Sample records for observed pressure dependence

  1. Observations of height-dependent pressure-perturbation structure of a strong mesoscale gravity wave

    NASA Technical Reports Server (NTRS)

    Starr, David O'C.; Korb, C. L.; Schwemmer, Geary K.; Weng, Chi Y.

    1992-01-01

    Airborne observations using a downward-looking, dual-frequency, near-infrared, differential absorption lidar system provide the first measurements of the height-dependent pressure-perturbation field associated with a strong mesoscale gravity wave. A pressure-perturbation amplitude of 3.5 mb was measured within the lowest 1.6 km of the atmosphere over a 52-km flight line. Corresponding vertical displacements of 250-500 m were inferred from lidar-observed displacement of aerosol layers. Accounting for probable wave orientation, a horizontal wavelength of about 40 km was estimated. Satellite observations reveal wave structure of a comparable scale in concurrent cirrus cloud fields over an extended area. Smaller-scale waves were also observed. Local meteorological soundings are analyzed to confirm the existence of a suitable wave duct. Potential wave-generation mechanisms are examined and discussed. The large pressure-perturbation wave is attributed to rapid amplification or possible wave breaking of a gravity wave as it propagated offshore and interacted with a very stable marine boundary layer capped by a strong shear layer.

  2. Pressure Dependence of the Boson Peak of Glassy Glycerol

    DOE PAGES

    Ahart, Muhtar; Aihaiti, Dilare; Hemley, Russell J.; ...

    2017-05-31

    The pressure dependence of the Boson peak (BP) of glycerol, including its behavior across the liquid-glass transition, has been studied under pressure using Raman scattering. A significant increase of the BP frequency was observed with pressure up to 11 GPa at room temperature. The pressure dependence of BP frequency ν BP is proportional to (1+P/P 0) 1/3, where P and P 0 are the pressure and a constant, respectively, the spectra are consistent with a soft potential model. The characteristic length of medium range order is close in size to a cyclic trimer of glycerol molecules, which is predicted asmore » the medium range order of a BP vibration using molecular dynamics simulations. The pressure dependence of a characteristic length of medium range order is nearly constant. The pressure induced structural changes in glycerol can be understood in terms of the shrinkage of voids with cyclic trimers remaining up to at least 11 GPa. Lastly, the pressure dependence of intermolecular O-H stretching mode indicates that the intermolecular hydrogen bond distance gradually decreases below the glass transition pressure of ~5 GPa, while it becomes nearly constant in the glassy state indicating the disappearance of the free volume in the dense glass.« less

  3. Pressure dependence of coherence-incoherence crossover behavior in KFe2As2 observed by resistivity and 75As-NMR/NQR

    NASA Astrophysics Data System (ADS)

    Wiecki, P.; Taufour, V.; Chung, D. Y.; Kanatzidis, M. G.; Bud'ko, S. L.; Canfield, P. C.; Furukawa, Y.

    2018-02-01

    We present the results of 75As nuclear magnetic resonance (NMR), nuclear quadrupole resonance (NQR), and resistivity measurements in KFe2As2 under pressure (p ). The temperature dependence of the NMR shift, nuclear spin-lattice relaxation time (T1), and resistivity show a crossover between a high-temperature incoherent, local-moment behavior and a low-temperature coherent behavior at a crossover temperature (T*). T* is found to increase monotonically with pressure, consistent with increasing hybridization between localized 3 d orbital-derived bands with the itinerant electron bands. No anomaly in T* is seen at the critical pressure pc=1.8 GPa where a change of slope of the superconducting (SC) transition temperature Tc(p ) has been observed. In contrast, Tc(p ) seems to correlate with antiferromagnetic spin fluctuations in the normal state as measured by the NQR 1 /T1 data, although such a correlation cannot be seen in the replacement effects of A in the A Fe2As2 (A =K , Rb, Cs) family. In the superconducting state, two T1 components are observed at low temperatures, suggesting the existence of two distinct local electronic environments. The temperature dependence of the short T1 s indicates a nearly gapless state below Tc. On the other hand, the temperature dependence of the long component 1 /T1 L implies a large reduction in the density of states at the Fermi level due to the SC gap formation. These results suggest a real-space modulation of the local SC gap structure in KFe2As2 under pressure.

  4. Pressure Dependence of Coherence-Incoherence Crossover Behavior in KFe 2As 2 Observed by Resistivity and 75As-NMR/NQR.

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

    Wiecki, P.; Taufour, V.; Chung, D. Y.

    We present the results of 75As nuclear magnetic resonance (NMR), nuclear quadrupole resonance (NQR), and resistivity measurements in KFe 2As 2 under pressure (p). The temperature dependence of the NMR shift, nuclear spin-lattice relaxation time (T1), and resistivity show a crossover between a high-temperature incoherent, local-moment behavior and a low-temperature coherent behavior at a crossover temperature (T *). T * is found to increase monotonically with pressure, consistent with increasing hybridization between localized 3d orbitalderived bands with the itinerant electron bands. No anomaly in T * is seen at the critical pressure pc = 1.8 GPa where a change ofmore » slope of the superconducting (SC) transition temperature Tc(p) has been observed. In contrast, Tc(p) seems to correlate with antiferromagnetic spin fluctuations in the normal state as measured by the NQR 1/T1 data, although such a correlation cannot be seen in the replacement effects of A in the KFe 2As 2 (A = K, Rb, Cs) family. In the superconducting state, two T1 components are observed at low temperatures, suggesting the existence of two distinct local electronic environments. The temperature dependence of the short T1s indicates a nearly gapless state below Tc. On the other hand, the temperature dependence of the long component 1/T1L implies a large reduction in the density of states at the Fermi level due to the SC gap formation. These results suggest a real-space modulation of the local SC gap structure in KFe 2As 2 under pressure.« less

  5. Pressure dependence of coherence-incoherence crossover behavior in KFe 2 As 2 observed by resistivity and As 75 -NMR/NQR

    DOE PAGES

    Wiecki, P.; Taufour, V.; Chung, D. Y.; ...

    2018-02-13

    We present the results of 75As nuclear magnetic resonance (NMR), nuclear quadrupole resonance (NQR), and resistivity measurements in KF e2 As 2 under pressure (p). The temperature dependence of the NMR shift, nuclear spin-lattice relaxation time (T 1), and resistivity show a crossover between a high-temperature incoherent, local-moment behavior and a low-temperature coherent behavior at a crossover temperature (T*). T* is found to increase monotonically with pressure, consistent with increasing hybridization between localized 3d orbital-derived bands with the itinerant electron bands. No anomaly in T* is seen at the critical pressure p c= 1.8 GPa where a change of slopemore » of the superconducting (SC) transition temperature T c( p ) has been observed. In contrast, T c( p ) seems to correlate with antiferromagnetic spin fluctuations in the normal state as measured by the NQR 1/T 1 data, although such a correlation cannot be seen in the replacement effects of A in the AFe 2As 2 (A=K,Rb,Cs) family. In the superconducting state, two T 1 components are observed at low temperatures, suggesting the existence of two distinct local electronic environments. The temperature dependence of the short T 1s indicates a nearly gapless state below T c. On the other hand, the temperature dependence of the long component 1/T 1Limplies a large reduction in the density of states at the Fermi level due to the SC gap formation. These results suggest a real-space modulation of the local SC gap structure in KFe 2As 2 under pressure.« less

  6. Pressure dependence of coherence-incoherence crossover behavior in KFe 2 As 2 observed by resistivity and As 75 -NMR/NQR

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

    Wiecki, P.; Taufour, V.; Chung, D. Y.

    We present the results of 75As nuclear magnetic resonance (NMR), nuclear quadrupole resonance (NQR), and resistivity measurements in KF e2 As 2 under pressure (p). The temperature dependence of the NMR shift, nuclear spin-lattice relaxation time (T 1), and resistivity show a crossover between a high-temperature incoherent, local-moment behavior and a low-temperature coherent behavior at a crossover temperature (T*). T* is found to increase monotonically with pressure, consistent with increasing hybridization between localized 3d orbital-derived bands with the itinerant electron bands. No anomaly in T* is seen at the critical pressure p c= 1.8 GPa where a change of slopemore » of the superconducting (SC) transition temperature T c( p ) has been observed. In contrast, T c( p ) seems to correlate with antiferromagnetic spin fluctuations in the normal state as measured by the NQR 1/T 1 data, although such a correlation cannot be seen in the replacement effects of A in the AFe 2As 2 (A=K,Rb,Cs) family. In the superconducting state, two T 1 components are observed at low temperatures, suggesting the existence of two distinct local electronic environments. The temperature dependence of the short T 1s indicates a nearly gapless state below T c. On the other hand, the temperature dependence of the long component 1/T 1Limplies a large reduction in the density of states at the Fermi level due to the SC gap formation. These results suggest a real-space modulation of the local SC gap structure in KFe 2As 2 under pressure.« less

  7. Observation of Ortho-Para Dependence of Pressure Broadening Coefficient in Acetylene νb{1}+νb{3} Vibration Band Using Dual-Comb Spectroscopy

    NASA Astrophysics Data System (ADS)

    Iwakuni, Kana; Okubo, Sho; Inaba, Hajime; Onae, Atsushi; Hong, Feng-Lei; Sasada, Hiroyuki; Yamada, Koichi MT

    2016-06-01

    We observe that the pressure-broadening coefficients depend on the ortho-para levels. The spectrum is taken with a dual-comb spectrometer which has the resolution of 48 MHz and the frequency accuracy of 8 digit when the signal-to-noise ratio is more than 20. In this study, about 4.4-Tz wide spectra of the P(31) to R(31) transitions in the νb{1}+νb{3} vibration band of 12C_2H_2 are observed at the pressure of 25, 60, 396, 1047, 1962 and 2654 Pa. Each rotation-vibration absorption line is fitted to Voight function and we determined pressure-broadening coefficients for each rotation-vibration transition. The Figure shows pressure broadening coefficient as a function of m. Here m is J"+1 for R and -J" for P-branch. The graph shows obvious dependence on ortho and para. We fit it to Pade function considering the population ratio of three-to-one for the ortho and para levels. This would lead to detailed understanding of the pressure boarding mechanism. S. Okubo et al., Applied Physics Express 8, 082402 (2015)

  8. Ram Pressure Stripping: Observations Meet Simulations

    NASA Astrophysics Data System (ADS)

    Past, Matthew; Ruszkowski, Mateusz; Sharon, Keren

    2017-01-01

    Ram pressure stripping occurs when a galaxy falls into the potential well of a cluster, removing gas and dust as the galaxy travels through the intracluster medium. This interaction leads to filamentary gas tails stretching behind the galaxy and plays an important role in galaxy evolution. Previously, these “jellyfish” galaxies had only been observed in nearby clusters, but recently, higher redshift (z > 0.3) examples have been found from HST data imaging.Recent work has shown that cosmic rays injected by supernovae can cause galactic disks to thicken due to cosmic ray pressure. We run three-dimensional magneto-hydrodynamical simulations of ram pressure stripping including cosmic rays to compare to previous models. We study how the efficiency of the ram pressure stripping of the gas, and the morphology of the filamentary tails, depend on the magnitude of the cosmic ray pressure support. We generate mock X-ray images and radio polarization data. Simultaneously, we perform an exhaustive search of the HST archive to increase the sample of jellyfish galaxies and compare selected cases to simulations.

  9. Energy and mass dependence of the contribution to storm-time plasma pressure observed by Arase/MEP-i

    NASA Astrophysics Data System (ADS)

    Kasahara, S.; Keika, K.; Yokota, S.; Hoshino, M.; Seki, K.; Nose, M.; Amano, T.; Yoshizumi, M.; Shinohara, I.

    2017-12-01

    The ring current is mainly controlled by the ion pressure and its spatial gradient. The ion pressure is dominated by ions with energies of a few to a few 100s keV. Oxygen ions of ionospheric origin can be energized in the plasma sheet and/or the inner magnetosphere up to a few tens to a few hundreds of keV. The ionospheric oxygen ions make a significant contribution to the ion pressure during geomagnetically active periods. This paper examines spatial variations and energy-spectral evolution of energetic ( 10 to 200 keV/q) ions during the main phase of a CIR-driven storm on 17 March 2017 (Storm 1) and a CME-driven storm on 27-28 May 2017 (Storm 2). We use ion data from the MEP-i instrument on board the Arase satellite. The instrument measured energetic ions with energies of 5-120 keV/q during Storm 1 and 9-180 keV/q during Storm 2; ion mass/charge was derived from energy and velocity measurements by an electrostatic analyzer and the time-of-flight system, respectively. Below is a brief summary of the MEP-i observations during the two storms. During Storm 1, MEP-i saw high fluxes of >10 keV/q protons and oxygen ions (and possibly other minor ions) at Lm 3.5 around midnight. MEP-i continued to observe high-flux ions until the end of the main phase. Both proton and oxygen ion pressures increased; the O-to-H ratio increased by about an order of magnitude, from 0.02 to 0.2-0.3. The high-flux >10 keV/q ions consisted of clearly different two populations: one dominated by 5-20 keV/q ions, likely originating from pre-existing cold plasma sheet population; and the other with structured dispersion signatures at 30-90 keV/q, likely due to the penetration of ions accelerated in the near-Earth plasma sheet. We found that both populations contributed to the total pressure almost equally. During Storm 2, MEP-i observed proton and oxygen high fluxes in a wide energy range (10-120 keV/q). The pressure increased for both protons and oxygen ions; the O-to-H ratio increased from 0

  10. Intensity and pressure dependence of resonance fluorescence of OH induced by a tunable UV laser

    NASA Technical Reports Server (NTRS)

    Killinger, D. K.; Wang, C. C.; Hanabusa, M.

    1976-01-01

    The intensity and pressure dependence of the fluorescence spectrum of OH in the presence of N2 and H2O molecules was studied. Saturation of the absorption transition was observed at low pressures, and the corresponding fluorescence signal was found to vary as the square root of the exciting intensity. This observed dependence agreed with the predicted dependence which took into account the presence of laser modes in the spectrum of the exciting radiation. With full laser power incident, a saturation parameter as high as 3 x 10 to the 5th was observed. The fluorescence spectrum was found to peak at 3145 and at 3090 A, with the relative peak intensities dependent upon gas pressures and upon the particular rotational electronic transition used for excitation. It is concluded that vibrational relaxation of the electronically excited OH due to water vapor in the system plays a dominant role in determining the observed fluorescence spectrum.

  11. Correlates of blood pressure in young insulin-dependent diabetics and their families.

    PubMed

    Tarn, A C; Thomas, J M; Drury, P L

    1990-09-01

    We compared the correlates of blood pressure in 163 young patients with insulin-dependent diabetes and in 232 of their non-diabetic siblings. A single observer recorded blood pressure in all subjects, plus all their available parents, using a standardized technique. Other variables recorded included age, weight, height, presence of diabetes and urinary albumin. The major factors accounting for over 50% of the variance of systolic blood pressure (SBP) in both groups were age, weight, paternal SBP and sex. In addition, in the diabetic group the logarithm of the random urinary albumin concentration was a significant explanatory variable. For diastolic blood pressure (DBP) approximately 16% of the variance was explained by age, weight and maternal DBP. Parental blood pressure was an important determinant of blood pressure in both the diabetic and non-diabetic sibling groups. The similarity of the correlates of blood pressure in the two groups suggests that the determinants of blood pressure in young insulin-dependent diabetic patients and in the general population are similar.

  12. Pressure-dependent boron isotopic fractionation observed by column chromatography

    NASA Astrophysics Data System (ADS)

    Musashi, M.; Oi, T.; Matsuo, M.; Nomura, M.

    2007-12-01

    Boron isotopic fractionation factor ( S ) between boron taken up in strongly basic anion exchange resin and boron in aqueous solution was determined by breakthrough column chromatography at 5 and 17 MPa at 25°C, using 0.1 mmol/L boric acid solution as feed solution. The S values obtained were 1.018 and 1.012, respectively, which were smaller than the value reported by using the same chromatographic method at atmospheric pressure at 25°C with the boron concentration of 10 mmol/L, but were larger than the values at the same condition with much higher concentration of 100 and 501 mmol/L, indicating that borate-polymerization reducing the isotopic fractionation was negligible. However, calculations based on the theory of isotope distribution between two phases estimated that 21% (5MPa) and 47% (17MPa) of boron taken up in the resin phase was in the three-coordinated B(OH)3-form, instead of in the four-coordinated B(OH)4--form, at high pressures even with the very diluted solution. We discussed this discrepancy by introducing (1) hydration or (2) a partial molar volume difference between isotopic molecules. It was inferred that borate ions were partially dehydrated upon transfer from the solution phase to the resin phase at high pressures, which resulted in smaller S values compared with those at the atmospheric pressure. Alternatively, it was likely that the S value decreased with increasing pressure, because the difference of the partial isotopic molar volumes between 10B(OH)3 and 11B(OH)3 was larger than that between 10B(OH)4- and 11B(OH)4-. If either will be the case, the influence of a pressure upon the isotope effect may not be negligible for boron isotopic exchange equilibrium. This knowledge is crucial for the principle of the boron isotopic pH-metry reconstructing a chemical variation at the paleo-deep oceanic environment where the early life may have been evolved.

  13. Temperature dependence of thermal pressure for NaCl

    NASA Astrophysics Data System (ADS)

    Singh, Chandra K.; Pande, Brijesh K.; Pandey, Anjani K.

    2018-05-01

    Engineering applications of the materials can be explored upto the desired limit of accuracy with the better knowledge of its mechanical and thermal properties such as ductility, brittleness and Thermal Pressure. For the resistance to fracture (K) and plastic deformation (G) the ratio K/G is treated as an indication of ductile or brittle character of solids. In the present work we have tested the condition of ductility and brittleness with the calculated values of K/G for the NaCl. It is concluded that the nature of NaCl can be predicted upto high temperature simply with the knowledge of its elastic stiffness constant only. Thermoelastic properties of materials at high temperature is directly related to thermal pressure and volume expansion of the materials. An expression for the temperature dependence of thermal pressure is formulated using basic thermodynamic identities. It is observed that thermal pressure ΔPth calculated for NaCl by using Kushwah formulation is in good agreement with the experimental values also the thermal pressure increases with the increase in temperature.

  14. Common/Dependent-Pressure-Vessel Nickel-Hydrogen Batteries

    NASA Technical Reports Server (NTRS)

    Timmerman, Paul J.

    2003-01-01

    The term "common/dependent pressure vessel" (C/DPV) denotes a proposed alternative configuration for a nickelhydrogen battery. The C/DPV configuration is so named because it is a hybrid of two prior configurations called "common pressure vessel" (CPV) and "dependent pressure vessel" (DPV). The C/DPV configuration has been proposed as a basis for designing highly reliable, long-life Ni/H2-batteries and cells for anticipated special applications in which it is expected that small charge capacities will suffice and sizes and weights must be minimized.

  15. Pressure-driven flow of a Herschel-Bulkley fluid with pressure-dependent rheological parameters

    NASA Astrophysics Data System (ADS)

    Panaseti, Pandelitsa; Damianou, Yiolanda; Georgiou, Georgios C.; Housiadas, Kostas D.

    2018-03-01

    The lubrication flow of a Herschel-Bulkley fluid in a symmetric long channel of varying width, 2h(x), is modeled extending the approach proposed by Fusi et al. ["Pressure-driven lubrication flow of a Bingham fluid in a channel: A novel approach," J. Non-Newtonian Fluid Mech. 221, 66-75 (2015)] for a Bingham plastic. Moreover, both the consistency index and the yield stress are assumed to be pressure-dependent. Under the lubrication approximation, the pressure at zero order depends only on x and the semi-width of the unyielded core is found to be given by σ(x) = -(1 + 1/n)h(x) + C, where n is the power-law exponent and the constant C depends on the Bingham number and the consistency-index and yield-stress growth numbers. Hence, in a channel of constant width, the width of the unyielded core is also constant, despite the pressure dependence of the yield stress, and the pressure distribution is not affected by the yield-stress function. With the present model, the pressure is calculated numerically solving an integro-differential equation and then the position of the yield surface and the two velocity components are computed using analytical expressions. Some analytical solutions are also derived for channels of constant and linearly varying widths. The lubrication solutions for other geometries are calculated numerically. The implications of the pressure-dependence of the material parameters and the limitations of the method are discussed.

