <span class="hlt">pressure</span> <span class="hlt">gradient</span> are associated with atherosclerotic plaque erosion in rabbits.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sameshima, Naoki; Yamashita, Atsushi; Sato, Shinya; Matsuda, Shuntaro; Matsuura, Yunosuke; Asada, Yujiro</p> <p>2014-01-01</p> <p>To clarify the contribution of hemodynamic factors to the onset of plaque erosion in smooth muscle cell (SMC)-rich atherosclerotic plaque. We developed a rabbit model of SMC-rich atherosclerotic plaque with various degree of stenosis induced by incomplete ligation and generated three-dimensional models of five rabbit femoral arteries based on 130-162 serial histological cross-sections at 100-μm intervals per artery. We performed a computational blood flow simulation using the Reynolds-averaged Navier-Stokes model and calculated the wall shear stress (WSS), turbulence kinetic energy (TKE), blood <span class="hlt">pressure</span> (BP) and blood <span class="hlt">pressure</span> <span class="hlt">gradients</span> (BPG) in eight sections (the inlet, the stenotic portion and areas 1, 2 and 5mm from the stenotic portion) in each rabbit. We also investigated whether the magnitude of WSS or TKE was related to the presence or absence of erosive injury by evaluating six points (the locally highest, median and lowest of WSS or TKE) in each section. The magnitudes of WSS, TKE and BPG, but not BP, correlated significantly with the extent of histologically-defined plaque erosion (WSS, r=0.55, p<0.001; TKE, r=0.53, p<0.001; BPG, r=0.61, p<0.0001, n=40). The values for WSS and TKE were significantly larger at sites with, compared to without, erosive injury (n=107 and n=119 points, respectively; both p<0.0001). These results suggest that increased values of WSS, TKE and BPG considerably contribute to the onset of plaque erosion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AcO....77..168R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AcO....77..168R"><span>Plant-herbivore interactions along elevational <span class="hlt">gradient</span>: Comparison of field and common garden data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rokaya, Maan Bahadur; Dostálek, Tomáš; Münzbergová, Zuzana</p> <p>2016-11-01</p> <p>In response to climate change, various organisms tend to migrate to higher elevations and latitudes. Unequal migration rates of plants and animals are expected to result in changes in the type and intensity of their interactions such as plant-herbivore interactions. In the present study, we studied the extent of herbivore damage in Salvia nubicola along an elevational <span class="hlt">gradient</span> in Manang, central Nepal. A common garden experiment was also carried out by sowing seeds collected from different populations along the elevational <span class="hlt">gradient</span>. As expected, the extent of herbivore damage in the field was significantly lower at higher elevations, and it increased with the population size and at sites without shrubs. In the common garden experiment, herbivore damage was higher in plants originating from lower elevations and from more open habitats. While higher herbivore <span class="hlt">pressure</span> in the field at lower elevations may suggest that plants will be better protected against herbivores at lower elevations, the common garden study demonstrated the opposite. A possible explanation could be that plants from higher elevations have to adapt to extreme conditions, and lower palatability is a side effect of these adaptations. Thus, S. nubicola in the Himalayan region is likely to survive the expected higher herbivore <span class="hlt">pressure</span> caused by an upward shift of herbivores under future climate change. Future studies should attempt to elucidate generality of such a conclusion by studying multiple species along similar <span class="hlt">gradients</span>. Our results from comparison of the field and common garden study suggest that future experiments need to include comparisons in common environments to understand the expected response of plants to changes in herbivore <span class="hlt">pressure</span>.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_23 --> <div id="page_24" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="461"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19740058005&hterms=Posture+measurement+blood+pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DPosture%2Bmeasurement%2Bblood%2Bpressure','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19740058005&hterms=Posture+measurement+blood+pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DPosture%2Bmeasurement%2Bblood%2Bpressure"><span>Intrathoracic and venous <span class="hlt">pressure</span> relationships during responses to changes in body position</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Avasthey, P.; Wood, E. H.</p> <p>1974-01-01</p> <p>Simultaneous end-expiratory <span class="hlt">pressures</span>, referred to midthoracic level, in the superior and abdominal venae cavae, pericardial space, and right and left heart, were recorded without thoracotomy in three anesthetized dogs during sudden changes from supine to vertical head-up or head-down body positions. Intrathoracic and dependent great vein <span class="hlt">pressures</span> referred to midchest level (sixth thoracic vertebra) decreased and showed simple hydrostatic <span class="hlt">gradients</span> in either vertical position. However, a discontinuity in the large vein hydrostatic <span class="hlt">gradient</span> occurred just distal to the superior margin of the thorax in either body position and was resumed again above this level. It is concluded that, just as the cerebrospinal fluid and intraperitoneal <span class="hlt">pressures</span> minimize the effects of gravitational and inertial forces on the cerebral and visceral circulations, the pericardial and pleural <span class="hlt">pressures</span> have a similar role for the heart proper.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/864858','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/864858"><span><span class="hlt">Gradient</span> zone boundary control in salt <span class="hlt">gradient</span> solar ponds</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Hull, John R.</p> <p>1984-01-01</p> <p>A method and apparatus for suppressing zone boundary migration in a salt <span class="hlt">gradient</span> solar pond includes extending perforated membranes across the pond at the boundaries, between the convective and non-convective zones, the perforations being small enough in size to prevent individual turbulence disturbances from penetrating the hole, but being large enough to allow easy molecular diffusion of salt thereby preventing the formation of convective zones in the <span class="hlt">gradient</span> layer. The total area of the perforations is a sizable fraction of the membrane area to allow sufficient salt diffusion while preventing turbulent entrainment into the <span class="hlt">gradient</span> zone.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5848244','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/5848244"><span><span class="hlt">Gradient</span> zone-boundary control in salt-<span class="hlt">gradient</span> solar ponds</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Hull, J.R.</p> <p>1982-09-29</p> <p>A method and apparatus for suppressing zone boundary migration in a salt <span class="hlt">gradient</span> solar pond includes extending perforated membranes across the pond at the boundaries, between the convective and non-convective zones, the perforations being small enough in size to prevent individual turbulence disturbances from penetrating the hole, but being large enough to allow easy molecular diffusion of salt thereby preventing the formation of convective zones in the <span class="hlt">gradient</span> layer. The total area of the perforations is a sizeable fraction of the membrane area to allow sufficient salt diffusion while preventing turbulent entrainment into the <span class="hlt">gradient</span> zone.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/5004819','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/5004819"><span>Maintaining <span class="hlt">ideal</span> body weight counseling sessions</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Brammer, S.H.</p> <p></p> <p>The purpose of this program is to provide employees with the motivation, knowledge and skills necessary to maintain <span class="hlt">ideal</span> body weight throughout life. The target audience for this program, which is conducted in an industrial setting, is the employee 40 years of age or younger who is at or near his/her <span class="hlt">ideal</span> body weight.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28435203','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28435203"><span>Dai-Kou type conjugate <span class="hlt">gradient</span> methods with a line search only using <span class="hlt">gradient</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Huang, Yuanyuan; Liu, Changhe</p> <p>2017-01-01</p> <p>In this paper, the Dai-Kou type conjugate <span class="hlt">gradient</span> methods are developed to solve the optimality condition of an unconstrained optimization, they only utilize <span class="hlt">gradient</span> information and have broader application scope. Under suitable conditions, the developed methods are globally convergent. Numerical tests and comparisons with the PRP+ conjugate <span class="hlt">gradient</span> method only using <span class="hlt">gradient</span> show that the methods are efficient.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=man&pg=5&id=EJ872227','ERIC'); return false;" href="https://eric.ed.gov/?q=man&pg=5&id=EJ872227"><span>The <span class="hlt">Ideal</span> Man and Woman According to University Students</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Weinstein, Lawrence; Laverghetta, Antonio V.; Peterson, Scott A.</p> <p>2009-01-01</p> <p>The present study determined if the <span class="hlt">ideal</span> man has changed over the years and who and what the <span class="hlt">ideal</span> woman is. We asked students at Cameron University to rate the importance of character traits that define the <span class="hlt">ideal</span> man and woman. Subjects also provided examples of famous people exemplifying the <span class="hlt">ideal</span>, good, average, and inferior man and woman. We…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.2564T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.2564T"><span>Microseismicity Induced by Fluid <span class="hlt">Pressure</span> Drop (Laboratory Study)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Turuntaev, Sergey; Zenchenko, Evgeny; Melchaeva, Olga</p> <p>2013-04-01</p> <p> <span class="hlt">gradient</span> maximal values. The model of AE relation with the pore <span class="hlt">pressure</span> <span class="hlt">gradient</span> was considered based on the following assumptions: AE event occurred when the pore <span class="hlt">pressure</span> <span class="hlt">gradient</span> reaches some critical value; the critical value varies and can be described by Weibull distribution. Permeability variation during the fluid <span class="hlt">pressure</span> drop was estimated by means of fluid <span class="hlt">pressure</span> data and pore-elastic equation solution for small time intervals (0.01 sec). The study showed possibility to solve both a direct problem of microseismicity variation relation with fluid <span class="hlt">pressure</span> changes and an inverse problem of defining permeability by registering microseismic activity variation in particular volume of porous medium alongside with pore <span class="hlt">pressure</span> measurements at some point.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/758787','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/758787"><span>Geothermal Resource/Reservoir Investigations Based on Heat Flow and Thermal <span class="hlt">Gradient</span> Data for the United States</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>D. D. Blackwell; K. W. Wisian; M. C. Richards</p> <p>2000-04-01</p> <p>Several activities related to geothermal resources in the western United States are described in this report. A database of geothermal site-specific thermal <span class="hlt">gradient</span> and heat flow results from individual exploration wells in the western US has been assembled. Extensive temperature <span class="hlt">gradient</span> and heat flow exploration data from the active exploration of the 1970's and 1980's were collected, compiled, and synthesized, emphasizing previously unavailable company data. Examples of the use and applications of the database are described. The database and results are available on the world wide web. In this report numerical models are used to establish basic qualitative relationships betweenmore » structure, heat input, and permeability distribution, and the resulting geothermal system. A series of steady state, two-dimensional numerical models evaluate the effect of permeability and structural variations on an <span class="hlt">idealized</span>, generic Basin and Range geothermal system and the results are described.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DPPYI2006D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DPPYI2006D"><span>Density-<span class="hlt">Gradient</span>-Driven trapped-electron-modes in improved-confinement RFP plasmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Duff, James</p> <p>2016-10-01</p> <p>Short wavelength density fluctuations in improved-confinement MST plasmas exhibit multiple features characteristic of the trapped-electron-mode (TEM), strong evidence that drift wave turbulence emerges in RFP plasmas when transport associated with MHD tearing is reduced. Core transport in the RFP is normally governed by magnetic stochasticity stemming from long wavelength tearing modes that arise from current profile peaking. Using inductive control, the tearing modes are reduced and global confinement is increased to values expected for a comparable tokamak plasma. The improved confinement is associated with a large increase in the <span class="hlt">pressure</span> <span class="hlt">gradient</span> that can destabilize drift waves. The measured density fluctuations have frequencies >50 kHz, wavenumbers k_phi*rho_s<0.14, and propagate in the electron drift direction. Their spectral emergence coincides with a sharp decrease in fluctuations associated with global tearing modes. Their amplitude increases with the local density <span class="hlt">gradient</span>, and they exhibit a density-<span class="hlt">gradient</span> threshold at R/L_n 15, higher than in tokamak plasmas by R/a. the GENE code, modified for RFP equilibria, predicts the onset of microinstability for these strong-<span class="hlt">gradient</span> plasma conditions. The density-<span class="hlt">gradient</span>-driven TEM is the dominant instability in the region where the measured density fluctuations are largest, and the experimental threshold-<span class="hlt">gradient</span> is close to the predicted critical <span class="hlt">gradient</span> for linear stability. While nonlinear analysis shows a large Dimits shift associated with predicted strong zonal flows, the inclusion of residual magnetic fluctuations causes a collapse of the zonal flows and an increase in the predicted transport to a level close to the experimentally measured heat flux. Similar circumstances could occur in the edge region of tokamak plasmas when resonant magnetic perturbations are applied for the control of ELMs. Work supported by US DOE.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013APS..DFDD21003K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013APS..DFDD21003K"><span>Application of the High <span class="hlt">Gradient</span> hydrodynamics code to simulations of a two-dimensional zero-<span class="hlt">pressure-gradient</span> turbulent boundary layer over a flat plate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kaiser, Bryan E.; Poroseva, Svetlana V.; Canfield, Jesse M.; Sauer, Jeremy A.; Linn, Rodman R.</p> <p>2013-11-01</p> <p>The High <span class="hlt">Gradient</span> hydrodynamics (HIGRAD) code is an atmospheric computational fluid dynamics code created by Los Alamos National Laboratory to accurately represent flows characterized by sharp <span class="hlt">gradients</span> in velocity, concentration, and temperature. HIGRAD uses a fully compressible finite-volume formulation for explicit Large Eddy Simulation (LES) and features an advection scheme that is second-order accurate in time and space. In the current study, boundary conditions implemented in HIGRAD are varied to find those that better reproduce the reduced physics of a flat plate boundary layer to compare with complex physics of the atmospheric boundary layer. Numerical predictions are compared with available DNS, experimental, and LES data obtained by other researchers. High-order turbulence statistics are collected. The Reynolds number based on the free-stream velocity and the momentum thickness is 120 at the inflow and the Mach number for the flow is 0.2. Results are compared at Reynolds numbers of 670 and 1410. A part of the material is based upon work supported by NASA under award NNX12AJ61A and by the Junior Faculty UNM-LANL Collaborative Research Grant.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29698471','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29698471"><span>Dose <span class="hlt">gradient</span> curve: A new tool for evaluating dose <span class="hlt">gradient</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sung, KiHoon; Choi, Young Eun</p> <p>2018-01-01</p> <p>Stereotactic radiotherapy, which delivers an ablative high radiation dose to a target volume for maximum local tumor control, requires a rapid dose fall-off outside the target volume to prevent extensive damage to nearby normal tissue. Currently, there is no tool to comprehensively evaluate the dose <span class="hlt">gradient</span> near the target volume. We propose the dose <span class="hlt">gradient</span> curve (DGC) as a new tool to evaluate the quality of a treatment plan with respect to the dose fall-off characteristics. The average distance between two isodose surfaces was represented by the dose <span class="hlt">gradient</span> index (DGI) estimated by a simple equation using the volume and surface area of isodose levels. The surface area was calculated by mesh generation and surface triangulation. The DGC was defined as a plot of the DGI of each dose interval as a function of the dose. Two types of DGCs, differential and cumulative, were generated. The performance of the DGC was evaluated using stereotactic radiosurgery plans for virtual targets. Over the range of dose distributions, the dose <span class="hlt">gradient</span> of each dose interval was well-characterized by the DGC in an easily understandable graph format. Significant changes in the DGC were observed reflecting the differences in planning situations and various prescription doses. The DGC is a rational method for visualizing the dose <span class="hlt">gradient</span> as the average distance between two isodose surfaces; the shorter the distance, the steeper the dose <span class="hlt">gradient</span>. By combining the DGC with the dose-volume histogram (DVH) in a single plot, the DGC can be utilized to evaluate not only the dose <span class="hlt">gradient</span> but also the target coverage in routine clinical practice.