  16. Structure and dynamics of water confined in a graphene nanochannel under gigapascal high pressure: dependence of friction on pressure and confinement.

    PubMed

    Yang, Lei; Guo, Yanjie; Diao, Dongfeng

    2017-05-31

    Recently, water flow confined in nanochannels has become an interesting topic due to its unique properties and potential applications in nanofluidic devices. The trapped water is predicted to experience high pressure in the gigapascal regime. Theoretical and experimental studies have reported various novel structures of the confined water under high pressure. However, the role of this high pressure on the dynamic properties of water has not been elucidated to date. In the present study, the structure evolution and interfacial friction behavior of water constrained in a graphene nanochannel were investigated via molecular dynamics simulations. Transitions of the confined water to different ice phases at room temperature were observed in the presence of lateral pressure at the gigapascal level. The friction coefficient at the water/graphene interface was found to be dependent on the lateral pressure and nanochannel height. Further theoretical analyses indicate that the pressure dependence of friction is related to the pressure-induced change in the structure of water and the confinement dependence results from the variation in the water/graphene interaction energy barrier. These findings provide a basic understanding of the dynamics of the nanoconfined water, which is crucial in both fundamental and applied science.

  17. Identification of yellow luminescence centers in Be-doped GaN through pressure-dependent studies

    NASA Astrophysics Data System (ADS)

    Teisseyre, Henryk; Lyons, John L.; Kaminska, Agata; Jankowski, Dawid; Jarosz, Dawid; Boćkowski, Michał; Suchocki, Andrzej; Van de Walle, Chris G.

    2017-06-01

    Effective acceptor doping of wide-band-gap semiconductors is still an outstanding problem. Beryllium has been suggested as a shallow acceptor in GaN, but despite sporadic announcements, Be-induced p-type doping has never been practically realized. Be-doped GaN possesses two luminescence bands; one at 3.38 eV and a second near 2.2 eV at an energy close to that of the parasitic yellow luminescence often found in undoped GaN crystals. We have performed high hydrostatic pressure studies of bulk, Be-doped gallium nitride crystals using the diamond anvil cell technique. We observed a splitting of the yellow luminescence line under hydrostatic pressure into two components, one which is strongly dependent on applied pressure and another whose pressure dependence is more modest. Together with hybrid functional calculations, we attribute the strongly-varying component to the beryllium-oxygen complex. The second component of the yellow luminescence possesses very similar pressure behavior to the yellow luminescence observed in undoped samples grown by the same method, behavior which we find consistent with the CN acceptor. At higher pressure, we observe the vanishing of yellow luminescence and a rapid increase in luminescence intensity of the UV line. We explain this as the pressure-induced transformation of the Be-O complex from a highly localized state with large lattice relaxation to a delocalized state with limited lattice relaxation.

  18. Pressure-dependent attenuation with microbubbles at low mechanical index.

    PubMed

    Tang, Meng-Xing; Eckersley, Robert J; Noble, J Alison

    2005-03-01

    It has previously been shown that the attenuation of ultrasound (US) by microbubble contrast agents is dependent on acoustic pressure (Chen et al. 2002). Although previous studies have modelled the pressure-dependence of attenuation in single bubbles, this paper investigates this subject by considering a bulk volume of bubbles together with other linear attenuators. Specifically, a new pressure-dependent attenuation model for an inhomogeneous volume of attenuators is proposed. In this model, the effect of the attenuation on US propagation is considered. The model was validated using experimental measurements on the US contrast agent Sonovue. The results indicate, at low acoustic pressures, a linear relationship between the attenuation of Sonovue, measured in dB, and the insonating acoustic pressure.

  19. Pressure Dependence of the Radial Breathing Mode of Carbon Nanotubes: The Effect of Fluid Adsorption

    NASA Astrophysics Data System (ADS)

    Longhurst, M. J.; Quirke, N.

    2007-04-01

    The pressure dependence of shifts in the vibrational modes of individual carbon nanotubes is strongly affected by the nature of the pressure transmitting medium as a result of adsorption at the nanotube surface. The adsorbate is treated as an elastic shell which couples with the radial breathing mode (RBM) of the nanotube via van der Waal interactions. Using analytical methods as well as molecular simulation, we observe a low frequency breathing mode for the adsorbed fluid at ˜50cm-1, as well as diameter dependent upshifts in the RBM frequency with pressure, suggesting metallic nanotubes may wet more than semiconducting ones.

  20. Pressure dependence of backbone chemical shifts in the model peptides Ac-Gly-Gly-Xxx-Ala-NH2.

    PubMed

    Erlach, Markus Beck; Koehler, Joerg; Crusca, Edson; Kremer, Werner; Munte, Claudia E; Kalbitzer, Hans Robert

    2016-06-01

    For a better understanding of nuclear magnetic resonance (NMR) detected pressure responses of folded as well as unstructured proteins the availability of data from well-defined model systems are indispensable. In this work we report the pressure dependence of chemical shifts of the backbone atoms (1)H(α), (13)C(α) and (13)C' in the protected tetrapeptides Ac-Gly-Gly-Xxx-Ala-NH2 (Xxx one of the 20 canonical amino acids). Contrary to expectation the chemical shifts of these nuclei have a nonlinear dependence on pressure in the range from 0.1 to 200 MPa. The polynomial pressure coefficients B 1 and B 2 are dependent on the type of amino acid studied. The coefficients of a given nucleus show significant linear correlations suggesting that the NMR observable pressure effects in the different amino acids have at least partly the same physical cause. In line with this observation the magnitude of the second order coefficients of nuclei being direct neighbors in the chemical structure are also weakly correlated.

  1. Comparison of the pressure dependences of Tc in the trivalent d -electron superconductors Sc, Y, La, and Lu up to megabar pressures

    NASA Astrophysics Data System (ADS)

    Debessai, M.; Hamlin, J. J.; Schilling, J. S.

    2008-08-01

    Whereas double hcp (dhcp) La superconducts at ambient pressure with Tc≃5K , the other trivalent d -electron metals Sc, Y, and Lu only superconduct if high pressures are applied. Earlier measurements of the pressure dependence of Tc for Sc and Lu metal are here extended to much higher pressures. Whereas Tc for Lu increases monotonically with pressure to 12.4 K at 174 GPa (1.74 Mbar), Tc for Sc reaches 19.6 K at 107 GPa, the second highest value observed for any elemental superconductor. At higher pressures a phase transition occurs whereupon Tc drops to 8.31 K at 111 GPa. The Tc(P) dependences for Sc and Lu are compared with those of Y and La. An interesting correlation is pointed out between the value of Tc and the fractional free volume available to the conduction electrons outside the ion cores, a quantity which is directly related to the number of d electrons in the conduction band.

  2. Effect of thermal pressurization on dynamic rupture propagation under depth-dependent stress

    NASA Astrophysics Data System (ADS)

    Urata, Y.; Kuge, K.; Kase, Y.

    2009-12-01

    Fluid and pore pressure evolution can affect dynamic propagation of earthquake ruptures owing to thermal pressurization (e.g., Mase and Smith, 1985). We investigate dynamic rupture propagation with thermal pressurization on a fault subjected to depth-dependent stress, on the basis of 3-D numerical simulations for spontaneous dynamic ruptures. We put a vertical strike-slip rectangular fault in a semi-infinite, homogenous, and elastic medium. The length and width of the fault are 8 and 3 km, respectively. We assume a depth-dependent stress estimated by Yamashita et al. (2004). The numerical algorithm is based on the finite-difference method by Kase and Kuge (2001). A rupture is initiated by increasing shear stress in a small patch at the bottom of the fault, and then proceeds spontaneously, governed by a slip-weakening law with the Coulomb failure criteria. Coefficients of friction and Dc are homogeneous on the fault. On a fault with thermal pressurization, we allow effective normal stress to vary with pore pressure change due to frictional heating by the formulation of Bizzarri and Cocco (2006). When thermal pressurization does not work, tractions drop in the same way everywhere and rupture velocity is subshear except near the free surface. Due to thermal pressurization, dynamic friction on the fault decreases and is heterogeneous not only vertically but horizontally, slip increases, and rupture velocity along the strike direction becomes supershear. As a result, plural peaks of final slip appear, as observed in the case of undrained dip-slip fault by Urata et al. (2008). We found in this study that the early stage of rupture growth under the depth-dependent stress is affected by the location of an initial crack. When a rupture is initiated at the center of the fault without thermal pressurization, the rupture cannot propagate and terminates. Thermal pressurization can help such a powerless rupture to keep propagating.

  3. Pressure dependence of the radial mode frequency in carbon nanotubes

    NASA Astrophysics Data System (ADS)

    Venkateswaran, Uma; Masica, D.; Sumanasekara, G.; Eklund, P.

    2003-03-01

    Recently, an analytical expression for the radial breathing mode frequency, ω_R, was derived by considering the oscillations of a thin hollow cylinder.[1] Using this result and the experimental pressure-dependence of the elastic and lattice constants of graphite, we show that the pressure derivative of ωR depends inversely on the nanotube diameter, D. Since ωR also depends inversely on D, the above result implies that the logarithmic pressure derivative of ω_R, i.e., dlnω_R/dP should be independent of D. We have performed high-pressure Raman scattering experiments on HiPCO-SWNT bundles using different laser excitations, thereby probing the radial modes from different diameter tubes. These measurements show an increase in dlnω_R/dP with increasing D. This difference between the predictions and experiments suggests that the main contribution to ω_R's pressure dependence in SWNT bundles stems from the tube-tube interactions within the bundle and from pressure-induced distortions to the tube cross-section. [1] G.D. Mahan, Phys. Rev. B 65, 235402 (2002).

  4. EXTRASOLAR STORMS: PRESSURE-DEPENDENT CHANGES IN LIGHT-CURVE PHASE IN BROWN DWARFS FROM SIMULTANEOUS HST AND SPITZER OBSERVATIONS

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

    Yang, Hao; Apai, Dániel; Karalidi, Theodora

    We present Spitzer /Infrared Array Camera Ch1 and Ch2 monitoring of six brown dwarfs during eight different epochs over the course of 20 months. For four brown dwarfs, we also obtained simulataneous Hubble Space Telescope ( HST )/WFC3 G141 grism spectra during two epochs and derived light curves in five narrowband filters. Probing different pressure levels in the atmospheres, the multiwavelength light curves of our six targets all exhibit variations, and the shape of the light curves evolves over the timescale of a rotation period, ranging from 1.4 to 13 hr. We compare the shapes of the light curves andmore » estimate the phase shifts between the light curves observed at different wavelengths by comparing the phase of the primary Fourier components. We use state-of-the-art atmosphere models to determine the flux contribution of different pressure layers to the observed flux in each filter. We find that the light curves that probe higher pressures are similar and in phase, but are offset and often different from the light curves that probe lower pressures. The phase differences between the two groups of light curves suggest that the modulations seen at lower and higher pressures may be introduced by different cloud layers.« less

  5. THE INFLUENCE OF PRESSURE-DEPENDENT VISCOSITY ON THE THERMAL EVOLUTION OF SUPER-EARTHS

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

    Stamenkovic, Vlada; Noack, Lena; Spohn, Tilman

    2012-03-20

    We study the thermal evolution of super-Earths with a one-dimensional (1D) parameterized convection model that has been adopted to account for a strong pressure dependence of the viscosity. A comparison with a 2D spherical convection model shows that the derived parameterization satisfactorily represents the main characteristics of the thermal evolution of massive rocky planets. We find that the pressure dependence of the viscosity strongly influences the thermal evolution of super-Earths-resulting in a highly sluggish convection regime in the lower mantles of those planets. Depending on the effective activation volume and for cooler initial conditions, we observe with growing planetary massmore » even the formation of a conductive lid above the core-mantle boundary (CMB), a so-called CMB-lid. For initially molten planets our results suggest no CMB-lids but instead a hot lower mantle and core as well as sluggish lower mantle convection. This implies that the initial interior temperatures, especially in the lower mantle, become crucial for the thermal evolution-the thermostat effect suggested to regulate the interior temperatures in terrestrial planets does not work for massive planets if the viscosity is strongly pressure dependent. The sluggish convection and the potential formation of the CMB-lid reduce the convective vigor throughout the mantle, thereby affecting convective stresses, lithospheric thicknesses, and heat fluxes. The pressure dependence of the viscosity may therefore also strongly affect the propensity of plate tectonics, volcanic activity, and the generation of a magnetic field of super-Earths.« less

  6. Pressure dependence of the electron-phonon interaction and the normal-state resistivity

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

    Rapp, O.; Sundqvist, B.

    1981-07-01

    Accurate measurements of the electrical resistance as a function of temperature and pressure are reported for Sn, Zr, dhcp La, and V. These measurements cover a temperature region around room temperature and pressures up to 1.3 GPa. From these data, including also our previous measurements for Al and published results for Pb, the pressure dependence of drho/dT (the resistivity-temperature derivative) is obtained. This quantity is found to be a significant factor in the pressure dependence of the electron-phonon interaction parameter lambda. For the nontransition metals the relative pressure dependence of drho/dT is much larger than the compressibility. Therefore the pressuremore » dependence of the superconducting T/sub c/ is quantitatively well accounted for by the resistance data for these metals. For the transition metals the pressure dependence of drho/dT is relatively smaller and T/sub c/(p) calculated from the resistance data is, at the best, only qualitatively correct. These differences are discussed. Estimates for the pressure dependence of the plasma frequency are obtained.« less

  7. The dependence of the sporicidal effects on the power and pressure of RF-generated plasma processes.

    PubMed

    Lassen, Klaus S; Nordby, Bolette; Grün, Reinar

    2005-07-01

    The sporicidal effect of 20 different radio-frequency plasma processes produced by combining five different gas mixtures [O(2), Ar/H(2) (50/50%), Ar/H(2) (5/95%), O(2)/H(2) (50/50%), O(2)/H(2) (95/5%)] with four power/pressure settings were tested. Sporicidal effects of oxygen-containing plasmas were dependent on power at low pressure settings but not at high pressure settings. In the absence of oxygen no power dependency was observed at either high or low pressure settings. Survivor curves obtained with the use of nonoxygen plasmas typically had a tailing tendency. Only a mixture-optimized Ar/H(2) (15/85%) plasma process was not encumbered by tailing, and produced a decimal reduction time (D value) below 2 min for Bacillus stearothermophilus spores. Scanning electron microscopy showed that a CF(4)/O(2) plasma did more damage to the substrate than the 15/85% Ar/H(2) plasma. The present results indicate that UV irradiation inactivation is swift and power and pressure independent. Additionally, it is produced at low energy. However, it is not complete. Inactivation through etching is highly power and pressure dependent; finally, inactivation by photodesorption is moderately power and pressure dependent. A sterilization process relying on this mechanism is very advantageous because it combines a highly sporicidal effect with low substrate damage. Copyright 2005 Wiley Periodicals, Inc.

  8. Measurement of the Energy and High-Pressure Dependence of X-ray-Induced Decomposition of Crystalline Strontium Oxalate

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

    Goldberger, David; Evlyukhin, Egor; Cifligu, Petrika

    We report measurements of the X-ray-induced decomposition of crystalline strontium oxalate (SrC2O4) as a function of energy and high pressure in two separate experiments. SrC2O4 at ambient conditions was irradiated with monochromatic synchrotron X-rays ranging in energy from 15 to 28 keV. A broad resonance of the decomposition yield was observed with a clear maximum when irradiating with ~20 keV X-rays and ambient pressure. Little or no decomposition was observed at 15 keV, which is below the Sr K-shell energy of 16.12 keV, suggesting that excitation of core electrons may play an important role in the destabilization of the C2O42–more » anion. A second experiment was performed to investigate the high-pressure dependence of the X-ray-induced decomposition of strontium oxalate at fixed energy. SrC2O4 was compressed in a diamond anvil cell (DAC) in the pressure range from 0 to 7.6 GPa with 1 GPa increments and irradiated in situ with 20 keV X-rays. A marked pressure dependence of the decomposition yield of SrC2O4 was observed with a decomposition yield maximum at around 1 GPa, suggesting that different crystal structures of the material play an important role in the decomposition process. This may be due in part to a phase transition observed near this pressure.« less

  9. Measurement of the Energy and High-Pressure Dependence of X-ray-Induced Decomposition of Crystalline Strontium Oxalate.

    PubMed

    Goldberger, David; Evlyukhin, Egor; Cifligu, Petrika; Wang, Yonggang; Pravica, Michael

    2017-09-28

    We report measurements of the X-ray-induced decomposition of crystalline strontium oxalate (SrC 2 O 4 ) as a function of energy and high pressure in two separate experiments. SrC 2 O 4 at ambient conditions was irradiated with monochromatic synchrotron X-rays ranging in energy from 15 to 28 keV. A broad resonance of the decomposition yield was observed with a clear maximum when irradiating with ∼20 keV X-rays and ambient pressure. Little or no decomposition was observed at 15 keV, which is below the Sr K-shell energy of 16.12 keV, suggesting that excitation of core electrons may play an important role in the destabilization of the C 2 O 4 2- anion. A second experiment was performed to investigate the high-pressure dependence of the X-ray-induced decomposition of strontium oxalate at fixed energy. SrC 2 O 4 was compressed in a diamond anvil cell (DAC) in the pressure range from 0 to 7.6 GPa with 1 GPa increments and irradiated in situ with 20 keV X-rays. A marked pressure dependence of the decomposition yield of SrC 2 O 4 was observed with a decomposition yield maximum at around 1 GPa, suggesting that different crystal structures of the material play an important role in the decomposition process. This may be due in part to a phase transition observed near this pressure.

  10. Size-dependent pressure-induced amorphization: a thermodynamic panorama.

    PubMed

    Machon, Denis; Mélinon, Patrice

    2015-01-14

    Below a critical particle size, some pressurized compounds (e.g. TiO2, Y2O3, PbTe) undergo a crystal-to-amorphous transformation instead of a polymorphic transition. This effect reflects the greater propensity of nanomaterials for amorphization. In this work, a panorama of thermodynamic interpretations is given: first, a descriptive analysis based on the energy landscape concept gives a general comprehension of the balance between thermodynamics and kinetics to obtain an amorphous state. Then, a formal approach based on Gibbs energy to describe the thermodynamics and phase transitions in nanoparticles gives a basic explanation of size-dependent pressure-induced amorphization. The features of this transformation (amorphization occurs at pressures lower than the polymorphic transition pressure!) and the nanostructuration can be explained in an elaborated model based on the Ginzburg-Landau theory of phase transition and on percolation theory. It is shown that the crossover between polymorphic transition and amorphization is highly dependent on the defect density and interfacial energy, i.e., on the synthesis process. Their behavior at high pressure is a quality control test for the nanoparticles.

  11. Strength and Anisotropy in Tournemire Shale: Temperature, Pressure and Time Dependences

    NASA Astrophysics Data System (ADS)

    Bonnelye, A.; Schubnel, A.; Zhi, G.; David, C.; Dick, P.

    2017-12-01

    Time and temperature dependent rock deformation has both scientific and socio-economic implications for natural hazards, the oil and gas industry and nuclear waste disposal. During the past decades, most studies on brittle creep have focused on igneous rocks and porous sedimentary rocks. To our knowledge, only few studies have been carried out on the brittle creep behavior of shale. We conducted a series of creep experiments on shale specimens coming from the French Institute for Nuclear Safety (IRSN) underground research laboratory located in Tournemire, France, under two different temperatures (26°C, 75°C) and confining pressures (10 MPa, 80 MPa), for three orientations (σ1along, perpendicular and 45° to bedding). In these long-term experiments (approximately 10 days), stress and strains were recorded continuously, while ultrasonic acoustic velocities were recorded every 1 15 minutes. The brittle creep failure stress of our Tournemire shale samples was systematically observed 50% higher than its short-term peak strength, with larger final axial strain accumulated. During creep, ultrasonic wave velocities first decreased, and then increased gradually. The magnitude of elastic wave velocity variations showed an important orientation and temperature dependence: velocities measured perpendicular to bedding showed increased variation, variation that was enhanced at higher temperature and higher pressure. The case of complete elastic anisotropy reversal was observed for sample deformed perpendicular to bedding, with amount of axial strain needed to reach anisotropy reversal reduced at higher temperature. SEM observations highlight the competition between crack growth, sealing/healing, and possibly mineral rotation, pressure solution or anisotropic compaction during creep defromation. Our study highlights that the short-term peak strength has little meaning in shale material, which can over-consolidate importantly by `plastic' flow. In addition, we show that elastic

  12. The temperature dependence of the pressure switching of Jahn Teller deformation in the deuterated ammonium copper Tutton salt

    NASA Astrophysics Data System (ADS)

    Augustyniak, Maria A.; Krupski, Marcin

    1999-09-01

    The pressure switch of the Jahn-Teller deformation direction in (ND 4) 2Cu(SO 4) 2·6D 2O was investigated in the temperature range 130-320 K. Below 295 K, the new, pressure-induced phase, is stable under ambient pressure. Switching back is observed on heating to above 297 K. In the range 150-295 K a strong temperature dependence of the switching pressure (from 24 to 450 MPa) is observed. Below 150 K, the switching process is slow and a coexistence of two phases is observed. We conclude that the switch of the Cu(D 2O) 6 complex deformation direction is the Jahn-Teller response to the changes in the hydrogen bond system.

  13. Dependence of magnetic anisotropy on MgO sputtering pressure in Co20Fe60B20/MgO stacks

    NASA Astrophysics Data System (ADS)

    Kaidatzis, A.; Serletis, C.; Niarchos, D.

    2017-10-01

    We investigated the dependence of magnetic anisotropy of Ta/Co20Fe60B20/MgO stacks on the Ar partial pressure during MgO deposition, in the range between 0.5 and 15 mTorr. The stacks are studied before and after annealing at 300°C and it is shown that magnetic anisotropy significantly depends on Ar partial pressure. High pressure results in stacks with very low perpendicular magnetic anisotropy even after annealing, while low pressure results in stacks with perpendicular anisotropy even at the as-deposited state. A monotonic increase of magnetic anisotropy energy is observed as Ar partial pressure is decreased.

  14. Time-dependent response of filamentary composite spherical pressure vessels

    NASA Technical Reports Server (NTRS)

    Dozier, J. D.

    1983-01-01

    A filamentary composite spherical pressure vessel is modeled as a pseudoisotropic (or transversely isotropic) composite shell, with the effects of the liner and fill tubes omitted. Equations of elasticity, macromechanical and micromechanical formulations, and laminate properties are derived for the application of an internally pressured spherical composite vessel. Viscoelastic properties for the composite matrix are used to characterize time-dependent behavior. Using the maximum strain theory of failure, burst pressure and critical strain equations are formulated, solved in the Laplace domain with an associated elastic solution, and inverted back into the time domain using the method of collocation. Viscoelastic properties of HBFR-55 resin are experimentally determined and a Kevlar/HBFR-55 system is evaluated with a FORTRAN program. The computed reduction in burst pressure with respect to time indicates that the analysis employed may be used to predict the time-dependent response of a filamentary composite spherical pressure vessel.

  15. Pressure dependence of the photocycle kinetics of bacteriorhodopsin.

    PubMed Central

    Klink, B U; Winter, R; Engelhard, M; Chizhov, I

    2002-01-01

    The pressure dependence of the photocycle kinetics of bacteriorhodopsin from Halobacterium salinarium was investigated at pressures up to 4 kbar at 25 degrees C and 40 degrees C. The kinetics can be adequately modeled by nine apparent rate constants, which are assigned to irreversible transitions of a single relaxation chain of nine kinetically distinguishable states P(1) to P(9). All states except P(1) and P(9) consist of two or more spectral components. The kinetic states P(2) to P(6) comprise only the two fast equilibrating spectral states L and M. From the pressure dependence, the volume differences DeltaV(o)(LM) between these two spectral states could be determined that range from DeltaV(o)(LM) = -11.4 +/- 0.7 ml/mol (P(2)) to DeltaV(o)(LM) = 14.6 +/- 2.8 mL/mol (P(6)). A model is developed that explains the dependence of DeltaV(o)(LM) on the kinetic state by the electrostriction effect of charges, which are formed and neutralized during the L/M transition. PMID:12496115

  16. Observation of number-density-dependent growth of plasmonic nanobubbles

    NASA Astrophysics Data System (ADS)

    Nakajima, Takashi; Wang, Xiaolong; Chatterjee, Souvik; Sakka, Tetsuo

    2016-06-01

    Interaction dynamics of laser pulses and nanoparticles are of great interest in recent years. In many cases, laser-nanoparticle interactions result in the formation of plasmonic nanobubbles, and the dynamics of nanoparticles and nanobubbles are inseparable. So far, very little attention has been paid to the number density. Here we report the first observation of number-density-dependent growth of plasmonic nanobubbles. Our results show that the nanobubbles growth depends (does not depend) on the number density at high (low) laser fluence, although the inter-particle distance in the solution is as long as 14-30 μm. This cannot be explained by the existing physical picture, and we propose a new model which takes into account the pressure waves arising from nanoparticles. The numerical results based on this model agree well with the experimental results. Our findings imply that the number density can be a new doorknob to control laser-nanobubble as well as laser-nanoparticle interactions.

  17. Observation of number-density-dependent growth of plasmonic nanobubbles.

    PubMed

    Nakajima, Takashi; Wang, Xiaolong; Chatterjee, Souvik; Sakka, Tetsuo

    2016-06-29

    Interaction dynamics of laser pulses and nanoparticles are of great interest in recent years. In many cases, laser-nanoparticle interactions result in the formation of plasmonic nanobubbles, and the dynamics of nanoparticles and nanobubbles are inseparable. So far, very little attention has been paid to the number density. Here we report the first observation of number-density-dependent growth of plasmonic nanobubbles. Our results show that the nanobubbles growth depends (does not depend) on the number density at high (low) laser fluence, although the inter-particle distance in the solution is as long as 14-30 μm. This cannot be explained by the existing physical picture, and we propose a new model which takes into account the pressure waves arising from nanoparticles. The numerical results based on this model agree well with the experimental results. Our findings imply that the number density can be a new doorknob to control laser-nanobubble as well as laser-nanoparticle interactions.

  18. Time-dependent observables in heavy ion collisions. Part II. In search of pressure isotropization in the φ 4 theory

    NASA Astrophysics Data System (ADS)

    Kovchegov, Yuri V.; Wu, Bin

    2018-03-01

    To understand the dynamics of thermalization in heavy ion collisions in the perturbative framework it is essential to first find corrections to the free-streaming classical gluon fields of the McLerran-Venugopalan model. The corrections that lead to deviations from free streaming (and that dominate at late proper time) would provide evidence for the onset of isotropization (and, possibly, thermalization) of the produced medium. To find such corrections we calculate the late-time two-point Green function and the energy-momentum tensor due to a single 2 → 2 scattering process involving two classical fields. To make the calculation tractable we employ the scalar φ 4 theory instead of QCD. We compare our exact diagrammatic results for these quantities to those in kinetic theory and find disagreement between the two. The disagreement is in the dependence on the proper time τ and, for the case of the two-point function, is also in the dependence on the space-time rapidity η: the exact diagrammatic calculation is, in fact, consistent with the free streaming scenario. Kinetic theory predicts a build-up of longitudinal pressure, which, however, is not observed in the exact calculation. We conclude that we find no evidence for the beginning of the transition from the free-streaming classical fields to the kinetic theory description of the produced matter after a single 2 → 2 rescattering.

  19. Pressure Dependence of Magnesite Flow Strength

    NASA Astrophysics Data System (ADS)

    Millard, J. W.; Holyoke, C. W., III; McDaniel, C.; Raterron, P.; Kronenberg, A. K.; Tokle, L.

    2017-12-01

    Recent experiments by Holyoke et al. (2014) indicate that magnesite is weak compared with olivine, leading to strain localization into magnesite-bearing horizons of downgoing subducting slabs, potentially leading to intermediate (200-400 km) deep focus earthquakes DFEs. Flow strengths (σ) of magnesite were determined as functions of strain rate and temperature (T), but not of pressure (P). In order to determine the pressure dependence of magnesite deforming by dislocation creep and low temperature plasticity (LTP), we performed triaxial deformation experiments on natural, coarse-grained (80 μm) magnesite aggregates at T = 900oC, strain rate of 2*10-5/s and P from 3.2 to 7.9 GPa in the D-DIA at Beamline 6-BMB at the Advanced Photon Source at Argonne National Lab. Strengths of magnesite aggregates increase as a function of pressure, from σ=0.85 GPa (at P = 3.2 GPa) to 1.69 GPa (at P = 7.9 GPa). Microstructures developed at P ≤ 6.2 GPa include grain flattening and sweeping undulatory extinction, and dynamic recrystallization at grain boundaries (by bulge nucleation), consistent with dislocation creep. Microstructures generated at P ≥ 6.7 GPa include some twins and kink bands, grain flattening and patchy undulatory extinction, and bulging recrystallization at grain boundaries. These microstructures indicate contributions to strain of both LTP and dislocation creep mechanisms. The pressure dependence can be described by a thermally activated enthalpy, where s increases with P by way of an activation volume V*. Based on both D-DIA and Griggs apparatus results (of Holyoke et al., 2014), V* = 8.5 (± 0.5) × 10-6 m3 mol-1. This value is comparable to V* determined for creep of olivine (9.5 (± 7) × 10-6 m3 mol-1 Durham et al., 2009), indicating that the strength difference between magnesite and olivine will continue to be significant at high pressures, and lead to strain localization at all subduction zone depths.

  20. Pressure dependence of side chain 13C chemical shifts in model peptides Ac-Gly-Gly-Xxx-Ala-NH2.

    PubMed

    Beck Erlach, Markus; Koehler, Joerg; Crusca, Edson; Munte, Claudia E; Kainosho, Masatsune; Kremer, Werner; Kalbitzer, Hans Robert

    2017-10-01

    For evaluating the pressure responses of folded as well as intrinsically unfolded proteins detectable by NMR spectroscopy the availability of data from well-defined model systems is indispensable. In this work we report the pressure dependence of 13 C chemical shifts of the side chain atoms in the protected tetrapeptides Ac-Gly-Gly-Xxx-Ala-NH 2 (Xxx, one of the 20 canonical amino acids). Contrary to expectation the chemical shifts of a number of nuclei have a nonlinear dependence on pressure in the range from 0.1 to 200 MPa. The size of the polynomial pressure coefficients B 1 and B 2 is dependent on the type of atom and amino acid studied. For H N , N and C α the first order pressure coefficient B 1 is also correlated to the chemical shift at atmospheric pressure. The first and second order pressure coefficients of a given type of carbon atom show significant linear correlations suggesting that the NMR observable pressure effects in the different amino acids have at least partly the same physical cause. In line with this observation the magnitude of the second order coefficients of nuclei being direct neighbors in the chemical structure also are weakly correlated. The downfield shifts of the methyl resonances suggest that gauche conformers of the side chains are not preferred with pressure. The valine and leucine methyl groups in the model peptides were assigned using stereospecifically 13 C enriched amino acids with the pro-R carbons downfield shifted relative to the pro-S carbons.

  1. Observations of Fabric Development in Polycrystalline Ice at Basal Pressures: Methods and Initial Results

    NASA Astrophysics Data System (ADS)

    Breton, D. J.; Baker, I.; Cole, D. M.

    2012-12-01

    Understanding and predicting the flow of polycrystalline ice is crucial to ice sheet modeling and paleoclimate reconstruction from ice cores. Ice flow rates depend strongly on the fabric (i.e. the distribution of grain sizes and crystallographic orientations) which evolves over time and enhances the flow rate in the direction of applied stress. The mechanisms for fabric evolution in ice have been extensively studied at atmospheric pressures, but little work has been done to observe these processes at the high pressures experienced deep within ice sheets where long-term changes in ice rheology are expected to have significance. We conducted compressive creep tests on a 917 kg m-3 polycrystalline ice specimen at 20 MPa hydrostatic pressure, thus simulating ~2,000 m depth. Initial specimen grain orientations were random, typical grain diameters were 1.2 mm, and the applied creep stress was 0.3 MPa. Subsequent microstructural analyses on the deformed specimen and a similarly prepared, undeformed specimen allowed characterization of crystal fabric evolution under pressure. Our microstructural analysis technique simultaneously collected grain shape and size data from Scanning Electron Microscope (SEM) micrographs and obtained crystallographic orientation data via Electron BackScatter Diffraction (EBSD). Combining these measurements allows rapid analysis of the ice fabric over large numbers of grains, yielding statistically useful numbers of grain size and full c- and a-axis grain orientation data. The combined creep and microstructural data demonstrate pressure-dependent effects on the mechanical and microstructural evolution of polycrystalline ice. We discuss possible mechanisms for the observed phenomena, and future directions for hydrostatic creep testing.

  2. Feasibility of controlling speed-dependent low-frequency brake vibration amplification by modulating actuation pressure

    NASA Astrophysics Data System (ADS)

    Sen, Osman Taha; Dreyer, Jason T.; Singh, Rajendra

    2014-12-01

    In this article, a feasibility study of controlling the low frequency torque response of a disc brake system with modulated actuation pressure (in the open loop mode) is conducted. First, a quasi-linear model of the torsional system is introduced, and analytical solutions are proposed to incorporate the modulation effect. Tractable expressions for three different modulation schemes are obtained, and conditions that would lead to a reduction in the oscillatory amplitudes are identified. Second, these conditions are evaluated with a numerical model of the torsional system with clearance nonlinearity, and analytical solutions are verified in terms of the trends observed. Finally, a laboratory experiment with a solenoid valve is built to modulate actuation pressure with a constant duty cycle, and time-frequency domain data are acquired. Measurements are utilized to assess analytical observations, and all methods show that the speed-dependent brake torque amplitudes can be altered with an appropriate modulation of actuation pressure.

  3. Upscaling pore pressure-dependent gas permeability in shales

    NASA Astrophysics Data System (ADS)

    Ghanbarian, Behzad; Javadpour, Farzam

    2017-04-01

    Upscaling pore pressure dependence of shale gas permeability is of great importance and interest in the investigation of gas production in unconventional reservoirs. In this study, we apply the Effective Medium Approximation, an upscaling technique from statistical physics, and modify the Doyen model for unconventional rocks. We develop an upscaling model to estimate the pore pressure-dependent gas permeability from pore throat size distribution, pore connectivity, tortuosity, porosity, and gas characteristics. We compare our adapted model with six data sets: three experiments, one pore-network model, and two lattice-Boltzmann simulations. Results showed that the proposed model estimated the gas permeability within a factor of 3 of the measurements/simulations in all data sets except the Eagle Ford experiment for which we discuss plausible sources of discrepancies.

  4. Fluidic origami with embedded pressure dependent multi-stability: a plant inspired innovation

    PubMed Central

    Li, Suyi; Wang, K. W.

    2015-01-01

    Inspired by the impulsive movements in plants, this research investigates the physics of a novel fluidic origami concept for its pressure-dependent multi-stability. In this innovation, fluid-filled tubular cells are synthesized by integrating different Miura-Ori sheets into a three-dimensional topological system, where the internal pressures are strategically controlled similar to the motor cells in plants. Fluidic origami incorporates two crucial physiological features observed in nature: one is distributed, pressurized cellular organization, and the other is embedded multi-stability. For a single fluidic origami cell, two stable folding configurations can coexist due to the nonlinear relationships among folding, crease material deformation and internal volume change. When multiple origami cells are integrated, additional multi-stability characteristics could occur via the interactions between pressurized cells. Changes in the fluid pressure can tailor the existence and shapes of these stable folding configurations. As a result, fluidic origami can switch between being mono-stable, bistable and multi-stable with pressure control, and provide a rapid ‘snap-through’ type of shape change based on the similar principles as in plants. The outcomes of this research could lead to the development of new adaptive materials or structures, and provide insights for future plant physiology studies at the cellular level. PMID:26400197

  5. Fluidic origami with embedded pressure dependent multi-stability: a plant inspired innovation.

    PubMed

    Li, Suyi; Wang, K W

    2015-10-06

    Inspired by the impulsive movements in plants, this research investigates the physics of a novel fluidic origami concept for its pressure-dependent multi-stability. In this innovation, fluid-filled tubular cells are synthesized by integrating different Miura-Ori sheets into a three-dimensional topological system, where the internal pressures are strategically controlled similar to the motor cells in plants. Fluidic origami incorporates two crucial physiological features observed in nature: one is distributed, pressurized cellular organization, and the other is embedded multi-stability. For a single fluidic origami cell, two stable folding configurations can coexist due to the nonlinear relationships among folding, crease material deformation and internal volume change. When multiple origami cells are integrated, additional multi-stability characteristics could occur via the interactions between pressurized cells. Changes in the fluid pressure can tailor the existence and shapes of these stable folding configurations. As a result, fluidic origami can switch between being mono-stable, bistable and multi-stable with pressure control, and provide a rapid 'snap-through' type of shape change based on the similar principles as in plants. The outcomes of this research could lead to the development of new adaptive materials or structures, and provide insights for future plant physiology studies at the cellular level. © 2015 The Author(s).

  6. Temperature and pressure dependent thermodynamic behavior of 2H-CuInO2

    NASA Astrophysics Data System (ADS)

    Bhamu, K. C.

    2018-05-01

    Density functional theory and quasi-harmonic Debye model has been used to study the thermodynamic properties of 2H-CuInO2. At the optimized structural parameters, pressure (0 to 80 GPa) dependent variation in the various thermodynamic properties, i.e. unit cell volume (V), bulk modulus (B), specific heat (Cv), Debye temperature (θD), Grüneisen parameter (γ) and thermal expansion coefficient (α) are calculated for various temperature values. The results predict that the pressure has significant effect on unit cell volume and bulk modulus while the temperature shows negligible effect on both parameters. With increasing temperature thermal expansion coefficient increase while with increasing pressure it decreases. The specific heat remains close to zero for ambient pressure and temperature values and it increases with increasing temperature. It is observed that the pressure has high impact on Debye temperature and Grüneisen parameter instead of temperature. Debye temperature and Grüneisen parameter both remains almost constant for the temperature range (0-300K) while Grüneisen parameter decrease with increasing pressure at constant temperature and Debye temperature increases rapidly with increasing pressure. An increase in Debye temperature with respect to pressure shows that the thermal vibration frequency changes rapidly.

  7. Pressure and temperature dependences of the reaction of OH with nitric acid

    NASA Technical Reports Server (NTRS)

    Stachnik, R. A.; Molina, L. T.; Molina, M. J.

    1986-01-01

    Rate constants for the reaction of OH with HNO3 have been measured by using a laser flash photolysis resonance absorption technique at 298 and 248 K in the presence of 10-730 Torr of He, N2, and SF6. A dependence on total pressure was observed with rate constant values increasing at 298 K from 1.11 x 10 to the -13th cu cm/molecule/s at 10 Torr to 1.45 x 10 to the -13th cu cm/molecule/s at 730 Torr, and at 248 K from 1.87 x 10 to the -13th cu cm/molecule/s at 10 Torr to 3.07 x 10 to the -13th cu cm/molecule/s at 730 Torr with helium as the diluent gas. Falloff behavior occurred at lower pressures with SF6 or N2 as the diluent gas. Extrapolated zero pressure rate constants were determined and correspond to an Arrhenius activation energy of E/R = -710 K.