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5919624','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5919624"><span>Dose <span class="hlt">gradient</span> curve: A new tool for evaluating dose <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Choi, Young Eun</p> <p>2018-01-01</p> <p>Purpose Stereotactic radiotherapy, which delivers an ablative high radiation dose to a target volume for maximum local tumor control, requires a rapid dose fall-off outside the target volume to prevent extensive damage to nearby normal tissue. Currently, there is no tool to comprehensively evaluate the dose <span class="hlt">gradient</span> near the target volume. We propose the dose <span class="hlt">gradient</span> curve (DGC) as a new tool to evaluate the quality of a treatment plan with respect to the dose fall-off characteristics. Methods The average distance between two isodose surfaces was represented by the dose <span class="hlt">gradient</span> index (DGI) estimated by a simple equation using the volume and surface area of isodose levels. The surface area was calculated by mesh generation and surface triangulation. The DGC was defined as a plot of the DGI of each dose interval as a function of the dose. Two types of DGCs, differential and cumulative, were generated. The performance of the DGC was evaluated using stereotactic radiosurgery plans for virtual targets. Results Over the range of dose distributions, the dose <span class="hlt">gradient</span> of each dose interval was well-characterized by the DGC in an easily understandable graph format. Significant changes in the DGC were observed reflecting the differences in planning situations and various prescription doses. Conclusions The DGC is a rational method for visualizing the dose <span class="hlt">gradient</span> as the average distance between two isodose surfaces; the shorter the distance, the steeper the dose <span class="hlt">gradient</span>. By combining the DGC with the dose-volume histogram (DVH) in a single plot, the DGC can be utilized to evaluate not only the dose <span class="hlt">gradient</span> but also the target coverage in routine clinical practice. PMID:29698471</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5217757','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5217757"><span><span class="hlt">Gradient</span> Pre-Emphasis to Counteract First-Order Concomitant Fields on Asymmetric MRI <span class="hlt">Gradient</span> Systems</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Tao, Shengzhen; Weavers, Paul T.; Trzasko, Joshua D.; Shu, Yunhong; Huston, John; Lee, Seung-Kyun; Frigo, Louis M.; Bernstein, Matt A.</p> <p>2016-01-01</p> <p>PURPOSE To develop a <span class="hlt">gradient</span> pre-emphasis scheme that prospectively counteracts the effects of the first-order concomitant fields for any arbitrary <span class="hlt">gradient</span> waveform played on asymmetric <span class="hlt">gradient</span> systems, and to demonstrate the effectiveness of this approach using a real-time implementation on a compact <span class="hlt">gradient</span> system. METHODS After reviewing the first-order concomitant fields that are present on asymmetric <span class="hlt">gradients</span>, a generalized <span class="hlt">gradient</span> pre-emphasis model assuming arbitrary <span class="hlt">gradient</span> waveforms is developed to counteract their effects. A numerically straightforward, simple to implement approximate solution to this pre-emphasis problem is derived, which is compatible with the current hardware infrastructure used on conventional MRI scanners for eddy current compensation. The proposed method was implemented on the <span class="hlt">gradient</span> driver sub-system, and its real-time use was tested using a series of phantom and in vivo data acquired from 2D Cartesian phase-difference, echo-planar imaging (EPI) and spiral acquisitions. RESULTS The phantom and in vivo results demonstrate that unless accounted for, first-order concomitant fields introduce considerable phase estimation error into the measured data and result in images exhibiting spatially dependent blurring/distortion. The resulting artifacts are effectively prevented using the proposed <span class="hlt">gradient</span> pre-emphasis. CONCLUSION An efficient and effective <span class="hlt">gradient</span> pre-emphasis framework is developed to counteract the effects of first-order concomitant fields of asymmetric <span class="hlt">gradient</span> systems. PMID:27373901</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27220209','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27220209"><span>Latitudinal <span class="hlt">gradients</span> in ecosystem engineering by oysters vary across habitats.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>McAfee, Dominic; Cole, Victoria J; Bishop, Melanie J</p> <p>2016-04-01</p> <p>Ecological theory predicts that positive interactions among organisms will increase across <span class="hlt">gradients</span> of increasing abiotic stress or consumer <span class="hlt">pressure</span>. This theory has been supported by empirical studies examining the magnitude of ecosystem engineering across environmental <span class="hlt">gradients</span> and between habitat settings at local scale. Predictions that habitat setting, by modifying both biotic and abiotic factors, will determine large-scale <span class="hlt">gradients</span> in ecosystem engineering have not been tested, however. A combination of manipulative experiments and field surveys assessed whether along the east Australian coastline: (1) facilitation of invertebrates by the oyster Saccostrea glomerata increased across a latitudinal <span class="hlt">gradient</span> in temperature; and (2) the magnitude of this effect varied between intertidal rocky shores and mangrove forests. It was expected that on rocky shores, where oysters are the primary ecosystem engineer, they would play a greater role in ameliorating latitudinal <span class="hlt">gradients</span> in temperature than in mangroves, where they are a secondary ecosystem engineer living under the mangrove canopy. On rocky shores, the enhancement of invertebrate abundance in oysters as compared to bare microhabitat decreased with latitude, as the maximum temperatures experienced by intertidal organisms diminished. By contrast, in mangrove forests, where the mangrove canopy resulted in maximum temperatures that were cooler and of greater humidity than on rocky shores, we found no evidence of latitudinal <span class="hlt">gradients</span> of oyster effects on invertebrate abundance. Contrary to predictions, the magnitude by which oysters enhanced biodiversity was in many instances similar between mangroves and rocky shores. Whether habitat-context modifies patterns of spatial variation in the effects of ecosystem engineers on community structure will depend, in part, on the extent to which the environmental amelioration provided by an ecosystem engineer replicates that of other co-occurring ecosystem engineers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JEI....26b3011T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JEI....26b3011T"><span>Local intensity area descriptor for facial recognition in <span class="hlt">ideal</span> and noise conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tran, Chi-Kien; Tseng, Chin-Dar; Chao, Pei-Ju; Ting, Hui-Min; Chang, Liyun; Huang, Yu-Jie; Lee, Tsair-Fwu</p> <p>2017-03-01</p> <p>We propose a local texture descriptor, local intensity area descriptor (LIAD), which is applied for human facial recognition in <span class="hlt">ideal</span> and noisy conditions. Each facial image is divided into small regions from which LIAD histograms are extracted and concatenated into a single feature vector to represent the facial image. The recognition is performed using a nearest neighbor classifier with histogram intersection and chi-square statistics as dissimilarity measures. Experiments were conducted with LIAD using the ORL database of faces (Olivetti Research Laboratory, Cambridge), the Face94 face database, the Georgia Tech face database, and the FERET database. The results demonstrated the improvement in accuracy of our proposed descriptor compared to conventional descriptors [local binary pattern (LBP), uniform LBP, local ternary pattern, histogram of oriented <span class="hlt">gradients</span>, and local directional pattern]. Moreover, the proposed descriptor was less sensitive to noise and had low histogram dimensionality. Thus, it is expected to be a powerful texture descriptor that can be used for various computer vision problems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28621353','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28621353"><span>Ternary <span class="hlt">gradient</span> metal-organic frameworks.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Chong; Rosi, Nathaniel L</p> <p>2017-09-08</p> <p><span class="hlt">Gradient</span> MOFs contain directional <span class="hlt">gradients</span> of either structure or functionality. We have successfully prepared two ternary <span class="hlt">gradient</span> MOFs based on bMOF-100 analogues, namely bMOF-100/102/106 and bMOF-110/100/102, via cascade ligand exchange reactions. The cubic unit cell parameter discrepancy within an individual ternary <span class="hlt">gradient</span> MOF crystal is as large as ∼1 nm, demonstrating the impressive compatibility and flexibility of the component MOF materials. Because of the presence of a continuum of unit cells, the pore diameters within individual crystals also change in a <span class="hlt">gradient</span> fashion from ∼2.5 nm to ∼3.0 nm for bMOF-100/102/106, and from ∼2.2 nm to ∼2.7 nm for bMOF-110/100/102, indicating significant porosity <span class="hlt">gradients</span>. Like previously reported binary <span class="hlt">gradient</span> MOFs, the composition of the ternary <span class="hlt">gradient</span> MOFs can be easily controlled by adjusting the reaction conditions. Finally, X-ray diffraction and microspectrophotometry were used to analyse fractured <span class="hlt">gradient</span> MOF crystals by comparing unit cell parameters and absorbance spectra at different locations, thus revealing the profile of heterogeneity (i.e. <span class="hlt">gradient</span> distribution of properties) and further confirming the formation of ternary <span class="hlt">gradient</span> MOFs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27939381','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27939381"><span>Impact of Elevated End-Diastolic Pulmonary Regurgitation <span class="hlt">Gradient</span> on Worse Clinical Outcomes in Hospitalized Patients With Heart Failure.