  8. Temperature and pressure dependences of kimberlite melts viscosity (experimental-theoretical study)

    NASA Astrophysics Data System (ADS)

    Persikov, Eduard; Bykhtiyarov, Pavel; Cokol, Alexsander

    2016-04-01

    Experimental data on temperature and pressure dependences of viscosity of model kimberlite melts (silicate 82 + carbonate 18, wt. %, 100NBO/T = 313) have been obtained for the first time at 100 MPa of CO2 pressure and at the lithostatic pressures up to 7.5 GPa in the temperature range 1350 oC - 1950 oC using radiation high gas pressure apparatus and press free split-sphere multi - anvil apparatus (BARS). Experimental data obtained on temperature and pressure dependences of viscosity of model kimberlite melts at moderate and high pressures is compared with predicted data on these dependences of viscosity of basaltic melts (100NBO/T = 58) in the same T, P - range. Dependences of the viscosity of model kimberlite and basaltic melts on temperature are consistent to the exponential Arrenian equation in the T, P - range of experimental study. The correct values of activation energies of viscous flow of kimberlite melts have been obtained for the first time. The activation energies of viscous flow of model kimberlite melts exponentially increase with increasing pressure and are equal: E = 130 ± 1.3 kJ/mole at moderate pressure (P = 100 MPa) and E = 160 ± 1.6 kJ/mole at high pressure (P = 5.5 GPa). It has been established too that the viscosity of model kimberlite melts exponentially increases on about half order of magnitude with increasing pressures from 100 MPa to 7.5 GPa at the isothermal condition (1800 oC). It has been established that viscosity of model kimberlite melts at the moderate pressure (100 MPa) is lover on about one order of magnitude to compare with the viscosity of basaltic melts, but at high pressure range (5.5 - 7.5 GPa), on the contrary, is higher on about half order of magnitude at the same values of the temperatures. Here we use both a new experimental data on viscosity of kimberlite melts and our structural chemical model for calculation and prediction the viscosity of magmatic melts [1] to determine the fundamental features of viscosity of

  9. Pressure dependence of critical temperature of bulk FeSe from spin fluctuation theory

    NASA Astrophysics Data System (ADS)

    Hirschfeld, Peter; Kreisel, Andreas; Wang, Yan; Tomic, Milan; Jeschke, Harald; Jacko, Anthony; Valenti, Roser; Maier, Thomas; Scalapino, Douglas

    2013-03-01

    The critical temperature of the 8K superconductor FeSe is extremely sensitive to pressure, rising to a maximum of 40K at about 10GPa. We test the ability of the current generation of fluctuation exchange pairing theories to account for this effect, by downfolding the density functional theory electronic structure for each pressure to a tight binding model. The Fermi surface found in such a procedure is then used with fixed Hubbard parameters to determine the pairing strength using the random phase approximation for the spin singlet pairing vertex. We find that the evolution of the Fermi surface captured by such an approach is alone not sufficient to explain the observed pressure dependence, and discuss alternative approaches. PJH, YW, AK were supported by DOE DE-FG02-05ER46236, the financial support of MT, HJ, and RV from the DFG Schwerpunktprogramm 1458 is kindly acknowledged.

  10. Metastable Ar(1 s5) density dependence on pressure and argon-helium mixture in a high pressure radio frequency dielectric barrier discharge

    NASA Astrophysics Data System (ADS)

    Emmons, D. J.; Weeks, D. E.; Eshel, B.; Perram, G. P.

    2018-01-01

    Simulations of an α-mode radio frequency dielectric barrier discharge are performed for varying mixtures of argon and helium at pressures ranging from 200 to 500 Torr using both zero and one-dimensional models. Metastable densities are analyzed as a function of argon-helium mixture and pressure to determine the optimal conditions, maximizing metastable density for use in an optically pumped rare gas laser. Argon fractions corresponding to the peak metastable densities are found to be pressure dependent, shifting from approximately 15% Ar in He at 200 Torr to 10% at 500 Torr. A decrease in metastable density is observed as pressure is increased due to a diminution in the reduced electric field and a quadratic increase in metastable loss rates through A r2* formation. A zero-dimensional effective direct current model of the dielectric barrier discharge is implemented, showing agreement with the trends predicted by the one-dimensional fluid model in the bulk plasma.

  11. Thermoelasticity and anomalies in the pressure dependence of phonon velocities in niobium

    NASA Astrophysics Data System (ADS)

    Zou, Yongtao; Li, Ying; Chen, Haiyan; Welch, David; Zhao, Yusheng; Li, Baosheng

    2018-01-01

    Compressional and shear wave velocities of polycrystalline niobium have been measured at simultaneously high pressures and temperatures up to 5.8 GPa and 1073 K, respectively, using ultrasonic interferometry in conjunction with synchrotron x-ray techniques. An anomalous pressure-induced softening behavior in the phonon velocities, probably owing to the topological change in the Fermi surface, has been observed at ˜4.8 GPa during cold compression, which is supported by the elasticity data from our first-principles calculations. In contrast, both the bulk (BS) and shear (G) moduli increase with pressures but decrease with temperatures upon compression at extreme P-T up to 5.8 GPa and 1073 K. Using finite strain equation-of-state approaches, the elasticity of bulk and shear moduli and their pressure and temperature dependences are derived from the directly measured velocities and densities, yielding BS0 = 174.9(3.2) GPa, G0 = 37.1(3) GPa, ∂BS/∂P = 3.97(9), ∂G/∂P = 0.83(5), ∂BS/∂T = -0.064(7) GPa/K, and ∂G/∂T = -0.012(3) GPa/K. On the basis of the current thermoelasticity data, Debye temperature and the high-pressure melting curve of Nb are derived. The origin of the anomalies in shear behavior at high pressure might be attributed to the progressive s-d electron-transfer-induced topological changes of the Fermi surface upon compression.

  12. Development of a Pressure-Dependent Constitutive Model with Combined Multilinear Kinematic and Isotropic Hardening

    NASA Technical Reports Server (NTRS)

    Allen Phillip A.; Wilson, Christopher D.

    2003-01-01

    The development of a pressure-dependent constitutive model with combined multilinear kinematic and isotropic hardening is presented. The constitutive model is developed using the ABAQUS user material subroutine (UMAT). First the pressure-dependent plasticity model is derived. Following this, the combined bilinear and combined multilinear hardening equations are developed for von Mises plasticity theory. The hardening rule equations are then modified to include pressure dependency. The method for implementing the new constitutive model into ABAQUS is given.

  13. An effective medium approach to modelling the pressure-dependent electrical properties of porous rocks

    NASA Astrophysics Data System (ADS)

    Han, Tongcheng

    2018-07-01

    Understanding the electrical properties of rocks under varying pressure is important for a variety of geophysical applications. This study proposes an approach to modelling the pressure-dependent electrical properties of porous rocks based on an effective medium model. The so-named Textural model uses the aspect ratios and pressure-dependent volume fractions of the pores and the aspect ratio and electrical conductivity of the matrix grains. The pores were represented by randomly oriented stiff and compliant spheroidal shapes with constant aspect ratios, and their pressure-dependent volume fractions were inverted from the measured variation of total porosity with differential pressure using a dual porosity model. The unknown constant stiff and compliant pore aspect ratios and the aspect ratio and electrical conductivity of the matrix grains were inverted by best fitting the modelled electrical formation factor to the measured data. Application of the approach to three sandstone samples covering a broad porosity range showed that the pressure-dependent electrical properties can be satisfactorily modelled by the proposed approach. The results demonstrate that the dual porosity concept is sufficient to explain the electrical properties of porous rocks under pressure through the effective medium model scheme.

  14. Brittle Creep of Tournemire Shale: Orientation, Temperature and Pressure Dependences

    NASA Astrophysics Data System (ADS)

    Geng, Zhi; Bonnelye, Audrey; Dick, Pierre; David, Christian; Chen, Mian; Schubnel, Alexandre

    2017-04-01

    Time and temperature dependent rock deformation has both scientific and socio-economic implications for natural hazards, the oil and gas industry and nuclear waste disposal. During the past decades, most studies on brittle creep have focused on igneous rocks and porous sedimentary rocks. To our knowledge, only few studies have been carried out on the brittle creep behavior of shale. Here, we conducted a series of creep experiments on shale specimens coming from the French Institute for Nuclear Safety (IRSN) underground research laboratory located in Tournemire, France. Conventional tri-axial experiments were carried under two different temperatures (26˚ C, 75˚ C) and confining pressures (10 MPa, 80 MPa), for three orientations (σ1 along, perpendicular and 45˚ to bedding). Following the methodology developed by Heap et al. [2008], differential stress was first increased to ˜ 60% of the short term peak strength (10-7/s, Bonnelye et al. 2016), and then in steps of 5 to 10 MPa every 24 hours until brittle failure was achieved. In these long-term experiments (approximately 10 days), stress and strains were recorded continuously, while ultrasonic acoustic velocities were recorded every 1˜15 minutes, enabling us to monitor the evolution of elastic wave speed anisotropy. Temporal evolution of anisotropy was illustrated by inverting acoustic velocities to Thomsen parameters. Finally, samples were investigated post-mortem using scanning electron microscopy. Our results seem to contradict our traditional understanding of loading rate dependent brittle failure. Indeed, the brittle creep failure stress of our Tournemire shale samples was systematically observed ˜50% higher than its short-term peak strength, with larger final axial strain accumulated. At higher temperatures, the creep failure strength of our samples was slightly reduced and deformation was characterized with faster 'steady-state' creep axial strain rates at each steps, and larger final axial strain

  15. Pressure-Dependent Light Emission of Charged and Neutral Excitons in Monolayer MoSe 2

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

    Fu, Xinpeng; Li, Fangfei; Lin, Jung-Fu

    Tailoring the excitonic properties in two-dimensional monolayer transition metal dichalcogenides (TMDs) through strain engineering is an effective means to explore their potential applications in optoelectronics and nanoelectronics. Here we report pressure-tuned photon emission of trions and excitons in monolayer MoSe2 via a diamond anvil cell (DAC) through photoluminescence measurements and theoretical calculations. Under quasi-hydrostatic compressive strain, our results show neutral (X0) and charged (X–) exciton emission of monolayer MoSe2 can be effectively tuned by alcohol mixture vs inert argon pressure transmitting media (PTM). During this process, X– emission undergoes a continuous blue shift until reaching saturation, while X0 emission turnsmore » up splitting. The pressure-dependent charging effect observed in alcohol mixture PTM results in the increase of the X– exciton component and facilitates the pressure-tuned emission of X– excitons. This substantial tunability of X– and X0 excitons in MoSe2 can be extended to other 2D TMDs, which holds potential for developing strained and optical sensing devices.« less

  16. Experimental evaluation of the pressure and temperature dependence of ion-induced nucleation.

    PubMed

    Munir, Muhammad Miftahul; Suhendi, Asep; Ogi, Takashi; Iskandar, Ferry; Okuyama, Kikuo

    2010-09-28

    An experimental system for the study of ion-induced nucleation in a SO(2)/H(2)O/N(2) gas mixture was developed, employing a soft x-ray at different pressure and temperature levels. The difficulties associated with these experiments included the changes in physical properties of the gas mixture when temperature and pressure were varied. Changes in the relative humidity (RH) as a function of pressure and temperature also had a significant effect on the different behaviors of the mobility distributions of particles. In order to accomplish reliable measurement and minimize uncertainties, an integrated on-line control system was utilized. As the pressure decreased in a range of 500-980 hPa, the peak concentration of both ions and nanometer-sized particles decreased, which suggests that higher pressure tended to enhance the growth of particles nucleated by ion-induced nucleation. Moreover, the modal diameters of the measured particle size distributions showed a systematic shift to larger sizes with increasing pressure. However, in the temperature range of 5-20 °C, temperature increases had no significant effects on the mobility distribution of particles. The effects of residence time, RH (7%-70%), and SO(2) concentration (0.08-6.7 ppm) on ion-induced nucleation were also systematically investigated. The results show that the nucleation and growth were significantly dependent on the residence time, RH, and SO(2) concentration, which is in agreement with both a previous model and previous observations. This research will be inevitable for a better understanding of the role of ions in an atmospheric nucleation mechanism.

  17. Pressure-dependence of the phase transitions and thermal expansion in zirconium and hafnium pyrovanadate

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

    Gallington, Leighanne C.; Hester, Brett R.; Kaplan, Benjamin S.

    Low or negative thermal expansion (NTE) has been previously observed in members of the ZrP{sub 2}O{sub 7} family at temperatures higher than their order-disorder phase transitions. The thermoelastic properties and phase behavior of the low temperature superstructure and high temperature negative thermal expansion phases of ZrV{sub 2}O{sub 7} and HfV{sub 2}O{sub 7} were explored via in situ variable temperature/pressure powder x-ray diffraction measurements. The phase transition temperatures of ZrV{sub 2}O{sub 7} and HfV{sub 2}O{sub 7} exhibited a very strong dependence on pressure (∼700 K GPa), with moderate compression suppressing the formation of their NTE phases below 513 K. Compression alsomore » reduced the magnitude of the coefficients of thermal expansion in both the positive and negative thermal expansion phases. Additionally, the high temperature NTE phase of ZrV{sub 2}O{sub 7} was found to be twice as stiff as the low temperature positive thermal expansion superstructure (24 and 12 GPa respectively). - Graphical abstract: The temperature at which ZrV{sub 2}O{sub 7} transforms to a phase displaying negative thermal expansion is strongly pressure dependent. The high temperature form of ZrV{sub 2}O{sub 7} is elastically stiffer than the low temperature form. - Highlights: • The order-disorder phase transition temperatures in ZrV{sub 2}O{sub 7} and HfV{sub 2}O{sub 7} are strongly pressure dependent (∼700 K.GPa). • The high temperature (disordered) phase of ZrV{sub 2}O{sub 7} is much stiffer than the ambient temperature (ordered) phase. • Compression reduces the magnitude of the negative thermal expansion in the high temperature phase of ZrV{sub 2}O{sub 7}.« less

  18. Pore-pressure sensitivities to dynamic strains: observations in active tectonic regions

    USGS Publications Warehouse

    Barbour, Andrew J.

    2015-01-01

    Triggered seismicity arising from dynamic stresses is often explained by the Mohr-Coulomb failure criterion, where elevated pore pressures reduce the effective strength of faults in fluid-saturated rock. The seismic response of a fluid-rock system naturally depends on its hydro-mechanical properties, but accurately assessing how pore-fluid pressure responds to applied stress over large scales in situ remains a challenging task; hence, spatial variations in response are not well understood, especially around active faults. Here I analyze previously unutilized records of dynamic strain and pore-pressure from regional and teleseismic earthquakes at Plate Boundary Observatory (PBO) stations from 2006 through 2012 to investigate variations in response along the Pacific/North American tectonic plate boundary. I find robust scaling-response coefficients between excess pore pressure and dynamic strain at each station that are spatially correlated: around the San Andreas and San Jacinto fault systems, the response is lowest in regions of the crust undergoing the highest rates of secular shear strain. PBO stations in the Parkfield instrument cluster are at comparable distances to the San Andreas fault (SAF), and spatial variations there follow patterns in dextral creep rates along the fault, with the highest response in the actively creeping section, which is consistent with a narrowing zone of strain accumulation seen in geodetic velocity profiles. At stations in the San Juan Bautista (SJB) and Anza instrument clusters, the response depends non-linearly on the inverse fault-perpendicular distance, with the response decreasing towards the fault; the SJB cluster is at the northern transition from creeping-to-locked behavior along the SAF, where creep rates are at moderate to low levels, and the Anza cluster is around the San Jacinto fault, where to date there have been no statistically significant creep rates observed at the surface. These results suggest that the strength

  19. Focal cartilage defect compromises fluid-pressure dependent load support in the knee joint.

    PubMed

    Dabiri, Yaghoub; Li, LePing

    2015-06-01

    A focal cartilage defect involves tissue loss or rupture. Altered mechanics in the affected joint may play an essential role in the onset and progression of osteoarthritis. The objective of the present study was to determine the compromised load support in the human knee joint during defect progression from the cartilage surface to the cartilage-bone interface. Ten normal and defect cases were simulated with a previously tested 3D finite element model of the knee. The focal defects were considered in both condyles within high load-bearing regions. Fluid pressurization, anisotropic fibril-reinforcement, and depth-dependent mechanical properties were considered for the articular cartilages and menisci. The results showed that a small cartilage defect could cause 25% reduction in the load support of the knee joint due to a reduced capacity of fluid pressurization in the defect cartilage. A partial-thickness defect could cause a fluid pressure decrease or increase in the remaining underlying cartilage depending on the defect depth. A cartilage defect also increased the shear strain at the cartilage-bone interface, which was more significant with a full-thickness defect. The effect of cartilage defect on the fluid pressurization also depended on the defect sites and contact conditions. In conclusion, a focal cartilage defect causes a fluid-pressure dependent load reallocation and a compromised load support in the joint, which depend on the defect depth, site, and contact condition. Copyright © 2015 John Wiley & Sons, Ltd.

  20. Atmospheric pressure loading parameters from very long baseline interferometry observations

    NASA Technical Reports Server (NTRS)

    Macmillan, D. S.; Gipson, John M.

    1994-01-01

    Atmospheric mass loading produces a primarily vertical displacement of the Earth's crust. This displacement is correlated with surface pressure and is large enough to be detected by very long baseline interferometry (VLBI) measurements. Using the measured surface pressure at VLBI stations, we have estimated the atmospheric loading term for each station location directly from VLBI data acquired from 1979 to 1992. Our estimates of the vertical sensitivity to change in pressure range from 0 to -0.6 mm/mbar depending on the station. These estimates agree with inverted barometer model calculations (Manabe et al., 1991; vanDam and Herring, 1994) of the vertical displacement sensitivity computed by convolving actual pressure distributions with loading Green's functions. The pressure sensitivity tends to be smaller for stations near the coast, which is consistent with the inverted barometer hypothesis. Applying this estimated pressure loading correction in standard VLBI geodetic analysis improves the repeatability of estimated lengths of 25 out of 37 baselines that were measured at least 50 times. In a root-sum-square (rss) sense, the improvement generally increases with baseline length at a rate of about 0.3 to 0.6 ppb depending on whether the baseline stations are close to the coast. For the 5998-km baseline from Westford, Massachusetts, to Wettzell, Germany, the rss improvement is about 3.6 mm out of 11.0 mm. The average rss reduction of the vertical scatter for inland stations ranges from 2.7 to 5.4 mm.

  1. Tire pressure special study : vehicle observation data

    DOT National Transportation Integrated Search

    2001-08-01

    Twenty seven percent of passenger cars with : regular passenger car tires have at least one : tire that is underinflated by 8 psi or more. : Tire Pressure Special Study: Vehicle : Observation Data is the third in a series of : research notes co...

  2. Pressure dependence of axisymmetric vortices in superfluid 3B

    NASA Astrophysics Data System (ADS)

    Fetter, Alexander L.

    1985-06-01

    The pressure dependence of the vortex core in rotating 3B is studied in the Ginzburg-Landau formalism with two distinct models of the strong-coupling corrections. The parametrization of Sauls and Serene [Phys. Rev. B 24, 183 (1981)] predicts a transition from a core with large magnetic moment below ~10 bars to one with small magnetic moment for higher pressures, in qualitative agreement with experiments. The earlier one-parameter model of Brinkman, Serene, and Anderson predicts no such transition, with the core having a large moment for all values of the parameter δ.

  3. Influence of the pressure dependent coefficient of friction on deep drawing springback predictions

    NASA Astrophysics Data System (ADS)

    Gil, Imanol; Galdos, Lander; Mendiguren, Joseba; Mugarra, Endika; Sáenz de Argandoña, Eneko

    2016-10-01

    This research studies the effect of considering an advanced variable friction coefficient on the springback prediction of stamping processes. Traditional constant coefficient of friction considerations are being replaced by more advanced friction coefficient definitions. The aim of this work is to show the influence of defining a pressure dependent friction coefficient on numerical springback predictions of a DX54D mild steel, a HSLA380 and a DP780 high strength steel. The pressure dependent friction model of each material was fitted to the experimental data obtained by Strip Drawing tests. Then, these friction models were implemented in a numerical simulation of a drawing process of an industrial automotive part. The results showed important differences between defining a pressure dependent friction coefficient or a constant friction coefficient.

  4. Scale-dependent coupling of hysteretic capillary pressure, trapping, and fluid mobilities

    NASA Astrophysics Data System (ADS)

    Doster, F.; Celia, M. A.; Nordbotten, J. M.

    2012-12-01

    Many applications of multiphase flow in porous media, including CO2-storage and enhanced oil recovery, require mathematical models that span a large range of length scales. In the context of numerical simulations, practical grid sizes are often on the order of tens of meters, thereby de facto defining a coarse model scale. Under particular conditions, it is possible to approximate the sub-grid-scale distribution of the fluid saturation within a grid cell; that reconstructed saturation can then be used to compute effective properties at the coarse scale. If both the density difference between the fluids and the vertical extend of the grid cell are large, and buoyant segregation within the cell on a sufficiently shorte time scale, then the phase pressure distributions are essentially hydrostatic and the saturation profile can be reconstructed from the inferred capillary pressures. However, the saturation reconstruction may not be unique because the parameters and parameter functions of classical formulations of two-phase flow in porous media - the relative permeability functions, the capillary pressure -saturation relationship, and the residual saturations - show path dependence, i.e. their values depend not only on the state variables but also on their drainage and imbibition histories. In this study we focus on capillary pressure hysteresis and trapping and show that the contribution of hysteresis to effective quantities is dependent on the vertical length scale. By studying the transition from the two extreme cases - the homogeneous saturation distribution for small vertical extents and the completely segregated distribution for large extents - we identify how hysteretic capillary pressure at the local scale induces hysteresis in all coarse-scale quantities for medium vertical extents and finally vanishes for large vertical extents. Our results allow for more accurate vertically integrated modeling while improving our understanding of the coupling of capillary

  5. Pressure Dependence of the Superfluid Fraction in 3He-A1

    NASA Astrophysics Data System (ADS)

    Bastea, M.; Okuda, Y.; Kojima, H.

    1995-03-01

    The superfluid fraction of 3He-A1 was determined in the Ginzburg-Landau (GL) region as a function of pressure between 10 and 30 bars from the measured spin-entropy wave velocity. The pressure dependence of the parameter β24, proportional to the fourth order coefficients of GL free energy expansion, was measured for the first time. At low pressures the parameter approaches the weak coupling limit in agreement with the theory of Sauls and Serene. The extracted strong coupling corrections to β24 and β5 at higher pressures are also consistent with the theory.

  6. A Pressure-Dependent Damage Model for Energetic Materials

    DTIC Science & Technology

    2013-04-01

    appropriate damage nucleation and evolution laws, and the equation of state ) with its reactive response. 15. SUBJECT TERMS pressure-dependent...evolution laws, and the equation of state ) with its reactive response. INTRODUCTION Explosions and deflagrations are classifications of sub-detonative...energetic material’s mechanical response (through the yield criterion, damage evolution and equation of state ) with its reactive response. DAMAGE-FREE

  7. Pressure-dependent ground states and fermiology in β- ( BDA-TTP ) 2 M Cl4 ( M=Fe,Ga )

    NASA Astrophysics Data System (ADS)

    Choi, E. S.; Graf, D.; Brooks, J. S.; Yamada, J.; Akutsu, H.; Kikuchi, K.; Tokumoto, M.

    2004-07-01

    We have investigated pressure- and magnetic-field-dependent electrical transport properties in the charge transfer salts β-(BDA-TTP)2MCl4(M=Fe,Ga) , both of which show a metal-insulator (MI) transition around 120K at ambient pressure. The zero field temperature-pressure phase diagrams of the two compounds are quite similar; the MI transition temperature decreases with pressure, and superconductivity is observed in both the magnetic and non-magnetic compounds above ˜4.5kbar . Likewise, Shubnikov-de Haas effect measurements show nearly identical Fermi surfaces. These similarities suggest that the magnetic interaction J between the conduction electrons and the magnetic moments in β-(BDA-TTP)2FeCl4 is small. Nevertheless, magnetoresistance measurements show remarkable differences and reveal that magnetic interactions with the conduction electrons are still effective in M=Fe compounds.

  8. Effect of Time-Dependent Pinning Pressure on Abnormal Grain Growth: Phase Field Simulation

    NASA Astrophysics Data System (ADS)

    Kim, Jeong Min; Min, Guensik; Shim, Jae-Hyeok; Lee, Kyung Jong

    2018-05-01

    The effect of the time-dependent pinning pressure of precipitates on abnormal grain growth has been investigated by multiphase field simulation with a simple precipitation model. The application of constant pinning pressure is problematic because it always induces abnormal grain growth or no grain growth, which is not reasonable considering the real situation. To produce time-dependent pinning pressure, both precipitation kinetics and precipitate coarsening kinetics have been considered with two rates: slow and fast. The results show that abnormal grain growth is suppressed at the slow precipitation rate. At the slow precipitation rate, the overall grain growth caused by the low pinning pressure in the early stage indeed plays a role in preventing abnormal grain growth by reducing the mobility advantage of abnormal grains. In addition, the fast precipitate coarsening rate tends to more quickly transform abnormal grain growth into normal grain growth by inducing the active growth of grains adjacent to the abnormal grains in the early stage. Therefore, the present study demonstrates that the time dependence of the pinning pressure of precipitates is a critical factor that determines the grain growth mode.

  9. Effect of Time-Dependent Pinning Pressure on Abnormal Grain Growth: Phase Field Simulation

    NASA Astrophysics Data System (ADS)

    Kim, Jeong Min; Min, Guensik; Shim, Jae-Hyeok; Lee, Kyung Jong

    2018-03-01

    The effect of the time-dependent pinning pressure of precipitates on abnormal grain growth has been investigated by multiphase field simulation with a simple precipitation model. The application of constant pinning pressure is problematic because it always induces abnormal grain growth or no grain growth, which is not reasonable considering the real situation. To produce time-dependent pinning pressure, both precipitation kinetics and precipitate coarsening kinetics have been considered with two rates: slow and fast. The results show that abnormal grain growth is suppressed at the slow precipitation rate. At the slow precipitation rate, the overall grain growth caused by the low pinning pressure in the early stage indeed plays a role in preventing abnormal grain growth by reducing the mobility advantage of abnormal grains. In addition, the fast precipitate coarsening rate tends to more quickly transform abnormal grain growth into normal grain growth by inducing the active growth of grains adjacent to the abnormal grains in the early stage. Therefore, the present study demonstrates that the time dependence of the pinning pressure of precipitates is a critical factor that determines the grain growth mode.

  10. Anisotropic physical properties and pressure dependent magnetic ordering of CrAuTe 4

    DOE PAGES

    Jo, Na Hyun; Kaluarachchi, Udhara S.; Wu, Yun; ...

    2016-11-11

    Systematic measurements of temperature-dependent magnetization, resistivity, and angle-resolved photoemission spectroscopy (ARPES) at ambient pressure as well as resistivity under pressures up to 5.25 GPa were conducted on single crystals of CrAuTe 4. Magnetization data suggest that magnetic moments are aligned antiferromagnetically along the crystallographic c axis below T N = 255 K. ARPES measurements show band reconstruction due to the magnetic ordering. Magnetoresistance data show clear anisotropy, and, at high fields, quantum oscillations. The Néel temperature decreases monotonically under pressure, decreasing to T N = 236 K at 5.22 GPa. The pressure dependencies of (i) T N, (ii) the residualmore » resistivity ratio, and (iii) the size and power-law behavior of the low-temperature magnetoresistance all show anomalies near 2 GPa suggesting that there may be a phase transition (structural, magnetic, and/or electronic) induced by pressure. Lastly, for pressures higher than 2 GPa a significantly different quantum oscillation frequency emerges, consistent with a pressure induced change in the electronic states.« less

  11. Study of Defect Levels in InAs/InAsSb Type-II Superlattice Using Pressure-Dependent Photoluminescence

    DTIC Science & Technology

    2015-07-07

    pressure is confirmed from power dependent PL measurements. We also examined the thermal activation energies at ambient pressure and close to the...with pressure is confirmed from power dependent PL measurements. We also examined the thermal activation energies at ambient pressure and close to...We also examined the thermal activation energies at ambient pressure and close to the crossover pressure. These results support and are consistent

  12. Pressure dependence of zero-field splittings in organic triplets. II. Carbonyls

    NASA Astrophysics Data System (ADS)

    Chan, I. Y.; Qian, X. Q.

    1990-01-01

    We have conducted optically detected magnetic resonance (ODMR) experiments at pressure up to 40 kbar for neat biactyl (BA), neat benzil (BZ), and acetophenone (AP) doped in dibromobenzene (DBB). The pressure dependences of their zero-field splitting (ZFS) parameters D and E are reported. For BA and BZ systems, the ‖D‖ value decreases greatly with increasing pressure. This behavior is in contrast with that of benzophenone (BP), whose ‖D‖ value increases sigmoidally 13% over the same pressure range. These results may be rationalized in a qualitative theory based on pressure modulation of the spin-orbit coupling (SOC) contribution to the ZFS. ln aromatic ketones, lattice compression modifies the twist angle of the phenyl ring(s) relative to the carbonyl frame, thus changing the energy of the 3ππ* state relative to that of the 3nπ* state. This variation of the energy denominator in a second order perturbation enhances the SOC contribution to the ZFS. In comparison, the increase of spin-spin (SS) dipolar interaction by isotropic compression is relatively unimportant. Consistent with this picture, the very small 3ππ*-3nπ* energy gap produces an enormous pressure sensitivity of D and E in AP/DBB. The behavior of the ZFS in this case may be interpreted as a consequence of pressure tuning of the 3ππ* state through an anticrossing region. In addition, a new set of high frequency ODMR signals appears under pressure. This is attributed to a new site of AP having the 3nπ* as the phosphorescent triplet state. The pressure dependence of ZFS for benzil shows complicated fine structure. This is a testimony to the flexible nature of benzil in both the dihedral angle of the dicarbonyl fragment and the phenyl twist angle.

  13. Estimating outflow facility through pressure dependent pathways of the human eye

    PubMed Central

    Gardiner, Bruce S.

    2017-01-01

    We develop and test a new theory for pressure dependent outflow from the eye. The theory comprises three main parameters: (i) a constant hydraulic conductivity, (ii) an exponential decay constant and (iii) a no-flow intraocular pressure, from which the total pressure dependent outflow, average outflow facilities and local outflow facilities for the whole eye may be evaluated. We use a new notation to specify precisely the meaning of model parameters and so model outputs. Drawing on a range of published data, we apply the theory to animal eyes, enucleated eyes and in vivo human eyes, and demonstrate how to evaluate model parameters. It is shown that the theory can fit high quality experimental data remarkably well. The new theory predicts that outflow facilities and total pressure dependent outflow for the whole eye are more than twice as large as estimates based on the Goldman equation and fluorometric analysis of anterior aqueous outflow. It appears likely that this discrepancy can be largely explained by pseudofacility and aqueous flow through the retinal pigmented epithelium, while any residual discrepancy may be due to pathological processes in aged eyes. The model predicts that if the hydraulic conductivity is too small, or the exponential decay constant is too large, then intraocular eye pressure may become unstable when subjected to normal circadian changes in aqueous production. The model also predicts relationships between variables that may be helpful when planning future experiments, and the model generates many novel testable hypotheses. With additional research, the analysis described here may find application in the differential diagnosis, prognosis and monitoring of glaucoma. PMID:29261696

  14. Kinematically irreversible particle motion in 2D suspensions due to surface-pressure-dependent surface rheology

    NASA Astrophysics Data System (ADS)

    Manikantan, Harishankar; Squires, Todd

    2017-11-01

    The surface viscosity of many insoluble surfactants depends strongly on the surface pressure (or surface tension) of that surfactant. Surface pressure gradients naturally arise in interfacial flows, and surface-pressure-dependent surface rheology alters 2D suspension dynamics in significant ways. We use the Lorentz reciprocal theorem to asymptotically quantify the irreversible dynamics that break Newtonian symmetries. We first show that a particle embedded in a surfactant-laden interface and translating parallel to or rotating near an interfacial boundary experiences a force in the direction perpendicular to the boundary. Building on this, we extend the theory to compute the first effects of pressure-dependent surface viscosity on 2D particle pairs in suspension. The fore-aft symmetry of pair trajectories in a Newtonian interface is lost, leading to well-separated (when pressure-thickening) or aggregated (when pressure-thinning) particles. Notably, the relative motion is kinematically irreversible, and pairs steadily evolve toward a particular displacement. Based on these irreversible pair interactions, we hypothesize that pressure-thickening (or -thinning) leads to shear-thinning (or -thickening) in 2D suspensions.

  15. The effects of stereotypes and observer pressure on athletic performance.

    PubMed

    Krendl, Anne; Gainsburg, Izzy; Ambady, Nalini

    2012-02-01

    Although the effects of negative stereotypes and observer pressure on athletic performance have been well researched, the effects of positive stereotypes on performance, particularly in the presence of observers, is not known. In the current study, White males watched a video either depicting Whites basketball players as the best free throwers in the NBA (positive stereotype), Black basketball players as the best free throwers in the NBA (negative stereotype), or a neutral sports video (control). Participants then shot a set of free throws, during which half the participants were also videotaped (observer condition), whereas the other half were not (no observer condition). Results demonstrated that positive stereotypes improved free throw performance, but only in the no observer condition. Interestingly, observer pressure interacted with the positive stereotype to lead to performance decrements. In the negative stereotype condition, performance decrements were observed both in the observer and no observer conditions.

  16. Pressure-dependent surface viscosity and its surprising consequences in interfacial lubrication flows

    NASA Astrophysics Data System (ADS)

    Manikantan, Harishankar; Squires, Todd M.

    2017-02-01

    The surface shear rheology of many insoluble surfactants depends strongly on the surface pressure (or concentration) of that surfactant. Here we highlight the dramatic consequences that surface-pressure-dependent surface viscosities have on interfacially dominant flows, by considering lubrication-style geometries within high Boussinesq (Bo) number flows. As with three-dimensional lubrication, high-Bo surfactant flows through thin gaps give high surface pressures, which in turn increase the local surface viscosity, further amplifying lubrication stresses and surface pressures. Despite their strong nonlinearity, the governing equations are separable, so that results from two-dimensional Newtonian lubrication analyses may be immediately adapted to treat surfactant monolayers with a general functional form of ηs(Π ) . Three paradigmatic systems are analyzed to reveal qualitatively new features: a maximum, self-limiting value for surfactant fluxes and particle migration velocities appears for Π -thickening surfactants, and kinematic reversibility is broken for the journal bearing and for suspensions more generally.

  17. How does pressure gravitate? Cosmological constant problem confronts observational cosmology

    NASA Astrophysics Data System (ADS)

    Narimani, Ali; Afshordi, Niayesh; Scott, Douglas

    2014-08-01

    An important and long-standing puzzle in the history of modern physics is the gross inconsistency between theoretical expectations and cosmological observations of the vacuum energy density, by at least 60 orders of magnitude, otherwise known as the cosmological constant problem. A characteristic feature of vacuum energy is that it has a pressure with the same amplitude, but opposite sign to its energy density, while all the precision tests of General Relativity are either in vacuum, or for media with negligible pressure. Therefore, one may wonder whether an anomalous coupling to pressure might be responsible for decoupling vacuum from gravity. We test this possibility in the context of the Gravitational Aether proposal, using current cosmological observations, which probe the gravity of relativistic pressure in the radiation era. Interestingly, we find that the best fit for anomalous pressure coupling is about half-way between General Relativity (GR), and Gravitational Aether (GA), if we include Planck together with WMAP and BICEP2 polarization cosmic microwave background (CMB) observations. Taken at face value, this data combination excludes both GR and GA at around the 3 σ level. However, including higher resolution CMB observations (``highL'') or baryonic acoustic oscillations (BAO) pushes the best fit closer to GR, excluding the Gravitational Aether solution to the cosmological constant problem at the 4- 5 σ level. This constraint effectively places a limit on the anomalous coupling to pressure in the parametrized post-Newtonian (PPN) expansion, ζ4 = 0.105 ± 0.049 (+highL CMB), or ζ4 = 0.066 ± 0.039 (+BAO). These represent the most precise measurement of this parameter to date, indicating a mild tension with GR (for ΛCDM including tensors, with 0ζ4=), and also among different data sets.

  18. Pressure Dependence of Komatiite Liquid Viscosity and Implications for Magma Ocean Rheology

    NASA Astrophysics Data System (ADS)

    O'Dwyer Brown, L.; Lesher, C. E.; Terasaki, H. G.; Yamada, A.; Sakamaki, T.; Shibazaki, Y.; Ohtani, E.

    2009-12-01

    The viscosities of komatiite liquids at high pressures and temperatures were investigated using the in-situ falling sphere technique at BL04B1, SPring-8. Komatiites are naturally occurring magmas, rich in network modifying cations. Despite the refractory and fluid nature of komatiite, we successfully measured the viscosity of molten komatiites from Gorgona Island, Colombia (MgO = 17.8 wt.%; NBO/T = 1.5) between 11 and 13 GPa at 2000 C, and from Belingwe, Zimbabwe (MgO = 28.14 wt.%; NBO/T = 2.1) from 12 to 14 GPa at 2000 C. Under isothermal conditions, the viscosity of Gorgona Island komatiite melt increased with pressure, consistent with our previous measurements at lower pressures for this composition. We interpreted this positive pressure dependence as the result of reductions in interatomic space diminishing the free volume of the liquid when compressed. The viscosity of molten komatiite from Belingwe also increased up to 12 GPa, however between 12 and 14 GPa the viscosity is nearly constant. In previous studies of depolymerized silicate liquids, the pressure dependence of viscosity has been shown to reverse from positive to negative between 8 and 10 GPa with corresponding changes in activation volume [1] [2]. In contrast, the activation volume for Belingwe liquid decreases to near zero, but does not become negative above 11 GPa. Similarly, the activation volume for Gorgona Island komatiite remains positive throughout the pressure range investigated. Molecular dynamics simulations of simple MgO-SiO2 liquids with NBO/T > 2 also show a positive pressure dependence, reflecting the dominant control of free-volume reduction on the viscosity of depolymerized melts. However, the more rapid reduction in activation volume with pressure in komatiite liquids may be related to the presence of Al, Ti and other cations that interact and undergo coordination changes unavailable in simple silicate liquids. Along Hadean and post-Hadean mantle adiabats the net effect of

  19. Movement of the lacrimal canalicular wall under intracanalicular pressure changes observed with dacryoendoscopy.

    PubMed

    Kakizaki, Hirohiko; Takahashi, Yasuhiro; Mito, Hidenori; Nakamura, Yasuhisa

    2015-01-01

    Movement of the lacrimal canalicular wall has been speculated to occur during blinking. Movement of the common internal ostium has been observed under nasal endoscopy, and pressure changes in the lacrimal canalicular cavity have been observed with a pressure sensor; however, lacrimal canalicular wall movement under pressure changes has not been observed. To examine movement of the lacrimal canalicular wall under intracanalicular pressure changes using dacryoendoscopy. The authors examined 20 obstruction-free lacrimal canaliculi in 10 patients. A dacryoendoscope was inserted, and water was poured into the intracanalicular cavity via the dacryoendoscope's water channel. The water was then poured or suctioned to cause positive or negative pressure changes in the intracanalicular cavity, and movement of the lacrimal canalicular wall was examined. The lacrimal canalicular wall moved flexibly with pressure changes. Under positive pressure, the intracanalicular cavity was dilated; however, it narrowed under negative pressure. The extent of movement was more dramatic in the common canalicular portion than the proximal canalicular portion. Intracanalicular pressure changes cause movement of the lacrimal canalicular wall. There was a consistent relationship between intracanalicular cavity changes and pressure changes, possibly contributing to lacrimal drainage of the canaliculus.