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Honda, Yasuyuki; Nagai, Toshiyuki; Sugano, Yasuo; Honda, Satoshi; Okada, Atsushi; Asaumi, Yasuhide; Aiba, Takeshi; Noguchi, Teruo; Kusano, Kengo; Ogawa, Hisao; Yasuda, Satoshi; Anzai, Toshihisa</p> <p>2017-02-15</p> <p>The echo Doppler end-diastolic pulmonary regurgitation (EDPR) <span class="hlt">gradient</span> correlates well with catheter-derived pulmonary artery diastolic <span class="hlt">pressure</span>. An elevated EDPR <span class="hlt">gradient</span> is associated with worse clinical outcomes in patients with stable coronary artery disease. However, the prognostic significance of EDPR <span class="hlt">gradient</span> in patients with heart failure (HF) is unclear. The aim of the present study was to investigate the prognostic impact of EDPR <span class="hlt">gradient</span> in HF. We retrospectively examined 751 consecutive hospitalized patients with acute HF. Those with acute coronary syndrome or in-hospital death and those without accessible EDPR <span class="hlt">gradient</span> data at discharge were excluded. Finally, 265 patients were examined and divided into 2 groups according to EDPR <span class="hlt">gradient</span> (cutoff 9 mm Hg). Adverse events were defined as worsening HF and death. Patients with elevated EDPR <span class="hlt">gradient</span> had higher B-type natriuretic peptide, lower age, and lower left ventricular ejection fraction at discharge than those with nonelevated EDPR <span class="hlt">gradient</span>. During a median follow-up of 429 days, elevated EDPR <span class="hlt">gradient</span> was independently associated with adverse events (hazard ratio 2.34, 95% CI 1.44 to 3.78, p <0.001) after adjustment for confounders. In conclusion, echo Doppler EDPR <span class="hlt">gradient</span> might be a noninvasive predictor of clinical outcomes in hospitalized patients with HF. Copyright © 2016 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPA....8d5201F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPA....8d5201F"><span>Instability of a shear layer between multicomponent fluids at supercritical <span class="hlt">pressure</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fu, Qing-fei; Zhang, Yun-xiao; Mo, Chao-jie; Yang, Li-jun</p> <p>2018-04-01</p> <p>The temporal instability of a thin shear layer lying between streams of two components of fluids has been studied. The effects of density profile of the layer on the instability behavior were mainly considered. The detailed density profile was obtained through Linear <span class="hlt">Gradient</span> Theory. The eigenvalue problem was calculated, and the temporal instability curves were obtained for the thermodynamic parameters, e.g. <span class="hlt">pressure</span> and temperature. The results show that, increase of <span class="hlt">pressure</span> leads to the increase of the maximum growth rate. However, increasing <span class="hlt">pressure</span> has opposite effects on the disturbances with small and large wave length. The increase of temperature causes the decrease of disturbance growth rate. The instability behavior of the shear layers was determined mainly by the interval between the inflections of the velocity and density profiles, and the maximum density <span class="hlt">gradient</span>. The total effects, determined by coupling density stratification, and interval between the inflections of the velocity and density profiles, were quite distinct for different ranges of temperature and <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.4586L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.4586L"><span>Trace metal concentrations in forest and lawn soils of Paris region (France) along a <span class="hlt">gradient</span> of urban <span class="hlt">pressure</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ludovic, Foti</p> <p>2017-04-01</p> <p> concentrations and subsequent risks in soils of Paris and Paris region (Île-de-France). Our study aims at filling this knowledge gap, focusing on contamination and pollution by TMs in lawns and forests that constitute the main types of vegetation in urban areas of Paris region. Considering the rational described above, the aims of the present study were (i) to examine the concentration of eight selected TMs (As, Cd, Cr, Cu, Fe, Ni, Pb, Zn) in soils of two land-uses (public lawns and woods) along an urban <span class="hlt">pressure</span> <span class="hlt">gradient</span> in Paris region, (ii) to distinguish origins and sources of contamination or pollution, (iii) to evaluate the individual and overall TM contamination degree as well as the individual and overall TM pollution degree, (iiii) to use soil characteristics to better understand soil origins and histories along the urban <span class="hlt">pressure</span> <span class="hlt">gradient</span> and the relationship between these characteristics and TM concentrations. Ultimately, this study provides a baseline TM assessment for the long-term monitoring of the evolution of TM soil contents in urban area of the Paris region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004AGUFM.T43B1327H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004AGUFM.T43B1327H"><span>Relationships between heat flow, thermal and <span class="hlt">pressure</span> fields in the Gulf of Mexico</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Husson, L.; Henry, P.; Le Pichon, X.</p> <p>2004-12-01</p> <p>The thermal field of the Gulf of Mexico (GoM) is restored from a comprehensive temperature-depth database. A striking feature is the systematic sharp <span class="hlt">gradient</span> increase between 2500 and 4000 m. The analysis of the <span class="hlt">pressure</span> (fracturation tests and mud weights) indicates a systematic correlation between the <span class="hlt">pressure</span> and temperature fields, as well as with the thickness of Plio-Pleistocene sedimentary layer, and is interpreted as the fact of cooling from fluid flow in the upper, almost hydrostatically <span class="hlt">pressured</span> layer. The Nusselt number, that we characterize by the ratio between the near high-P <span class="hlt">gradient</span> over low-P <span class="hlt">gradient</span> varies spatially and is correlated to the structural pattern of the GoM; this observation outlines the complex relationships between heat and fluid flows, structure and sedimentation. The deep thermal signal is restored in terms of <span class="hlt">gradient</span> and heat flow density from a statistical analysis of the thermal data combined to the thermal modelling of about 175 wells. At a regional scale, although the sedimentary cover is warmer in Texas than in Louisiana in terms of temperature, the steady state basal heat flow is higher in Louisiana. In addition, beneath the Corsair Fault, which lay offshore parallel to the Texan coast, the high heat flow suggests a zone of Tertiary lithospheric thinning.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_24 --> <div id="page_25" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="481"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/6020818','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/6020818"><span>Determination of some pure compound <span class="hlt">ideal</span>-gas enthalpies of formation</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Steele, W. V.; Chirico, R. D.; Nguyen, A.</p> <p>1989-06-01</p> <p>The results of a study aimed at improvement of group-additivity methodology for estimation of thermodynamic properties of organic substances are reported. Specific weaknesses where ring corrections were unknown or next-nearest-neighbor interactions were only estimated because of lack of experimental data are addressed by experimental studies of enthalpies of combustion in the condensed- phase and vapor <span class="hlt">pressure</span> measurements. <span class="hlt">Ideal</span>-gas enthalpies of formation are reported for acrylamide, succinimide, ..gamma..-butyrolactone, 2-pyrrolidone, 2,3-dihydrofuran, 3,4-dihydro-2H-pyran, 1,3-cyclohexadiene, 1,4-cyclohexadiene, and 1-methyl-1-phenylhydrazine. Ring corrections, group terms, and next-nearest-neighbor interaction terms useful in the application of group additivity correlations are derived. 44 refs., 2 figs., 59 tabs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.9957H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.9957H"><span>Quantification of the effect of temperature <span class="hlt">gradients</span> in soils on subsurface radon signal</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Haquin, Gustavo; Ilzycer, Danielle; Kamai, Tamir; Zafrir, Hovav; Weisbrod, Noam</p> <p>2017-04-01</p> <p>Temperature <span class="hlt">gradients</span> that develop in soils due to atmospheric temperature cycles are factors of primary importance in determining the rates and directions of subsurface gas flow. Models including mechanisms of thermal convection and thermal diffusion partially explain the impact of temperature <span class="hlt">gradients</span> on subsurface radon transport. However, the overall impact of temperature <span class="hlt">gradients</span> on subsurface radon transport is still not well understood. A laboratory setup was designed and built to experimentally investigate the influence of temperature <span class="hlt">gradients</span> on radon transport under well controlled conditions. A 60 cm diameter and 120 cm tall column was thermally insulated except from the atmosphere-soil interface, such that it was constructed to simulate field conditions where temperature <span class="hlt">gradients</span> in soils are developed following atmospheric temperature cycles. The column was filled with fine grinded phosphate rock which provided the porous media with radon source. Radon in soil-air was continuously monitored using NaI gamma detectors positioned at different heights along the column. Soil temperature, differential <span class="hlt">pressure</span>, and relative humidity were monitored along the column. Experiments based on steep and gradual stepwise changes in ambient temperature were conducted. Absolute changes on radon levels in the order of 10-30% were measured at temperature <span class="hlt">gradients</span> of up to ±20oC/m. Results showed a non-linear correlation between the temperature <span class="hlt">gradient</span> and the subsurface radon concentration. An asymmetric relationship between the radon concentration and the temperature <span class="hlt">gradients</span> for ΔT>0 and ΔT<0 was also observed. Laboratory simulations of the time- and depth-dependent temperature wave functions with frequencies ranged from a daily cycle to few days were performed. In response to the harmonic temperature behaviour radon oscillations at similar frequencies were detected correspondingly. In this work a quantitative relationship between radon and temperature</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28092550','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28092550"><span>$L_{0}$ <span class="hlt">Gradient</span> Projection.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ono, Shunsuke</p> <p>2017-04-01</p> <p>Minimizing L 0 <span class="hlt">gradient</span>, the number of the non-zero <span class="hlt">gradients</span> of an image, together with a quadratic data-fidelity to an input image has been recognized as a powerful edge-preserving filtering method. However, the L 0 <span class="hlt">gradient</span> minimization has an inherent difficulty: a user-given parameter controlling the degree of flatness does not have a physical meaning since the parameter just balances the relative importance of the L 0 <span class="hlt">gradient</span> term to the quadratic data-fidelity term. As a result, the setting of the parameter is a troublesome work in the L 0 <span class="hlt">gradient</span> minimization. To circumvent the difficulty, we propose a new edge-preserving filtering method with a novel use of the L 0 <span class="hlt">gradient</span>. Our method is formulated as the minimization of the quadratic data-fidelity subject to the hard constraint that the L 0 <span class="hlt">gradient</span> is less than a user-given parameter α . This strategy is much more intuitive than the L 0 <span class="hlt">gradient</span> minimization because the parameter α has a clear meaning: the L 0 <span class="hlt">gradient</span> value of the output image itself, so that one can directly impose a desired degree of flatness by α . We also provide an efficient algorithm based on the so-called alternating direction method of multipliers for computing an approximate solution of the nonconvex problem, where we decompose it into two subproblems and derive closed-form solutions to them. The advantages of our method are demonstrated through extensive experiments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/7614499','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/7614499"><span>Reappraisal of quantitative evaluation of pulmonary regurgitation and estimation of pulmonary artery <span class="hlt">pressure</span> by continuous wave Doppler echocardiography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lei, M H; Chen, J J; Ko, Y L; Cheng, J J; Kuan, P; Lien, W P</p> <p>1995-01-01</p> <p>This study assessed the usefulness of continuous wave Doppler echocardiography and color flow mapping in evaluating pulmonary regurgitation (PR) and estimating pulmonary artery (PA) <span class="hlt">pressure</span>. Forty-three patients were examined, and high quality Doppler spectral recordings of PR were obtained in 32. All patients underwent cardiac catheterization, and simultaneous PA and right ventricular (RV) <span class="hlt">pressures</span> were recorded in 17. Four Doppler regurgitant flow velocity patterns were observed: pandiastolic plateau, biphasic, peak and plateau, and early diastolic triangular types. The peak diastolic and end-diastolic PA-to-RV <span class="hlt">pressure</span> <span class="hlt">gradients</span> derived from the Doppler flow profiles correlated well with the catheter measurements (r = 0.95 and r = 0.95, respectively). As PA <span class="hlt">pressure</span> increased, the PR flow velocity became higher; a linear relationship between either systolic or mean PA <span class="hlt">pressure</span> and Doppler-derived peak diastolic <span class="hlt">pressure</span> <span class="hlt">gradient</span> was noted (r = 0.90 and 0.94, respectively). Based on peak diastolic <span class="hlt">gradients</span> of < 15, 15-30 or > 30 mm Hg, patients could be separated as those with mild, moderate or severe pulmonary hypertension, respectively (p < 0.05). A correlation was also observed between PA diastolic <span class="hlt">pressure</span> and Doppler-derived end-diastolic <span class="hlt">pressure</span> <span class="hlt">gradient</span> (r = 0.91). Moreover, the Doppler velocity decay slope of PR closely correlated with that derived from the catheter method (r = 0.98). The decay slope tended to be steeper with the increment in regurgitant jet area and length obtained from color flow mapping. In conclusion, continuous wave Doppler evaluation of PR is a useful means for noninvasive estimation of PA <span class="hlt">pressure</span>, and the Doppler velocity decay slope seems to reflect the severity of PR.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27373901','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27373901"><span><span class="hlt">Gradient</span> pre-emphasis to counteract first-order concomitant fields on asymmetric MRI <span class="hlt">gradient</span> systems.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tao, Shengzhen; Weavers, Paul T; Trzasko, Joshua D; Shu, Yunhong; Huston, John; Lee, Seung-Kyun; Frigo, Louis M; Bernstein, Matt A</p> <p>2017-06-01</p> <p>To develop a <span class="hlt">gradient</span> pre-emphasis scheme that prospectively counteracts the effects of the first-order concomitant fields for any arbitrary <span class="hlt">gradient</span> waveform played on asymmetric <span class="hlt">gradient</span> systems, and to demonstrate the effectiveness of this approach using a real-time implementation on a compact <span class="hlt">gradient</span> system. After reviewing the first-order concomitant fields that are present on asymmetric <span class="hlt">gradients</span>, we developed a generalized <span class="hlt">gradient</span> pre-emphasis model assuming arbitrary <span class="hlt">gradient</span> waveforms to counteract their effects. A numerically straightforward, easily implemented approximate solution to this pre-emphasis problem was derived that was compatible with the current hardware infrastructure of conventional MRI scanners for eddy current compensation. The proposed method was implemented on the <span class="hlt">gradient</span> driver subsystem, and its real-time use was tested using a series of phantom and in vivo data acquired from two-dimensional Cartesian phase-difference, echo-planar imaging, and spiral acquisitions. The phantom and in vivo results demonstrated that unless accounted for, first-order concomitant fields introduce considerable phase estimation error into the measured data and result in images with spatially dependent blurring/distortion. The resulting artifacts were effectively prevented using the proposed <span class="hlt">gradient</span> pre-emphasis. We have developed an efficient and effective <span class="hlt">gradient</span> pre-emphasis framework to counteract the effects of first-order concomitant fields of asymmetric <span class="hlt">gradient</span> systems. Magn Reson Med 77:2250-2262, 2017. © 2016 International Society for Magnetic Resonance in Medicine. © 2016 International Society for Magnetic Resonance in Medicine.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15233670','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15233670"><span>The cost-effectiveness of hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> monitoring in the prevention of recurrent variceal hemorrhage.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Targownik, Laura E; Spiegel, Brennan M R; Dulai, Gareth S; Karsan, Hetal A; Gralnek, Ian M</p> <p>2004-07-01</p> <p>Recurrent variceal hemorrhage is common following an initial bleed in patients with cirrhosis. The current standard of care for secondary prophylaxis is endoscopic band ligation (EBL). Combination of beta-blocker and nitrate therapy, guided by hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> (HVPG) monitoring, is a novel alternative strategy. We sought to determine the cost-effectiveness of these competing strategies. Decision analysis with Markov modeling was used to calculate the cost-effectiveness of three competing strategies: (1) EBL; (2) beta-blocker and nitrate therapy without HVPG monitoring (HVPG-); and (3) beta-blocker and nitrate therapy with HVPG monitoring (HVPG+). Patients in the HVPG+ strategy who failed to achieve an HVPG decline from medical therapy were offered EBL. Cost estimates were from a third-party payer perspective. The main outcome measure was the cost per recurrent variceal hemorrhage prevented. Under base-case conditions, the HVPG+ strategy was the most effective yet most expensive approach, followed by EBL and HVPG-. Compared to the EBL strategy, the HVPG+ strategy cost an incremental 5,974 dollars per recurrent bleed prevented. In a population with 100% compliance with all therapies, the incremental cost of HVPG-versus EBL fell to 5,270 dollars per recurrent bleed prevented. The model results were sensitive to the cost of EBL, the cost of HVPG monitoring, and the probability of medical therapy producing an adequate HVPG decline. Compared to EBL for the secondary prophylaxis of variceal rebleeding, combination medical therapy guided by HVPG monitoring is more effective and only marginally more expensive.