  20. Silicate melts: The “anomalous” pressure dependence of the viscosity

    NASA Astrophysics Data System (ADS)

    Bottinga, Y.; Richet, P.

    1995-07-01

    The decrease of the specific volume, when the extent of polymerization diminishes, is a cause of the pressure sensitivity of the viscosity of silicate melts. This effect can be explained by means of the Adam and Gibbs (1965) theory, taking into account the pressure dependence of the degree of polymerization of the melt and its influence on the configurational entropy. At temperatures close to their glass transitions, liquid silica and SiO2sbnd Na2O melts have configurational entropies that are probably due to the mixing of their bridging and nonbridging oxygen atoms.

  1. Magnetic field and pressure dependant resistivity behaviour of MnAs

    NASA Astrophysics Data System (ADS)

    Satya, A. T.; Amaladass, E. P.; Mani, Awadhesh

    2018-04-01

    The studies on the effect of magnetic field and external pressure on temperature dependant electrical resistivity behaviour of polycrystalline MnAs have been reported. At ambient pressure, ρ(T) shows a first order magnetic transition associated with change in sign of the temperature coefficient of resistivity from positive in the ferromagnetic (FM) phase to negative in the paramagnetic (PM) phase. The magneto resistance is negative and shows a peak at the FM transition temperature (T C ). The first order hysteresis width decreases with increase in magnetic field and the intersection of extrapolated linear variations of T C with field for the cooling and warming cycles enabled determination of the tricritical point. At high pressures, ρ(T) displays non monotonic variation exhibiting a low temperature minimum ({T}\\min L) and a high temperature maximum ({T}\\max H) accompanying broad thermal hysteresis above {T}\\min L. It is surmised that spin disorder scattering is responsible for the resistivity behaviour above {T}\\min L and the essential features of ρ(T) are qualitatively explained using Kasuya theoretical model. Below the {T}\\min L, ρ(T) follows linear logarithmic temperature dependence similar to the effect occurring due to Kondo type of scattering of conduction electrons with localised moments.

  2. The major influence of the atmosphere on intracranial pressure: an observational study

    NASA Astrophysics Data System (ADS)

    Herbowski, Leszek

    2017-01-01

    The impact of the atmosphere on human physiology has been studied widely within the last years. In practice, intracranial pressure is a pressure difference between intracranial compartments and the surrounding atmosphere. This means that gauge intracranial pressure uses atmospheric pressure as its zero point, and therefore, this method of pressure measurement excludes the effects of barometric pressure's fluctuation. The comparison of these two physical quantities can only take place through their absolute value relationship. The aim of this study is to investigate the direct effect of barometric pressure on the absolute intracranial pressure homeostasis. A prospective observational cross-sectional open study was conducted in Szczecin, Poland. In 28 neurosurgical patients with suspected normal-pressure hydrocephalus, intracranial intraventricular pressure was monitored in a sitting position. A total of 168 intracranial pressure and atmospheric pressure measurements were performed. Absolute atmospheric pressure was recorded directly. All values of intracranial gauge pressure were converted to absolute pressure (the sum of gauge intracranial pressure and local absolute atmospheric pressure). The average absolute mean intracranial pressure in the patients is 1006.6 hPa (95 % CI 1004.5 to 1008.8 hPa, SEM 1.1), and the mean absolute atmospheric pressure is 1007.9 hPa (95 % CI 1006.3 to 1009.6 hPa, SEM 0.8). The observed association between atmospheric and intracranial pressure is strongly significant (Spearman correlation r = 0.87, p < 0.05) and all the measurements are perfectly reliable (Bland-Altman coefficient is 4.8 %). It appears from this study that changes in absolute intracranial pressure are related to seasonal variation. Absolute intracranial pressure is shown to be impacted positively by atmospheric pressure.

  3. In Situ Observations of Thermoreversible Gelation and Phase Separation of Agarose and Methylcellulose Solutions under High Pressure.

    PubMed

    Kometani, Noritsugu; Tanabe, Masahiro; Su, Lei; Yang, Kun; Nishinari, Katsuyoshi

    2015-06-04

    Thermoreversible sol-gel transitions of agarose and methylcellulose (MC) aqueous solutions on isobaric cooling or heating under high pressure up to 400 MPa have been investigated by in situ observations of optical transmittance and falling-ball experiments. For agarose, which undergoes the gelation on cooling, the application of pressure caused a gradual rise in the cloud-point temperature over the whole pressure range examined, which is almost consistent with the pressure dependence of gelling temperature estimated by falling-ball experiments, suggesting that agarose gel is stabilized by compression and that the gelation occurs nearly in parallel with phase separation under ambient and high-pressure conditions. For MC, which undergoes the gelation on heating, the cloud-point temperature showed a slight rise with an initial elevation of pressure up to ∼150 MPa, whereas it showed a marked depression above 200 MPa. In contrast, the gelling temperature of MC, which is nearly identical to the cloud-point temperature at ambient pressure, showed a monotonous rise with increasing pressure up to 350 MPa, which means that MC undergoes phase separation prior to gelation on heating under high pressure above 200 MPa. Similar results were obtained for the melting process of MC gel on cooling. The unique behavior of the sol-gel transition of MC under high pressure has been interpreted in terms of the destruction of hydrophobic hydration by compression.

  4. Observation of pressure variation in the cavitation region of submerged journal bearings

    NASA Technical Reports Server (NTRS)

    Etsion, I.; Ludwig, L. P.

    1980-01-01

    Visual observations and pressure measurements in the cavitation zone of a submerged journal bearing are described. Tests were performed at various shaft speeds and ambient pressure levels. Some photographs of the cavitation region are presented showing strong reverse flow at the downstream end of the region. Pressure profiles are presented showing significant pressure variations inside the cavitation zone, contrary to common assumptions of constant cavitation pressure.

  5. Pressure Variations in Metamorphic Rocks: Implications for the Interpretation of Petrographic Observations

    NASA Astrophysics Data System (ADS)

    Tajčmanová, Lucie

    2014-05-01

    Metamorphic petrologists and structural geologists, using direct measurements, bring the only direct observational constrains for validating geodynamic models. Therefore, petrological and structural geological observations are essential for the quality and reproducibility of geodynamic reconstructions and models. One of the important assumptions for geodynamic reconstructions arises from the pressure and temperature estimates in the petrology analysis. Pressure is commonly converted to depth through the equation for lithostatic pressure and so the original position of the rock sample within the Earth's interior can be constrained. The current assumption that the studied sample corresponds to uniform pressure may not be correct, and if so, it has serious implications. Increasing evidence from analytical data shows that pressure is not constant even on a grain scale, posing new challenges because, if ignored, it leads to an incorrect use of petrology data in constraining geodynamic models. Well known examples of the preservation of coesite and diamond in a host mineral like garnet show that high pressure inclusions are preserved during decompression. Tajčmanová et al. (2014) has shown that grain-scale pressure variations can develop and that these pressure variations allow compositional zoning in minerals preserved over geological time scales. A new unconventional barometric method based on equilibrium under pressure variations has been developed . Such pressure variations are also connected with differences in fluid pressure in open systems and can be thus observed at all scales. Tajčmanová L., Podladchikov Y., Powell R., Moulas E., Vrijmoed J. and Connolly J. (2014). Grain scale pressure variations and chemical equilibrium in high-grade metamorphic rocks.Journal of Metamorphic Geology, doi:10.1111/jmg.12066 This work was supported by ERC starting grant 335577 to Lucie Tajcmanova

  6. Pressure-Dependent Photoluminescence Study of Wurtzite InP Nanowires.

    PubMed

    Chauvin, Nicolas; Mavel, Amaury; Patriarche, Gilles; Masenelli, Bruno; Gendry, Michel; Machon, Denis

    2016-05-11

    The elastic properties of InP nanowires are investigated by photoluminescence measurements under hydrostatic pressure at room temperature and experimentally deduced values of the linear pressure coefficients are obtained. The pressure-induced energy shift of the A and B transitions yields a linear pressure coefficient of αA = 88.2 ± 0.5 meV/GPa and αB = 89.3 ± 0.5 meV/GPa with a small sublinear term of βA = βB = -2.7 ± 0.2 meV/GPa(2). Effective hydrostatic deformation potentials of -6.12 ± 0.04 and -6.2 ± 0.04 eV are derived from the results for the A and B transitions, respectively. A decrease of the integrated intensity is observed above 0.5 GPa and is interpreted as a carrier transfer from the first to the second conduction band of the wurtzite InP.

  7. Driving force for indentation cracking in glass: composition, pressure and temperature dependence

    PubMed Central

    Rouxel, Tanguy

    2015-01-01

    The occurrence of damage at the surface of glass parts caused by sharp contact loading is a major issue for glass makers, suppliers and end-users. Yet, it is still a poorly understood problem from the viewpoints both of glass science and solid mechanics. Different microcracking patterns are observed at indentation sites depending on the glass composition and indentation cracks may form during both the loading and the unloading stages. Besides, we do not know much about the fracture toughness of glass and its composition dependence, so that setting a criterion for crack initiation and predicting the extent of the damage yet remain out of reach. In this study, by comparison of the behaviour of glasses from very different chemical systems and by identifying experimentally the individual contributions of the different rheological processes leading to the formation of the imprint—namely elasticity, densification and shear flow—we obtain a fairly straightforward prediction of the type and extent of the microcracks which will most likely form, depending on the physical properties of the glass. Finally, some guidelines to reduce the driving force for microcracking are proposed in the light of the effects of composition, temperature and pressure, and the areas for further research are briefly discussed. PMID:25713446

  8. The major influence of the atmosphere on intracranial pressure: an observational study.

    PubMed

    Herbowski, Leszek

    2017-01-01

    The impact of the atmosphere on human physiology has been studied widely within the last years. In practice, intracranial pressure is a pressure difference between intracranial compartments and the surrounding atmosphere. This means that gauge intracranial pressure uses atmospheric pressure as its zero point, and therefore, this method of pressure measurement excludes the effects of barometric pressure's fluctuation. The comparison of these two physical quantities can only take place through their absolute value relationship. The aim of this study is to investigate the direct effect of barometric pressure on the absolute intracranial pressure homeostasis. A prospective observational cross-sectional open study was conducted in Szczecin, Poland. In 28 neurosurgical patients with suspected normal-pressure hydrocephalus, intracranial intraventricular pressure was monitored in a sitting position. A total of 168 intracranial pressure and atmospheric pressure measurements were performed. Absolute atmospheric pressure was recorded directly. All values of intracranial gauge pressure were converted to absolute pressure (the sum of gauge intracranial pressure and local absolute atmospheric pressure). The average absolute mean intracranial pressure in the patients is 1006.6 hPa (95 % CI 1004.5 to 1008.8 hPa, SEM 1.1), and the mean absolute atmospheric pressure is 1007.9 hPa (95 % CI 1006.3 to 1009.6 hPa, SEM 0.8). The observed association between atmospheric and intracranial pressure is strongly significant (Spearman correlation r = 0.87, p < 0.05) and all the measurements are perfectly reliable (Bland-Altman coefficient is 4.8 %). It appears from this study that changes in absolute intracranial pressure are related to seasonal variation. Absolute intracranial pressure is shown to be impacted positively by atmospheric pressure.

  9. Observations of a high-pressure phase creation in oleic acid

    NASA Astrophysics Data System (ADS)

    Kościesza, R.; Kulisiewicz, L.; Delgado, A.

    2010-03-01

    Oleic acid is one of the unsaturated fatty acids which frequently appears in food products such as edible fats and oils. A molecule of oleic acid possesses a double carbon bond, C=C, which is responsible for a transition to a new phase when pressure is applied. This work presents the results of optical observations of such a transition. The observations were made in two cases, the first being static p-T conditions under 60 MPa at 20°C and the other the dynamic application of the pressure up to 350 MPa. The obtained visualization reveals differences in the creation of the phase and in its further appearance. Some crystal forms may be recognized. These results tend to be of interest for food engineers due to increasing interest in high-pressure food preservation among nutritionists and medical scientists concerned with fatty acids.

  10. Critical heat flux phenomena depending on pre-pressurization in transient heat input

    NASA Astrophysics Data System (ADS)

    Park, Jongdoc; Fukuda, Katsuya; Liu, Qiusheng

    2017-07-01

    The critical heat flux (CHF) levels that occurred due to exponential heat inputs for varying periods to a 1.0-mm diameter horizontal cylinder immersed in various liquids were measured to develop an extended database on the effect of various pressures and subcoolings by photographic study. Two main mechanisms of CHF were found. One mechanism is due to the time lag of the hydrodynamic instability (HI) which starts at steady-state CHF upon fully developed nucleate boiling, and the other mechanism is due to the explosive process of heterogeneous spontaneous nucleation (HSN) which occurs at a certain HSN superheat in originally flooded cavities on the cylinder surface. The incipience of boiling processes was completely different depending on pre-pressurization. Also, the dependence of pre-pressure in transient CHFs changed due to the wettability of boiling liquids. The objective of this work is to clarify the transient CHF phenomena due to HI or HSN by photographic.

  11. Vortex, ULF wave and Aurora Observation after Solar Wind Dynamic Pressure Change

    NASA Astrophysics Data System (ADS)

    Shi, Q.

    2017-12-01

    Here we will summarize our recent study and show some new results on the Magnetosphere and Ionosphere Response to Dynamic Pressure Change/disturbances in the Solar Wind and foreshock regions. We study the step function type solar wind dynamic pressure change (increase/decrease) interaction with the magnetosphere using THEMIS satellites at both dayside and nightside in different geocentric distances. Vortices generated by the dynamic pressure change passing along the magnetopause are found and compared with model predictions. ULF waves and vortices are excited in the dayside and nightside plasma sheet when dynamic pressure change hit the magnetotail. The related ionospheric responses, such as aurora and TCVs, are also investigated. We compare Global MHD simulations with the observations. We will also show some new results that dayside magnetospheric FLRs might be caused by foreshock structures.Shi, Q. Q. et al. (2013), THEMIS observations of ULF wave excitation in the nightside plasma sheet during sudden impulse events, J. Geophys. Res. Space Physics, 118, doi:10.1029/2012JA017984. Shi, Q. Q. et al. (2014), Solar wind pressure pulse-driven magnetospheric vortices and their global consequences, J. Geophys. Res. Space Physics, 119, doi:10.1002/2013JA019551. Tian, A.M. et al.(2016), Dayside magnetospheric and ionospheric responses to solar wind pressure increase: Multispacecraft and ground observations, J. Geophys. Res., 121, doi:10.1002/2016JA022459. Shen, X.C. et al.(2015), Magnetospheric ULF waves with increasing amplitude related to solar wind dynamic pressure changes: THEMIS observations, J. Geophys. Res., 120, doi:10.1002/2014JA020913Zhao, H. Y. et al. (2016), Magnetospheric vortices and their global effect after a solar wind dynamic pressure decrease, J. Geophys. Res. Space Physics, 121, doi:10.1002/2015JA021646. Shen, X. C., et al. (2017), Dayside magnetospheric ULF wave frequency modulated by a solar wind dynamic pressure negative impulse, J. Geophys. Res

  12. Electron kinetics dependence on gas pressure in laser-induced oxygen plasma experiment: Theoretical analysis

    NASA Astrophysics Data System (ADS)

    Gamal, Yosr E. E.-D.; Abdellatif, Galila

    2017-08-01

    A study is performed to investigate the dependency of threshold intensity on gas pressure observed in the measurements of the breakdown of molecular oxygen that carried out by Phuoc (2000) [1]. In this experiment, the breakdown was induced by 532 nm laser radiation of pulse width 5.5 ns and spot size of 8.5 μm, in oxygen over a wide pressure range (190-3000 Torr). The analysis aimed to explore the electron kinetic reliance on gas pressure for the separate contribution of each of the gain and loss processes encountered in this study. The investigation is based on an electron cascade model applied previously in Gamal and Omar (2001) [2] and Gaabour et al. (2013) [3]. This model solves numerically a differential equation designates the time evolution of the electron energy distribution, and a set of rate equations that describe the change of excited states population. The numerical examination of the electron energy distribution function and its parameters revealed that photo-ionization of the excited molecules plays a significant role in enhancing the electron density growth rate over the whole tested gas pressure range. This process is off set by diffusion of electrons out of the focal volume in the low-pressure regime. At atmospheric pressure electron, collisional processes dominate and act mainly to populate the excited states. Hence photo-ionization becomes efficient and compete with the encountered loss processes (electron diffusion, vibrational excitation of the ground state molecules as well as two body attachments). At high pressures ( 3000 Torr) three body attachments are found to be the primary cause of losses which deplete the electron density and hence results in the slow decrease of the threshold intensity.

  13. Application of reference-modified density functional theory: Temperature and pressure dependences of solvation free energy.

    PubMed

    Sumi, Tomonari; Maruyama, Yutaka; Mitsutake, Ayori; Mochizuki, Kenji; Koga, Kenichiro

    2018-02-05

    Recently, we proposed a reference-modified density functional theory (RMDFT) to calculate solvation free energy (SFE), in which a hard-sphere fluid was introduced as the reference system instead of an ideal molecular gas. Through the RMDFT, using an optimal diameter for the hard-sphere reference system, the values of the SFE calculated at room temperature and normal pressure were in good agreement with those for more than 500 small organic molecules in water as determined by experiments. In this study, we present an application of the RMDFT for calculating the temperature and pressure dependences of the SFE for solute molecules in water. We demonstrate that the RMDFT has high predictive ability for the temperature and pressure dependences of the SFE for small solute molecules in water when the optimal reference hard-sphere diameter determined for each thermodynamic condition is used. We also apply the RMDFT to investigate the temperature and pressure dependences of the thermodynamic stability of an artificial small protein, chignolin, and discuss the mechanism of high-temperature and high-pressure unfolding of the protein. © 2017 Wiley Periodicals, Inc. © 2017 Wiley Periodicals, Inc.

  14. Perils of Neglecting Lattice Relaxation in the Pressure Dependence of Deep Luminescence Bands in Wide Gap Semiconductors

    NASA Astrophysics Data System (ADS)

    Iota, V.; Weinstein, B. A.

    1998-03-01

    Deep defect states are often assumed to be insensitive to pressure because of their localized atomic-like character. In apparent conflict with this, experiments on widegap II-VI materials find that the pressure shifts of many 'midgap' photoluminescence (PL) bands associated with large-lattice-relaxation defects are more rapid than the shift of the bandgap(B. Weinstein, T. Ritter, et. al., Phys. Stat. Sol. (b) 198), 167 (1996). To study this, we measured the effects of pressure on the PL and PL-excitation (PLE) bands arising from the Zn-vacancy (V_Zn) and the P_Se deep acceptor centers in ZnSe. Using the observed pressure variation of the Stokes shifts and the established 1 atm. configuration coordinate (CC) models( D.Y. Jeon, H.P Gislason, G.D. Watkins, Phys. Rev. B 48), 7872 (1993), we were able to infer quantitative CC-diagrams at any pressure. Our results show that the pressure dependence of the lattice relaxation contributes a substantial fraction (several meV/kbar) to the overall shift of the PL-bands, and, hence, must be included. For the case of the V_Zn, simple calculations of the Jahn-Teller splitting using dangling-bond orbitals support this conclusion. figures

  15. Temperature- and pressure-dependent absorption cross sections of gaseous hydrocarbons at 3.39 µm

    NASA Astrophysics Data System (ADS)

    Klingbeil, A. E.; Jeffries, J. B.; Hanson, R. K.

    2006-07-01

    The pressure- and temperature-dependent absorption cross sections of several neat hydrocarbons and multi-component fuels are measured using a 3.39 µm helium-neon laser. Absorption cross section measurements are reported for methane, ethylene, propane, n-heptane, iso-octane, n-decane, n-dodecane, JP-10, gasoline and jet-A with an estimated uncertainty of less than 3.5%. The experimental conditions range from 298 to 673 K and from 500 to 2000 Torr with nitrogen as the bath gas. An apparatus is designed to facilitate these measurements, and specific care is taken to ensure the compositional accuracy of the hydrocarbon/N2 mixtures. The absorption cross sections of the smallest hydrocarbons, methane and ethylene, vary with temperature and pressure. The cross sections of larger hydrocarbons show negligible dependence on pressure and only a weak dependence on temperature. The reported data increase the range of conditions and the number of hydrocarbons for which cross section measurements are available at the HeNe laser wavelength.