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28523153','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28523153"><span>Pleural <span class="hlt">pressure</span> theory revisited: a role for capillary equilibrium.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Casha, Aaron R; Caruana-Gauci, Roberto; Manche, Alexander; Gauci, Marilyn; Chetcuti, Stanley; Bertolaccini, Luca; Scarci, Marco</p> <p>2017-04-01</p> <p>Theories elucidating pleural <span class="hlt">pressures</span> should explain all observations including the equal and opposite recoil of the chest wall and lungs, the less than expected pleural hydrostatic <span class="hlt">gradient</span> and its variation at lobar margins, why pleural <span class="hlt">pressures</span> are negative and how pleural fluid circulation functions. A theoretical model describing equilibrium between buoyancy, hydrostatic forces, and capillary forces is proposed. The capillary equilibrium model described depends on control of pleural fluid volume and protein content, powered by an active pleural pump. The interaction between buoyancy forces, hydrostatic <span class="hlt">pressure</span> and capillary <span class="hlt">pressure</span> was calculated, and values for pleural thickness and <span class="hlt">pressure</span> were determined using values for surface tension, contact angle, pleural fluid and lung densities found in the literature. Modelling can explain the issue of the differing hydrostatic vertical pleural <span class="hlt">pressure</span> <span class="hlt">gradient</span> at the lobar margins for buoyancy forces between the pleural fluid and the lung floating in the pleural fluid according to Archimedes' hydrostatic paradox. The capillary equilibrium model satisfies all salient requirements for a pleural <span class="hlt">pressure</span> model, with negative <span class="hlt">pressures</span> maximal at the apex, equal and opposite forces in the lung and chest wall, and circulatory pump action. This model predicts that pleural effusions cannot occur in emphysema unless concomitant heart failure increases lung density. This model also explains how the non-confluence of the lung with the chest wall (e.g., lobar margins) makes the pleural <span class="hlt">pressure</span> more negative, and why pleural <span class="hlt">pressures</span> would be higher after an upper lobectomy compared to a lower lobectomy. Pathological changes in pleural fluid composition and lung density alter the equilibrium between capillarity and buoyancy hydrostatic <span class="hlt">pressure</span> to promote pleural effusion formation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5418293','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5418293"><span>Pleural <span class="hlt">pressure</span> theory revisited: a role for capillary equilibrium</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Caruana-Gauci, Roberto; Manche, Alexander; Gauci, Marilyn; Chetcuti, Stanley; Bertolaccini, Luca</p> <p>2017-01-01</p> <p>Background Theories elucidating pleural <span class="hlt">pressures</span> should explain all observations including the equal and opposite recoil of the chest wall and lungs, the less than expected pleural hydrostatic <span class="hlt">gradient</span> and its variation at lobar margins, why pleural <span class="hlt">pressures</span> are negative and how pleural fluid circulation functions. Methods A theoretical model describing equilibrium between buoyancy, hydrostatic forces, and capillary forces is proposed. The capillary equilibrium model described depends on control of pleural fluid volume and protein content, powered by an active pleural pump. Results The interaction between buoyancy forces, hydrostatic <span class="hlt">pressure</span> and capillary <span class="hlt">pressure</span> was calculated, and values for pleural thickness and <span class="hlt">pressure</span> were determined using values for surface tension, contact angle, pleural fluid and lung densities found in the literature. Modelling can explain the issue of the differing hydrostatic vertical pleural <span class="hlt">pressure</span> <span class="hlt">gradient</span> at the lobar margins for buoyancy forces between the pleural fluid and the lung floating in the pleural fluid according to Archimedes’ hydrostatic paradox. The capillary equilibrium model satisfies all salient requirements for a pleural <span class="hlt">pressure</span> model, with negative <span class="hlt">pressures</span> maximal at the apex, equal and opposite forces in the lung and chest wall, and circulatory pump action. Conclusions This model predicts that pleural effusions cannot occur in emphysema unless concomitant heart failure increases lung density. This model also explains how the non-confluence of the lung with the chest wall (e.g., lobar margins) makes the pleural <span class="hlt">pressure</span> more negative, and why pleural <span class="hlt">pressures</span> would be higher after an upper lobectomy compared to a lower lobectomy. Pathological changes in pleural fluid composition and lung density alter the equilibrium between capillarity and buoyancy hydrostatic <span class="hlt">pressure</span> to promote pleural effusion formation. PMID:28523153</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26492727','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26492727"><span><span class="hlt">Idealism</span> and materialism in perception.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rose, David; Brown, Dora</p> <p>2015-01-01</p> <p>Koenderink (2014, Perception, 43, 1-6) has said most Perception readers are deluded, because they believe an 'All Seeing Eye' observes an objective reality. We trace the source of Koenderink's assertion to his metaphysical <span class="hlt">idealism</span>, and point to two major weaknesses in his position-namely, its dualism and foundationalism. We counter with arguments from modern philosophy of science for the existence of an objective material reality, contrast Koenderink's enactivism to his <span class="hlt">idealism</span>, and point to ways in which phenomenology and cognitive science are complementary and not mutually exclusive.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012APS..DPPVI3003P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012APS..DPPVI3003P"><span>Heating and current drive requirements for <span class="hlt">ideal</span> MHD stability and ITB sustainment in ITER steady state scenarios</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Poli, Francesca</p> <p>2012-10-01</p> <p>Steady state scenarios envisaged for ITER aim at optimizing the bootstrap current, while maintaining sufficient confinement and stability to provide the necessary fusion yield. Non-inductive scenarios will need to operate with Internal Transport Barriers (ITBs) in order to reach adequate fusion gain at typical currents of 9 MA. However, the large <span class="hlt">pressure</span> <span class="hlt">gradients</span> associated with ITBs in regions of weak or negative magnetic shear can be conducive to <span class="hlt">ideal</span> MHD instabilities in a wide range of βN, reducing the no-wall limit. Scenarios are established as relaxed flattop states with time-dependent transport simulations with TSC [1]. Fully non-inductive configurations with current in the range of 7-10 MA and various heating mixes (NB, EC, IC and LH) have been studied against variations of the <span class="hlt">pressure</span> profile peaking and of the Greenwald fraction. It is found that stable equilibria have qmin> 2 and moderate ITBs at 2/3 of the minor radius [2]. The ExB flow shear from toroidal plasma rotation is expected to be low in ITER, with a major role in the ITB dynamics being played by magnetic geometry. Combinations of H&CD sources that maintain reverse or weak magnetic shear profiles throughout the discharge and ρ(qmin)>=0.5 are the focus of this work. The ITER EC upper launcher, designed for NTM control, can provide enough current drive off-axis to sustain moderate ITBs at mid-radius and maintain a non-inductive current of 8-9MA and H98>=1.5 with the day one heating mix. LH heating and current drive is effective in modifying the current profile off-axis, facilitating the formation of stronger ITBs in the rampup phase, their sustainment at larger radii and larger bootstrap fraction. The implications for steady state operation and fusion performance are discussed.[4pt] [1] Jardin S.C. et al, J. Comput. Phys. 66 (1986) 481[0pt] [2] Poli F.M. et al, Nucl. Fusion 52 (2012) 063027.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26283413','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26283413"><span><span class="hlt">Pressure</span> and shear stress in trabecular bone marrow during whole bone loading.