  16. Pressure-dependent refractive indices of gases by THz time-domain spectroscopy.

    PubMed

    Sang, Bark Hyeon; Jeon, Tea-In

    2016-12-12

    Noncontact terahertz time-domain spectroscopy was employed to measure pressure-dependent refractive indices of gases such as helium (He), argon (Ar), krypton (Kr), oxygen (O2), nitrogen (N2), methane (CH4), and carbon dioxide (CO2). The refractive indices of these gases scaled linearly with pressure, for pressures in the 55-3,750 torr range. At the highest pressure, the refractive indices ((n-1) x 106) of He and CO2 were 170 and 2,390, respectively. The refractive index of CO2 was 14.1-fold higher than that of He, owing to the stronger polarizability of CO2. Although the studied gases differed in terms of their molecular structure, their refractive indices were strongly determined by polarizability. The measured refractive indices agreed well with the theoretical calculations.

  17. Dependence of the subharmonic signal from contrast agent microbubbles on ambient pressure: A theoretical analysis.

    PubMed

    Jiménez-Fernández, J

    2018-01-01

    This paper investigates the dependence of the subharmonic response in a signal scattered by contrast agent microbubbles on ambient pressure to provide quantitative estimations of local blood pressure. The problem is formulated by assuming a gas bubble encapsulated by a shell of finite thickness with dynamic behavior modeled by a nonlinear viscoelastic constitutive equation. For ambient overpressure compatible with the clinical range, the acoustic pressure intervals where the subharmonic signal may be detected (above the threshold for the onset and below the limit value for the first chaotic transition) are determined. The analysis shows that as the overpressure is increased, all harmonic components are displaced to higher frequencies. This displacement is significant for the subharmonic of order 1/2 and explains the increase or decrease in the subharmonic amplitude with ambient pressure described in previous works. Thus, some questions related to the monotonic dependence of the subharmonic amplitude on ambient pressure are clarified. For different acoustic pressures, quantitative conditions for determining the intervals where the subharmonic amplitude is a monotonic or non-monotonic function of the ambient pressure are provided. Finally, the influence of the ambient pressure on the subharmonic resonance frequency is analyzed.

  18. Pressure dependence of excited-state charge-carrier dynamics in organolead tribromide perovskites

    NASA Astrophysics Data System (ADS)

    Liu, X. C.; Han, J. H.; Zhao, H. F.; Yan, H. C.; Shi, Y.; Jin, M. X.; Liu, C. L.; Ding, D. J.

    2018-05-01

    Excited-state charge-carrier dynamics governs the performance of organometal trihalide perovskites (OTPs) and is strongly influenced by the crystal structure. Characterizing the excited-state charge-carrier dynamics in OTPs under high pressure is imperative for providing crucial insights into structure-property relations. Here, we conduct in situ high-pressure femtosecond transient absorption spectroscopy experiments to study the excited-state carrier dynamics of CH3NH3PbBr3 (MAPbBr3) under hydrostatic pressure. The results indicate that compression is an effective approach to modulate the carrier dynamics of MAPbBr3. Across each pressure-induced phase, carrier relaxation, phonon scattering, and Auger recombination present different pressure-dependent properties under compression. Responsiveness is attributed to the pressure-induced variation in the lattice structure, which also changes the electronic band structure. Specifically, simultaneous prolongation of carrier relaxation and Auger recombination is achieved in the ambient phase, which is very valuable for excess energy harvesting. Our discussion provides clues for optimizing the photovoltaic performance of OTPs.

  19. Pressure-dependent kinetics of initial reactions in iso-octane pyrolysis.

    PubMed

    Ning, HongBo; Gong, ChunMing; Li, ZeRong; Li, XiangYuan

    2015-05-07

    This study focuses on the studies of the main pressure-dependent reaction types of iso-octane (iso-C8H18) pyrolysis, including initial C-C bond fission of iso-octane, isomerization, and β-scission reactions of the alkyl radicals produced by the C-C bond fission of iso-octane. For the C-C bond fission of iso-octane, the minimum energy potentials are calculated at the CASPT2(2e,2o)/6-31+G(d,p)//CAS(2e,2o)/6-31+G(d,p) level of theory. For the isomerization and the β-scission reactions of the alkyl radicals, the optimization of the geometries and the vibrational frequencies of the reactants, transition states, and products are performed at the B3LYP/CBSB7 level, and their single point energies are calculated by using the composite CBS-QB3 method. Variable reaction coordinate transition state theory (VRC-TST) is used for the high-pressure limit rate constant calculation and Rice-Ramsperger-Kassel-Marcus/master equation (RRKM/ME) is used to calculate the pressure-dependent rate constants of these channels with pressure varying from 0.01-100 atm. The rate constants obtained in this work are in good agreement with those available from literatures. We have updated the rate constants and thermodynamic parameters for species involved in these reactions into a current chemical kinetic mechanism and also have improved the concentration profiles of main products such as C3H6 and C4H6 in the shock tube pyrolysis of iso-octane. The results of this study provide insight into the pyrolysis of iso-octane and will be helpful in the future development of branched paraffin kinetic mechanisms.

  20. Uniaxial strain orientation dependence of superconducting transition temperature (Tc) and critical superconducting pressure (Pc) in β-(BDA-TTP)2I3.

    PubMed

    Kikuchi, Koichi; Isono, Takayuki; Kojima, Masayuki; Yoshimoto, Haruo; Kodama, Takeshi; Fujita, Wataru; Yokogawa, Keiichi; Yoshino, Harukazu; Murata, Keizo; Kaihatsu, Takayuki; Akutsu, Hiroki; Yamada, Jun-ichi

    2011-12-14

    Dependence of the superconducting transition temperature (T(c)) and critial superconducting pressure (P(c)) of the pressure-induced superconductor β-(BDA-TTP)(2)I(3) [BDA-TTP = 2,5-bis(1,3-dithian-2-ylidene)-1,3,4,6-tetrathiapentalene] on the orientation of uniaxial strain has been investigated. On the basis of the overlap between the upper and lower bands in the energy dispersion curve, the pressure orientation is thought to change the half-filled band to the quarter-filled one. The observed variations in T(c) and P(c) are explained by considering the degree of application of the pressure and the degree of contribution of the effective electronic correlation at uniaxial strains with different orientations parallel to the conducting donor layer. © 2011 American Chemical Society

  1. Frequency, pressure and strain dependence of nonlinear elasticity in Berea Sandstone

    DOE PAGES

    Riviere, Jacques; Johnson, Paul Allan; Marone, Chris; ...

    2016-04-14

    Acoustoelasticity measurements in a sample of room dry Berea sandstone are conducted at various loading frequencies to explore the transition between the quasi-static ( f → 0) and dynamic (few kilohertz) nonlinear elastic response. We carry out these measurements at multiple confining pressures and perform a multivariate regression analysis to quantify the dependence of the harmonic content on strain amplitude, frequency, and pressure. The modulus softening (equivalent to the harmonic at 0f) increases by a factor 2–3 over 3 orders of magnitude increase in frequency. Harmonics at 2f, 4f, and 6f exhibit similar behaviors. In contrast, the harmonic at 1fmore » appears frequency independent. This result corroborates previous studies showing that the nonlinear elasticity of rocks can be described with a minimum of two physical mechanisms. This study provides quantitative data that describes the rate dependency of nonlinear elasticity. Furthermore, these findings can be used to improve theories relating the macroscopic elastic response to microstructural features.« less

  2. Density functional and theoretical study of the temperature and pressure dependency of the plasmon energy of solids

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

    Attarian Shandiz, M., E-mail: mohammad.attarianshandiz@mail.mcgill.ca; Gauvin, R.

    The temperature and pressure dependency of the volume plasmon energy of solids was investigated by density functional theory calculations. The volume change of crystal is the major factor responsible for the variation of valence electron density and plasmon energy in the free electron model. Hence, to introduce the effect of temperature and pressure for the density functional theory calculations of plasmon energy, the temperature and pressure dependency of lattice parameter was used. Also, by combination of the free electron model and the equation of state based on the pseudo-spinodal approach, the temperature and pressure dependency of the plasmon energy wasmore » modeled. The suggested model is in good agreement with the results of density functional theory calculations and available experimental data for elements with the free electron behavior.« less

  3. Tritiated Water on Molecular Sieve: Water Dynamics and Pressure Observations

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

    Walters, R.T.

    1999-04-23

    The production of fusion energy in a Tokamak using deuterium and tritium requires the safe handling and processing of exhaust gases that contain various amounts of tritium. Initial operation of the Tokamak Fusion Test Reactor (TFTR), Princeton Plasma Physics Laboratory, oxidized exhaust gases for tritium recovery or long-term storage. One of the most efficient and safest ways to contain tritiated water is to sorb it onto a pelletized 4A molecular sieve. A Disposable Molecular Sieve Bed (DMSB) was designed as a pressure vessel because of the possibility of pressure generation from the radiolysis of tritiated water on molecular sieve. Hydrogenmore » production contributes to the complexity of the containers used to transport and store tritiated water, and increases the fabrication costs. Two months after removing a DMSB from the process at TFTR, a pressure in excess of that predicted from self-radiolysis was observed. Interestingly, pressure measurements at longer times (up to 2.5 years) showed less pressure than expected. Pressure was not being generated in the DMSBs at the predicted rate. This was unexpected and prompted an investigation into the mechanism responsible for the anomalous pressure measurements.« less

  4. Temperature and Pressure Dependences of the Elastic Properties of Tantalum Single Crystals Under <100> Tensile Loading: A Molecular Dynamics Study

    NASA Astrophysics Data System (ADS)

    Li, Wei-bing; Li, Kang; Fan, Kan-qi; Zhang, Da-xing; Wang, Wei-dong

    2018-04-01

    Atomistic simulations are capable of providing insights into physical mechanisms responsible for mechanical properties of the transition metal of Tantalum (Ta). By using molecular dynamics (MD) method, temperature and pressure dependences of the elastic properties of Ta single crystals are investigated through <100> tensile loading. First of all, a comparative study between two types of embedded-atom method (EAM) potentials is made in term of the elastic properties of Ta single crystals. The results show that Ravelo-EAM (Physical Review B, 2013, 88: 134101) potential behaves well at different hydrostatic pressures. Then, the MD simulation results based on the Ravelo-EAM potential show that Ta will experience a body-centered-cubic (BCC) to face-centered-cubic (FCC) phase transition before fracture under <100> tensile loading at 1 K temperature, and model size and strain rate have no obvious effects on tensile behaviors of Ta. Next, from the simulation results at the system temperature from 1 to 1500 K, it can be derived that the elastic modulus of E 100 linearly decrease with the increasing temperature, while the yielding stress decrease with conforming a quadratic polynomial formula. Finally, the pressure dependence of the elastic properties is performed from 0 to 140 GPa and the observations show that the elastic modulus increases with the increasing pressure overall.

  5. Pressure-dependence of the phase transitions and thermal expansion in zirconium and hafnium pyrovanadate

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

    Gallington, Leighanne C.; Hester, Brett R.; Kaplan, Benjamin S.

    Low or negative thermal expansion (NTE) has been previously observed in members of the ZrP 2O 7 family at temperatures higher than their order-disorder phase transitions. The thermoelastic properties and phase behavior of the low temperature superstructure and high temperature negative thermal expansion phases of ZrV 2O 7 and HfV 2O 7 were explored via in situ variable temperature/pressure powder x-ray diffraction measurements. The phase transition temperatures of ZrV 2O 7 and HfV 2O 7 exhibited a very strong dependence on pressure (~700 K GPa), with moderate compression suppressing the formation of their NTE phases below 513 K. Compression alsomore » reduced the magnitude of the coefficients of thermal expansion in both the positive and negative thermal expansion phases. Additionally, the high temperature NTE phase of ZrV 2O 7 was found to be twice as stiff as the low temperature positive thermal expansion superstructure (24 and 12 GPa respectively).« less

  6. Experimental evidence regarding the pressure dependence of fission track annealing in apatite

    NASA Astrophysics Data System (ADS)

    Schmidt, J. S.; Lelarge, M. L. M. V.; Conceicao, R. V.; Balzaretti, N. M.

    2014-03-01

    The main purposes of fission track thermochronology are unravelling the thermal histories of sedimentary basins, determining uplift and denudation rates, identifying the structural evolution of orogenic belts, determining sedimentary provenance, and dating volcanic rocks. The effect of temperature on fission tracks is well known and is used to determine the thermal history; however, the effect of pressure on the stability of tracks is still under debate. The present work aims to understand the role of pressure on the annealing kinetics of apatite fission tracks. The samples of Durango apatite used in our experiments were chosen for their international recognition as a calibration standard for geological dating. Neutron irradiation of the samples, after total annealing of their spontaneous tracks, produced induced tracks with homogeneous densities and lengths. The effect of pressure associated with temperature on fission track annealing was verified by experimental procedures using a hydraulic press of 1000 t with a toroidal chamber profile. The experiments consisted of a combination of applying 2 and 4 GPa with 20,150,190,235, and 290 °C for 1 and 10 h. The annealing rate was analysed by measuring the lengths of the fission tracks after each experiment using optical microscopy. The results demonstrate that the annealing of apatite fission tracks has a pressure dependence for samples subjected to 2 and 4 GPa. However, when extrapolated to pressures of ⩽150 MPa, compatible with the normal geological context in which apatite fission track methodology is broadly used, this dependence becomes insignificant compared to the temperature effect.

  7. Does the accuracy of blood pressure measurement correlate with hearing loss of the observer?

    PubMed

    Song, Soohwa; Lee, Jongshill; Chee, Youngjoon; Jang, Dong Pyo; Kim, In Young

    2014-02-01

    The auscultatory method is influenced by the hearing level of the observers. If the observer has hearing loss, it is possible to measure blood pressure inaccurately by misreading the Korotkoff sounds at systolic blood pressure (SBP) and diastolic blood pressure (DBP). Because of the potential clinical problems this discrepancy may cause, we used a hearing loss simulator to determine how hearing level affects the accuracy of blood pressure measurements. Two data sets (data set A, 32 Korotkoff sound video clips recorded by the British Hypertension Society; data set B, 28 Korotkoff sound data acquired from the Korotkoff sound recording system developed by Hanyang University) were used and all the data were attenuated to simulate a hearing loss of 5, 10, 15, 20, and 25 dB using the hearing loss simulator. Five observers with normal hearing assessed the blood pressures from these data sets and the differences between the values measured from the original recordings (no attenuation) and the attenuated versions were analyzed. Greater attenuation of the Korotkoff sounds, or greater hearing loss, resulted in larger blood pressure measurement differences when compared with the original data. When measuring blood pressure with hearing loss, the SBP tended to be underestimated and the DBP was overestimated. The mean differences between the original data and the 25 dB hearing loss data for the two data sets combined were 1.55±2.71 and -4.32±4.21 mmHg for SBP and DBP, respectively. This experiment showed that the accuracy of blood pressure measurements using the auscultatory method is affected by observer hearing level. Therefore, to reduce possible error using the auscultatory method, observers' hearing should be tested.

  8. Concentration dependent refractive index of a binary mixture at high pressure.

    PubMed

    Croccolo, Fabrizio; Arnaud, Marc-Alexandre; Bégué, Didier; Bataller, Henri

    2011-07-21

    In the present work binary mixtures of varying concentrations of two miscible hydrocarbons, 1,2,3,4-tetrahydronaphtalene (THN) and n-dodecane (C12), are subjected to increasing pressure up to 50 MPa in order to investigate the dependence of the so-called concentration contrast factor (CF), i.e., (∂n/∂c)(p, T), on pressure level. The refractive index is measured by means of a Mach-Zehnder interferometer. The setup and experimental procedure are validated with different pure fluids in the same pressure range. The refractive index of the THN-C12 mixture is found to vary both over pressure and concentration, and the concentration CF is found to exponentially decrease as the pressure is increased. The measured values of the refractive index and the concentration CFs are compared with values obtained by two different theoretical predictions, the well-known Lorentz-Lorenz formula and an alternative one proposed by Looyenga. While the measured refractive indices agree very well with predictions given by Looyenga, the measured concentration CFs show deviations from the latter of the order of 6% and more than the double from the Lorentz-Lorenz predictions.

  9. Pressure Dependence of the Charge-Density-Wave Gap in Rare-Earth Tri-Tellurides

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

    Sacchetti, A.; /Zurich, ETH; Arcangeletti, E.

    2009-12-14

    We investigate the pressure dependence of the optical properties of CeTe{sub 3}, which exhibits an incommensurate charge-density-wave (CDW) state already at 300 K. Our data are collected in the mid-infrared spectral range at room temperature and at pressures between 0 and 9 GPa. The energy for the single particle excitation across the CDW gap decreases upon increasing the applied pressure, similarly to the chemical pressure by rare-earth substitution. The broadening of the bands upon lattice compression removes the perfect nesting condition of the Fermi surface and therefore diminishes the impact of the CDW transition on the electronic properties of RTe{submore » 3}.« less

  10. ENERGETIC PARTICLE PRESSURE AT INTERPLANETARY SHOCKS: STEREO-A OBSERVATIONS

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

    Lario, D.; Decker, R. B.; Roelof, E. C.

    2015-11-10

    We study periods of elevated energetic particle intensities observed by STEREO-A when the partial pressure exerted by energetic (≥83 keV) protons (P{sub EP}) is larger than the pressure exerted by the interplanetary magnetic field (P{sub B}). In the majority of cases, these periods are associated with the passage of interplanetary shocks. Periods when P{sub EP} exceeds P{sub B} by more than one order of magnitude are observed in the upstream region of fast interplanetary shocks where depressed magnetic field regions coincide with increases of energetic particle intensities. When solar wind parameters are available, P{sub EP} also exceeds the pressure exertedmore » by the solar wind thermal population (P{sub TH}). Prolonged periods (>12 hr) with both P{sub EP} > P{sub B} and P{sub EP} > P{sub TH} may also occur when energetic particles accelerated by an approaching shock encounter a region well upstream of the shock characterized by low magnetic field magnitude and tenuous solar wind density. Quasi-exponential increases of the sum P{sub SUM} = P{sub B} + P{sub TH} + P{sub EP} are observed in the immediate upstream region of the shocks regardless of individual changes in P{sub EP}, P{sub B}, and P{sub TH}, indicating a coupling between P{sub EP} and the pressure of the background medium characterized by P{sub B} and P{sub TH}. The quasi-exponential increase of P{sub SUM} implies a radial gradient ∂P{sub SUM}/∂r > 0 that is quasi-stationary in the shock frame and results in an outward force applied to the plasma upstream of the shock. This force can be maintained by the mobile energetic particles streaming upstream of the shocks that, in the most intense events, drive electric currents able to generate diamagnetic cavities and depressed solar wind density regions.« less

  11. Pressure dependence of the magnetic order in CrAs: a neutron diffraction investigation

    DOE PAGES

    Keller, L.; White, J. S.; Babkevich, P.; ...

    2015-01-29

    The suppression of magnetic order with pressure concomitant with the appearance of pressure-induced superconductivity was recently discovered in CrAs. Here we present a neutron diffraction study of the pressure evolution of the helimagnetic ground-state towards and in the vicinity of the superconducting phase. Neutron diffraction on polycrystalline CrAs was employed from zero pressure to 0.65 GPa and at various temperatures. The helimagnetic long-range order is sustained under pressure and the magnetic propagation vector does not show any considerable change. The average ordered magnetic moment is reduced from 1.73(2) μ B at ambient pressure to 0.4(1) μ B close to themore » critical pressure P c ≈ 0.7 GPa, at which magnetic order is completely suppressed. The width of the magnetic Bragg peaks strongly depends on temperature and pressure, showing a maximum in the region of the onset of superconductivity. In conclusion, we interpret this as associated with competing ground-states in the vicinity of the superconducting phase.« less

  12. Pressure dependence of the magnetic order in CrAs: a neutron diffraction investigation

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

    Keller, L.; White, J. S.; Babkevich, P.