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Metzger, Thomas A; Schwaner, Stephen A; LaNeve, Anthony J; Kreipke, Tyler C; Niebur, Glen L</p> <p>2015-09-18</p> <p>Skeletal adaptation to mechanical loading is controlled by mechanobiological signaling. Osteocytes are highly responsive to applied strains, and are the key mechanosensory cells in bone. However, many cells residing in the marrow also respond to mechanical cues such as hydrostatic <span class="hlt">pressure</span> and shear stress, and hence could play a role in skeletal adaptation. Trabecular bone encapsulates marrow, forming a poroelastic solid. According to the mechanical theory, deformation of the pores induces motion in the fluid-like marrow, resulting in <span class="hlt">pressure</span> and velocity <span class="hlt">gradients</span>. The latter results in shear stress acting between the components of the marrow. To characterize the mechanical environment of trabecular bone marrow in situ, pore <span class="hlt">pressure</span> within the trabecular compartment of whole porcine femurs was measured with miniature <span class="hlt">pressure</span> transducers during stress-relaxation and cyclic loading. <span class="hlt">Pressure</span> <span class="hlt">gradients</span> ranging from 0.013 to 0.46 kPa/mm were measured during loading. This range was consistent with calculated <span class="hlt">pressure</span> <span class="hlt">gradients</span> from continuum scale poroelastic models with the same permeability. Micro-scale computational fluid dynamics models created from computed tomography images were used to calculate the micromechanical stress in the marrow using the measured <span class="hlt">pressure</span> differentials as boundary conditions. The volume averaged shear stress in the marrow ranged from 1.67 to 24.55 Pa during cyclic loading, which exceeds the mechanostimulatory threshold for mesenchymal lineage cells. Thus, the loading of bone through activities of daily living may be an essential component of bone marrow health and mechanobiology. Additional studies of cell-level interactions during loading in healthy and disease conditions will provide further incite into marrow mechanobiology. Copyright © 2015 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29479736','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29479736"><span><span class="hlt">Gradient</span> waveform pre-emphasis based on the <span class="hlt">gradient</span> system transfer function.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Stich, Manuel; Wech, Tobias; Slawig, Anne; Ringler, Ralf; Dewdney, Andrew; Greiser, Andreas; Ruyters, Gudrun; Bley, Thorsten A; Köstler, Herbert</p> <p>2018-02-25</p> <p>The <span class="hlt">gradient</span> system transfer function (GSTF) has been used to describe the distorted k-space trajectory for image reconstruction. The purpose of this work was to use the GSTF to determine the pre-emphasis for an undistorted <span class="hlt">gradient</span> output and intended k-space trajectory. The GSTF of the MR system was determined using only standard MR hardware without special equipment such as field probes or a field camera. The GSTF was used for trajectory prediction in image reconstruction and for a <span class="hlt">gradient</span> waveform pre-emphasis. As test sequences, a <span class="hlt">gradient</span>-echo sequence with phase-encoding <span class="hlt">gradient</span> modulation and a <span class="hlt">gradient</span>-echo sequence with a spiral read-out trajectory were implemented and subsequently applied on a structural phantom and in vivo head measurements. Image artifacts were successfully suppressed by applying the GSTF-based pre-emphasis. Equivalent results are achieved with images acquired using GSTF-based post-correction of the trajectory as a part of image reconstruction. In contrast, the pre-emphasis approach allows reconstruction using the initially intended trajectory. The artifact suppression shown for two sequences demonstrates that the GSTF can serve for a novel pre-emphasis. A pre-emphasis based on the GSTF information can be applied to any arbitrary sequence type. © 2018 International Society for Magnetic Resonance in Medicine.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/2312454','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/2312454"><span>Responses to negative <span class="hlt">pressure</span> surrounding the neck in anesthetized animals.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wolin, A D; Strohl, K P; Acree, B N; Fouke, J M</p> <p>1990-01-01</p> <p>Continuous positive <span class="hlt">pressure</span> applied at the nose has been shown to cause a decrease in upper airway resistance. The present study was designed to determine whether a similar positive transmural <span class="hlt">pressure</span> <span class="hlt">gradient</span>, generated by applying a negative <span class="hlt">pressure</span> at the body surface around the neck, altered upper airway patency. Studies were performed in nine spontaneously breathing anesthetized supine dogs. Airflow was measured with a pneumotachograph mounted on an airtight muzzle placed over the nose and mouth of each animal. Upper airway <span class="hlt">pressure</span> was measured as the differential <span class="hlt">pressure</span> between the extrathoracic trachea and the inside of the muzzle. Upper airway resistance was monitored as an index of airway patency. Negative <span class="hlt">pressure</span> (-2 to -20 cmH2O) was applied around the neck by using a cuirass extending from the jaw to the thorax. In each animal, increasingly negative <span class="hlt">pressures</span> were transmitted to the airway wall in a progressive, although not linear, fashion. Decreasing the <span class="hlt">pressure</span> produced a progressive fall in upper airway resistance, without causing a significant change in respiratory drive or respiratory timing. At -5 cmH2O <span class="hlt">pressure</span>, there occurred a significant fall in upper airway resistance, comparable with the response of a single, intravenous injection of sodium cyanide (0.5-3.0 mg), a respiratory stimulant that produces substantial increases in respiratory drive. We conclude that upper airway resistance is influenced by the transmural <span class="hlt">pressure</span> across the airway wall and that such a <span class="hlt">gradient</span> can be accomplished by making the extraluminal <span class="hlt">pressure</span> more negative.(ABSTRACT TRUNCATED AT 250 WORDS)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ApJ...827L..29S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ApJ...827L..29S"><span>The Role of Cosmic-Ray <span class="hlt">Pressure</span> in Accelerating Galactic Outflows</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Simpson, Christine M.; Pakmor, Rüdiger; Marinacci, Federico; Pfrommer, Christoph; Springel, Volker; Glover, Simon C. O.; Clark, Paul C.; Smith, Rowan J.</p> <p>2016-08-01</p> <p>We study the formation of galactic outflows from supernova (SN) explosions with the moving-mesh code AREPO in a stratified column of gas with a surface density similar to the Milky Way disk at the solar circle. We compare different simulation models for SN placement and energy feedback, including cosmic rays (CRs), and find that models that place SNe in dense gas and account for CR diffusion are able to drive outflows with similar mass loading as obtained from a random placement of SNe with no CRs. Despite this similarity, CR-driven outflows differ in several other key properties including their overall clumpiness and velocity. Moreover, the forces driving these outflows originate in different sources of <span class="hlt">pressure</span>, with the CR diffusion model relying on non-thermal <span class="hlt">pressure</span> <span class="hlt">gradients</span> to create an outflow driven by internal <span class="hlt">pressure</span> and the random-placement model depending on kinetic <span class="hlt">pressure</span> <span class="hlt">gradients</span> to propel a ballistic outflow. CRs therefore appear to be non-negligible physics in the formation of outflows from the interstellar medium.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22654242-role-cosmic-ray-pressure-accelerating-galactic-outflows','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22654242-role-cosmic-ray-pressure-accelerating-galactic-outflows"><span>THE ROLE OF COSMIC-RAY <span class="hlt">PRESSURE</span> IN ACCELERATING GALACTIC OUTFLOWS</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Simpson, Christine M.; Pakmor, Rüdiger; Pfrommer, Christoph</p> <p></p> <p>We study the formation of galactic outflows from supernova (SN) explosions with the moving-mesh code AREPO in a stratified column of gas with a surface density similar to the Milky Way disk at the solar circle. We compare different simulation models for SN placement and energy feedback, including cosmic rays (CRs), and find that models that place SNe in dense gas and account for CR diffusion are able to drive outflows with similar mass loading as obtained from a random placement of SNe with no CRs. Despite this similarity, CR-driven outflows differ in several other key properties including their overallmore » clumpiness and velocity. Moreover, the forces driving these outflows originate in different sources of <span class="hlt">pressure</span>, with the CR diffusion model relying on non-thermal <span class="hlt">pressure</span> <span class="hlt">gradients</span> to create an outflow driven by internal <span class="hlt">pressure</span> and the random-placement model depending on kinetic <span class="hlt">pressure</span> <span class="hlt">gradients</span> to propel a ballistic outflow. CRs therefore appear to be non-negligible physics in the formation of outflows from the interstellar medium.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhFl...27a6101S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhFl...27a6101S"><span>Numerical modelling of underwater detonation of non-<span class="hlt">ideal</span> condensed-phase explosives</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schoch, Stefan; Nikiforakis, Nikolaos</p> <p>2015-01-01</p> <p>The interest in underwater detonation tests originated from the military, since the expansion and subsequent collapse of the explosive bubble can cause considerable damage to surrounding structures or vessels. In military applications, the explosive is typically represented as a pre-burned material under high <span class="hlt">pressure</span>, a reasonable assumption due to the short reaction zone lengths, and complete detonation of the unreacted explosive. Hence, numerical simulations of underwater detonation tests have been primarily concerned with the prediction of target loading and the damage incurred rather than the accurate modelling of the underwater detonation process. The mining industry in contrast has adopted the underwater detonation test as a means to experimentally characterise the energy output of their highly non-<span class="hlt">ideal</span> explosives depending on explosive type and charge configuration. This characterisation requires a good understanding of how the charge shape, pond topography, charge depth, and additional charge confinement affect the energy release, some of which can be successfully quantified with the support of accurate numerical simulations. In this work, we propose a numerical framework which is able to capture the non-<span class="hlt">ideal</span> explosive behaviour and in addition is capable of capturing both length scales: the reaction zone and the pond domain. The length scale problem is overcome with adaptive mesh refinement, which, along with the explosive model, is validated against experimental data of various TNT underwater detonations. The variety of detonation and bubble behaviour observed in non-<span class="hlt">ideal</span> detonations is demonstrated in a parameter study over the reactivity of TNT. A representative underwater mining test containing an ammonium-nitrate fuel-oil ratestick charge is carried out to demonstrate that the presented method can be readily applied alongside experimental underwater detonation tests.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27354274','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27354274"><span>Cross-sectional analysis of deprivation and <span class="hlt">ideal</span> cardiovascular health in the Paris Prospective Study 3.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Empana, J P; Perier, M C; Singh-Manoux, A; Gaye, B; Thomas, F; Prugger, C; Plichart, M; Wiernik, E; Guibout, C; Lemogne, C; Pannier, B; Boutouyrie, P; Jouven, X</p> <p>2016-12-01</p> <p>We hypothesised that deprivation might represent a barrier to attain an <span class="hlt">ideal</span> cardiovascular health (CVH) as defined by the American Heart Association (AHA). The baseline data of 8916 participants of the Paris Prospective Study 3, an observational cohort on novel markers for future cardiovascular disease, were used. The AHA 7-item tool includes four health behaviours (smoking, body weight, physical activity and optimal diet) and three biological measures (blood cholesterol, blood glucose and blood <span class="hlt">pressure</span>). A validated 11-item score of individual material and psychosocial deprivation, the Evaluation de la Précarité et des Inégalités dans les Centres d'Examens de Santé-Evaluation of Deprivation and Inequalities in Health Examination centres (EPICES) score was used. The mean age was 59.5 years (standard deviation 6.2), 61.2% were men and 9.98% had an <span class="hlt">ideal</span> CVH. In sex-specific multivariable polytomous logistic regression, the odds ratio (OR) for <span class="hlt">ideal</span> behavioural CVH progressively decreased with quartile of increasing deprivation, from 0.54 (95% CI 0.41 to 0.72) to 0.49 (0.37 to 0.65) in women and from 0.61 (0.50 to 0.76) to 0.57 (0.46 to 0.71) in men. Associations with <span class="hlt">ideal</span> biological CVH were confined to the most deprived women (OR=0.60; 95% CI 0.37 to 0.99), whereas in men, greater deprivation was related to higher OR of intermediate biological CVH (OR=1.28; 95% CI 1.05 to 1.57 for the third quartile vs the first quartile). Higher material and psychosocial deprivation may represent a barrier to reach an <span class="hlt">ideal</span> CVH. NCT00741728. Published by the BMJ Publishing Group Limited. For permission to use (where not already granted under a licence) please go to http://www.bmj.com/company/products-services/rights-and-licensing/.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16131552','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16131552"><span>Medical learning curves and the Kantian <span class="hlt">ideal</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Le Morvan, P; Stock, B</p> <p>2005-09-01</p> <p>A hitherto unexamined problem for the "Kantian <span class="hlt">ideal</span>" that one should always treat patients as ends in themselves, and never only as a means to other ends, is explored in this paper. The problem consists of a prima facie conflict between this Kantian <span class="hlt">ideal</span> and the reality of medical practice. This conflict arises because, at least presently, medical practitioners can only acquire certain skills and abilities by practising on live, human patients, and given the inevitability and ubiquity of learning curves, this learning requires some patients to be treated only as a means to this end. A number of ways of attempting to establish the compatibility of the Kantian <span class="hlt">Ideal</span> with the reality of medical practice are considered. Each attempt is found to be unsuccessful. Accordingly, until a way is found to reconcile them, we conclude that the Kantian <span class="hlt">ideal</span> is inconsistent with the reality of medical practice.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1734219','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1734219"><span>Medical learning curves and the Kantian <span class="hlt">ideal</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Le Morvan, P; Stock, B</p> <p>2005-01-01</p> <p>A hitherto unexamined problem for the "Kantian <span class="hlt">ideal</span>" that one should always treat patients as ends in themselves, and never only as a means to other ends, is explored in this paper. The problem consists of a prima facie conflict between this Kantian <span class="hlt">ideal</span> and the reality of medical practice. This conflict arises because, at least presently, medical practitioners can only acquire certain skills and abilities by practising on live, human patients, and given the inevitability and ubiquity of learning curves, this learning requires some patients to be treated only as a means to this end. A number of ways of attempting to establish the compatibility of the Kantian <span class="hlt">Ideal</span> with the reality of medical practice are considered. Each attempt is found to be unsuccessful. Accordingly, until a way is found to reconcile them, we conclude that the Kantian <span class="hlt">ideal</span> is inconsistent with the reality of medical practice. PMID:16131552</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA500051','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA500051"><span>Estimation of Time Dependent Properties from Surface <span class="hlt">Pressure</span> in Open Cavities</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2008-02-01</p> <p>static <span class="hlt">pressure</span> of the cavity. The stagnation and static <span class="hlt">pressures</span> are measured separately with Druck Model DPI 145 <span class="hlt">pressure</span> transducers (with a quoted...interacting with the ZNMF actuator jets, the 2D shape of the vortical structures transform to a 3D shape with spanwise vortical structures. These...Therefore, the <span class="hlt">pressure</span> <span class="hlt">gradient</span> in the d direction is dd ° 3d Substituting Equation (5.3) into Equation (5.5) results in ^l = PJk(e^-Re^)/c^ (5.6</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_25 --> <div class="footer-extlink text-muted" style="margin-bottom:1rem; text-align:center;">Some links on this page may take you to non-federal websites. Their policies may differ from this site.</div> </div><!-- container --> <footer><a id="backToTop" href="#top"> </a><nav><a id="backToTop" href="#top"> </a><ul class="links"><a id="backToTop" href="#top"> </a><li><a id="backToTop" href="#top"></a><a href="/sitemap.html">Site Map</a></li> <li><a href="/members/index.html">Members Only</a></li> <li><a href="/website-policies.html">Website Policies</a></li> <li><a href="https://doe.responsibledisclosure.com/hc/en-us" target="_blank">Vulnerability Disclosure Program</a></li> <li><a href="/contact.html">Contact Us</a></li> </ul> <div class="small">Science.gov is maintained by the U.S. Department of Energy's <a href="https://www.osti.gov/" target="_blank">Office of Scientific and Technical Information</a>, in partnership with <a href="https://www.cendi.gov/" target="_blank">CENDI</a>.</div> </nav> </footer> <script type="text/javascript"><!-- // var lastDiv = ""; function showDiv(divName) { // hide last div if (lastDiv) { document.getElementById(lastDiv).className = "hiddenDiv"; } //if value of the box is not nothing and an object with that name exists, then change the class if (divName && document.getElementById(divName)) { document.getElementById(divName).className = "visibleDiv"; lastDiv = divName; } } //--> </script> <script> /** * Function that tracks a click on an outbound link in Google Analytics. * This function takes a valid URL string as an argument, and uses that URL string * as the event label. */ var trackOutboundLink = function(url,collectionCode) { try { h = window.open(url); setTimeout(function() { ga('send', 'event', 'topic-page-click-through', collectionCode, url); }, 1000); } catch(err){} }; </script> <!-- Google Analytics --> <script> (function(i,s,o,g,r,a,m){i['GoogleAnalyticsObject']=r;i[r]=i[r]||function(){ (i[r].q=i[r].q||[]).push(arguments)},i[r].l=1*new Date();a=s.createElement(o), m=s.getElementsByTagName(o)[0];a.async=1;a.src=g;m.parentNode.insertBefore(a,m) })(window,document,'script','//www.google-analytics.com/analytics.js','ga'); ga('create', 'UA-1122789-34', 'auto'); ga('send', 'pageview'); </script> <!-- End Google Analytics --> <script> showDiv('page_1') </script> </body> </html>