    The suppression of magnetic order with pressure concomitant with the appearance of pressure-induced superconductivity was recently discovered in CrAs. Here we present a neutron diffraction study of the pressure evolution of the helimagnetic ground-state towards and in the vicinity of the superconducting phase. Neutron diffraction on polycrystalline CrAs was employed from zero pressure to 0.65 GPa and at various temperatures. The helimagnetic long-range order is sustained under pressure and the magnetic propagation vector does not show any considerable change. The average ordered magnetic moment is reduced from 1.73(2) μ B at ambient pressure to 0.4(1) μ B close to themore » critical pressure P c ≈ 0.7 GPa, at which magnetic order is completely suppressed. The width of the magnetic Bragg peaks strongly depends on temperature and pressure, showing a maximum in the region of the onset of superconductivity. In conclusion, we interpret this as associated with competing ground-states in the vicinity of the superconducting phase.« less

  13. Ocean Wave-to-Ice Energy Transfer Determined from Seafloor Pressure and Ice Shelf Seismic Observations

    NASA Astrophysics Data System (ADS)

    Chen, Z.; Bromirski, P. D.; Gerstoft, P.; Stephen, R. A.; Wiens, D.; Aster, R. C.; Nyblade, A.

    2017-12-01

    Ice shelves play an important role in buttressing land ice from reaching the sea, thus restraining the rate of sea level rise. Long-period gravity wave impacts excite vibrations in ice shelves that may trigger tabular iceberg calving and/or ice shelf collapse events. Three kinds of seismic plate waves were continuously observed by broadband seismic arrays on the Ross Ice Shelf (RIS) and on the Pine Island Glacier (PIG) ice shelf: (1) flexural-gravity waves, (2) flexural waves, and (3) extensional Lamb waves, suggesting that all West Antarctic ice shelves are subjected to similar gravity wave excitation. Ocean gravity wave heights were estimated from pressure perturbations recorded by an ocean bottom differential pressure gauge at the RIS front, water depth 741 m, about 8 km north of an on-ice seismic station that is 2 km from the shelf front. Combining the plate wave spectrum, the frequency-dependent energy transmission and reflection at the ice-water interface were determined. In addition, Young's modulus and Poisson's ratio of the RIS are estimated from the plate wave motions, and compared with the widely used values. Quantifying these ice shelf parameters from observations will improve modeling of ice shelf response to ocean forcing, and ice shelf evolution.

  14. [Sulphureous mud-bath therapy and changes in blood pressure: observational investigation].

    PubMed

    Costantino, M; Marongiu, M B; Russomanno, G; Conti, V; Manzo, V; Filippelli, A

    2015-01-01

    The chronic arthropathies currently appear to be a major cause of disability with a negative impact on quality of life and health care spending. The mud-bath therapy is a spa treatment that induces benefic effects in chronic rheumatic diseases. It has long been debated on the assumption that the mud-bath spa therapy could have adverse cardiovascular effects which often induce caution and even a contraindication to the use of this treatment in chronic arthropathies associated with cardiovascular alterations such as hypertension. The aim of this observational study was to investigate, in arthrorheumatic subjects, the effects of sulphureous mud-bath cycle on blood pressure and the possible appearance of adverse drug reaction. 169 patients, with age range 42-86 years, suffering by chronic arthropathies were treated with sulphureous mud-bath therapy for 2 weeks. According to the arterial pressure values, measured before the spa treatment, the patients considered were divided in three groups: with normal blood pressure (NOR group); with high blood pressure, after, the latter group was divided in IPET (patients in treatment with antihypertensive drugs) and IPENT (patients not in antihypertensive therapy). The arterial pressure values, maximum and minimum, expressed in mmHg, were detected in the first (T1) - sixth (T6) and twelfth (T12) day of spa treatment. The media arterial pressure values collected before and after T1, before and after T6, before and after T12 , before T1 and after T12 were compared. The data, presented as mean±SD, were compared with the paired Student t test. A p value ≤0.05 was considered significant. The comparison between the mean values detected in pre and post T1, pre and post T6, pre and post T12 have showed that sulphureous mud-bath therapy induced a significant (p<0.05) reduction of arterial blood pressure values in patients suffering of chronic arthropathies with high blood pressure in antihypertensive therapy or not (IPET and IPENT groups

  15. Mode I Fracture Toughness of Rock - Intrinsic Property or Pressure-Dependent?

    NASA Astrophysics Data System (ADS)

    Stoeckhert, F.; Brenne, S.; Molenda, M.; Alber, M.

    2016-12-01

    The mode I fracture toughness of rock is usually regarded as an intrinsic material parameter independent of pressure. However, most fracture toughness laboratory tests are conducted only at ambient pressure. To investigate fracture toughness of rock under elevated pressures, sleeve fracturing laboratory experiments were conducted with various rock types and a new numerical method was developed for the evaluation of these experiments. The sleeve fracturing experiments involve rock cores with central axial boreholes that are placed in a Hoek triaxial pressure cell to apply an isostatic confining pressure. A polymere tube is pressurized inside these hollow rock cylinders until they fail by tensile fracturing. Numerical simulations incorporating fracture mechanical models are used to obtain a relation between tensile fracture propagation and injection pressure. These simulations indicate that the magnitude of the injection pressure at specimen failure is only depending on the fracture toughness of the tested material, the specimen dimensions and the magnitude of external loading. The latter two are known parameters in the experiments. Thus, the fracture toughness can be calculated from the injection pressure recorded at specimen breakdown. All specimens had a borehole diameter to outer diameter ratio of about 1:10 with outer diameters of 40 and 62 mm. The length of the specimens was about two times the diameter. Maximum external loading was 7.5 MPa corresponding to maximum injection pressures at specimen breakdown of about 100 MPa. The sample set tested in this work includes Permian and Carboniferous sandstones, Jurassic limestones, Triassic marble, Permian volcanic rocks and Devonian slate from Central Europe. The fracture toughness values determined from the sleeve fracturing experiments without confinement using the new numerical method were found to be in good agreement with those from Chevron bend testing according to the ISRM suggested methods. At elevated

  16. Observation of pressure variation in the cavitation region of submerged journal bearings

    NASA Technical Reports Server (NTRS)

    Etsion, I.; Ludwig, L. P.

    1981-01-01

    Visual observations and pressure measurements in the cavitation zone of a submerged journal bearing are described. Tests are run at speeds of 1840 and 3000 rpm, and at each speed, four different levels of the ambient supply pressure are applied, ranging from 13.6 KPa to 54.4 KPa. A strong reverse flow is detected inside the cavitation area adjacent to its downstream end, and significant pressure variations on the order of 50 KPa are found inside the cavitation region at the downstream portion of its circumferential extent. Results indicate that the assumption of a constant cavitation pressure is incorrect in the case of enclosed cavitations, and it is postulated that oil which is saturated with air under atmospheric pressure becomes oversaturated in the subcavity pressure loop.

  17. Electron mass in dilute nitrides and its anomalous dependence on hydrostatic pressure.

    PubMed

    Pettinari, G; Polimeni, A; Masia, F; Trotta, R; Felici, M; Capizzi, M; Niebling, T; Stolz, W; Klar, P J

    2007-04-06

    The dependence of the electron mass on hydrostatic pressure P in N-diluted GaAs1-xNx (x=0.10% and 0.21%) is investigated by magnetophotoluminescence. Exceedingly large fluctuations (up to 60%/kbar) in the electron mass with increasing P are found. These originate from a pressure-driven tuning of the hybridization degree between the conduction band minimum and specific nitrogen-related states. Present results suggest a hierarchy between different nitrogen complexes as regards the extent of the perturbation these complexes exert on the electronic properties of the GaAs host.

  18. Adiabatic pressure dependence of the 2.7 and 1.9 micron water vapor bands

    NASA Technical Reports Server (NTRS)

    Mathai, C. V.; Walls, W. L.; Broersma, S.

    1977-01-01

    An acoustic excitation technique is used to determine the adiabatic pressure derivative of the spectral absorptance of the 2.7 and 1.9 micron water vapor bands, and the 3.5 micron HCl band. The dependence of this derivative on thermodynamic parameters such as temperature, concentration, and pressure is evaluated. A cross-flow water vapor system is used to measure spectral absorptance. Taking F as the ratio of nonrigid to rotor line strengths, it is found that an F factor correction is needed for the 2.7 micron band. The F factor for the 1.9 micron band is also determined. In the wings of each band a wavelength can be found where the concentration dependence is predominant. Farther out in the wings a local maximum occurs for the temperature derivative. It is suggested that the pressure derivative is significant in the core of the band.

  19. Temperature and Pressure Dependences of the Elastic Properties of Tantalum Single Crystals Under <100> Tensile Loading: A Molecular Dynamics Study.

    PubMed

    Li, Wei-Bing; Li, Kang; Fan, Kang-Qi; Zhang, Da-Xing; Wang, Wei-Dong

    2018-04-24

    Atomistic simulations are capable of providing insights into physical mechanisms responsible for mechanical properties of the transition metal of Tantalum (Ta). By using molecular dynamics (MD) method, temperature and pressure dependences of the elastic properties of Ta single crystals are investigated through <100> tensile loading. First of all, a comparative study between two types of embedded-atom method (EAM) potentials is made in term of the elastic properties of Ta single crystals. The results show that Ravelo-EAM (Physical Review B, 2013, 88: 134101) potential behaves well at different hydrostatic pressures. Then, the MD simulation results based on the Ravelo-EAM potential show that Ta will experience a body-centered-cubic (BCC) to face-centered-cubic (FCC) phase transition before fracture under <100> tensile loading at 1 K temperature, and model size and strain rate have no obvious effects on tensile behaviors of Ta. Next, from the simulation results at the system temperature from 1 to 1500 K, it can be derived that the elastic modulus of E 100 linearly decrease with the increasing temperature, while the yielding stress decrease with conforming a quadratic polynomial formula. Finally, the pressure dependence of the elastic properties is performed from 0 to 140 GPa and the observations show that the elastic modulus increases with the increasing pressure overall.

  20. Exponential Boundary Observers for Pressurized Water Pipe

    NASA Astrophysics Data System (ADS)

    Hermine Som, Idellette Judith; Cocquempot, Vincent; Aitouche, Abdel

    2015-11-01

    This paper deals with state estimation on a pressurized water pipe modeled by nonlinear coupled distributed hyperbolic equations for non-conservative laws with three known boundary measures. Our objective is to estimate the fourth boundary variable, which will be useful for leakage detection. Two approaches are studied. Firstly, the distributed hyperbolic equations are discretized through a finite-difference scheme. By using the Lipschitz property of the nonlinear term and a Lyapunov function, the exponential stability of the estimation error is proven by solving Linear Matrix Inequalities (LMIs). Secondly, the distributed hyperbolic system is preserved for state estimation. After state transformations, a Luenberger-like PDE boundary observer based on backstepping mathematical tools is proposed. An exponential Lyapunov function is used to prove the stability of the resulted estimation error. The performance of the two observers are shown on a water pipe prototype simulated example.

  1. Irreversible particle motion in surfactant-laden interfaces due to pressure-dependent surface viscosity

    NASA Astrophysics Data System (ADS)

    Manikantan, Harishankar; Squires, Todd M.

    2017-09-01

    The surface shear viscosity of an insoluble surfactant monolayer often depends strongly on its surface pressure. Here, we show that a particle moving within a bounded monolayer breaks the kinematic reversibility of low-Reynolds-number flows. The Lorentz reciprocal theorem allows such irreversibilities to be computed without solving the full nonlinear equations, giving the leading-order contribution of surface pressure-dependent surface viscosity. In particular, we show that a disc translating or rotating near an interfacial boundary experiences a force in the direction perpendicular to that boundary. In unbounded monolayers, coupled modes of motion can also lead to non-intuitive trajectories, which we illustrate using an interfacial analogue of the Magnus effect. This perturbative approach can be extended to more complex geometries, and to two-dimensional suspensions more generally.

  2. Observer-dependent sign inversions of polarization singularities.

    PubMed

    Freund, Isaac

    2014-10-15

    We describe observer-dependent sign inversions of the topological charges of vector field polarization singularities: C points (points of circular polarization), L points (points of linear polarization), and two virtually unknown singularities we call γ(C) and α(L) points. In all cases, the sign of the charge seen by an observer can change as she changes the direction from which she views the singularity. Analytic formulas are given for all C and all L point sign inversions.

  3. Raw Pressure Data from Observation Wells at Brady's Hot Springs

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

    David Lim

    This .csv files contain the raw water pressure data from three observation wells during pumping tests performed in the Spring of 2016. Included is a "read me" file explaining the details of where and how the data were collected.

  4. Social pressure-induced craving in patients with alcohol dependence: application of virtual reality to coping skill training.

    PubMed

    Lee, Jung Suk; Namkoong, Kee; Ku, Jeonghun; Cho, Sangwoo; Park, Ji Yeon; Choi, You Kyong; Kim, Jae-Jin; Kim, In Young; Kim, Sun I; Jung, Young-Chul

    2008-12-01

    This study was conducted to assess the interaction between alcohol cues and social pressure in the induction of alcohol craving. Fourteen male patients with alcohol dependence and 14 age-matched social drinkers completed a virtual reality coping skill training program composed of four blocks according to the presence of alcohol cues (x2) and social pressure (x2). Before and after each block, the craving levels were measured using a visual analogue scale. Patients with alcohol dependence reported extremely high levels of craving immediately upon exposure to a virtual environment with alcohol cues, regardless of social pressure. In contrast, the craving levels of social drinkers were influenced by social pressure from virtual avatars. Our findings imply that an alcohol cue-laden environment should interfere with the ability to use coping skills against social pressure in real-life situations.

  5. Pronounced low-frequency vibrational thermal transport in C60 fullerite realized through pressure-dependent molecular dynamics simulations

    NASA Astrophysics Data System (ADS)

    Giri, Ashutosh; Hopkins, Patrick E.

    2017-12-01

    Fullerene condensed-matter solids can possess thermal conductivities below their minimum glassy limit while theorized to be stiffer than diamond when crystallized under pressure. These seemingly disparate extremes in thermal and mechanical properties raise questions into the pressure dependence on the thermal conductivity of C60 fullerite crystals, and how the spectral contributions to vibrational thermal conductivity changes under applied pressure. To answer these questions, we investigate the effect of strain on the thermal conductivity of C60 fullerite crystals via pressure-dependent molecular dynamics simulations under the Green-Kubo formalism. We show that the thermal conductivity increases rapidly with compressive strain, which demonstrates a power-law relationship similar to their stress-strain relationship for the C60 crystals. Calculations of the density of states for the crystals under compressive strains reveal that the librational modes characteristic in the unstrained case are diminished due to densification of the molecular crystal. Over a large compression range (0-20 GPa), the Leibfried-Schlömann equation is shown to adequately describe the pressure dependence of thermal conductivity, suggesting that low-frequency intermolecular vibrations dictate heat flow in the C60 crystals. A spectral decomposition of the thermal conductivity supports this hypothesis.

  6. Proton dependence of tobacco mosaic virus dissociation by pressure.

    PubMed

    Santos, Jose L R; Bispo, Jose A C; Landini, Gustavo F; Bonafe, Carlos F S

    2004-09-01

    Tobacco mosaic virus (TMV) is an intensely studied model of viruses. This paper reports an investigation into the dissociation of TMV by pH and pressure up to 220 MPa. The viral solution (0.25 mg/ml) incubated at 277 K showed a significant decrease in light scattering with increasing pH, suggesting dissociation. This observation was confirmed by HPLC gel filtration and electron microscopy. The calculated volume change of dissociation (DeltaV) decreased (absolute value) from -49.7 ml/mol of subunit at pH 3.8 to -21.7 ml/mol of subunit at pH 9.0. The decrease from pH 9.0 to 3.8 caused a stabilization of 14.1 kJ/mol of TMV subunit. The estimated proton release calculated from pressure-induced dissociation curves was 0.584 mol H(+)/mol of TMV subunit. These results suggest that the degree of virus inactivation by pressure and the immunogenicity of the inactivated structures can be optimized by modulating the surrounding pH.

  7. The pressure-induced, lactose-dependent changes in the composition and size of casein micelles.

    PubMed

    Wang, Pengjie; Jin, Shaoming; Guo, Huiyuan; Zhao, Liang; Ren, Fazheng

    2015-04-15

    The effects of lactose on the changes in the composition and size of casein micelles induced by high-pressure treatment and the related mechanism of action were investigated. Dispersions of ultracentrifuged casein micelle pellets with 0-10% (w/v) lactose were subjected to high pressure (400 MPa) at 20 °C for 40 min. The results indicated that the level of non-sedimentable caseins was positively related to the amount of lactose added prior to pressure treatment, and negatively correlated to the size. A mechanism for the pressure-induced, lactose-dependent changes in the casein micelles is proposed. Lactose inhibits the hydrophobic interactions between the micellar fragments during or after pressure release, through the hydrophilic layer formed by their hydrogen bonds around the micellar fragments. In addition, lactose does not favour the association between calcium and the casein aggregates after pressure release. Due to these two functions, lactose inhibited the formation of larger micelles after pressure treatment. Copyright © 2014 Elsevier Ltd. All rights reserved.

  8. Pressure-Dependent Yields and Product Branching Ratios in the Broadband Photolysis of Chlorine Nitrate

    NASA Technical Reports Server (NTRS)

    Nickolaisen, Scott L.; Sander, Stanley P.; Friedl, Randall R.

    1996-01-01

    The photolysis of chlorine nitrate was studied using broadband flash photolysis coupled with long-path ultraviolet-visible absorption spectroscopy. Branching ratios for the Cl + NO3 and ClO + NO2 product channels were determined from time-dependent measurements of ClO and NO3 concentrations. Yields of the ClO and NO3 products displayed a dependence on the bath gas density and the spectral distribution of the photolysis pulse. Product yields decreased with increasing bath gas density regardless of the spectral distribution of the photolysis pulse; however, the decrease in product yield was much more pronounced when photolysis was limited to longer wavelengths. For photolysis in a quartz cell (lambda > 200 nm) the yield decreased by a factor of 2 over the pressure 10-100 Torr. In a Pyrex cell (lambda > 300 nm), the yield decreased by a factor of 50 over the same pressure range. When photolysis was limited to lambda > 350 nm, the yield decreased by a factor of 250. Branching ratios for the photolysis channels [ClONO2 + h.nu yields ClO + NO2 (1a) and ClONO2 + h.nu yields Cl + NO3 (lb)] were determined from the relative ClO and NO3 product yields at various pressures. Although the absolute product yield displayed a pressure dependence, the branching between the two channels was independent of pressure. The relative branching ratios (assuming negligible contributions from other channels) are 0.61 +/- 0.20 for channel 1a and 0.39 +/- 0.20 for channel lb for photolysis with lambda > 200 nm and 0.44 +/- 0.08 for channel 1a and 0.56 +/- 0.08 for channel 1b for photolysis with lambda > 300 nm. The implications of these results for the chemistry of the lower stratosphere are discussed.

  9. New observations on the pressure dependence of luminescence from Eu2+-doped MF2 (M = Ca, Sr, Ba) fluorides.

    PubMed

    Su, Fu Hai; Chen, Wei; Ding, Kun; Li, Guo Hua

    2008-05-29

    The luminescence from Eu(2+) ions in MF2 (M = Ca, Sr, Ba) fluorides has been investigated under the pressure range of 0-8 GPa. The emission band originating from the 4f(6)5d(1) --> 4f(7) transition of Eu(2+) ions in CaF2 and SrF2 shows the red-shift as increasing pressure with pressure coefficients of -17 meV/GPa for CaF2 and -18 meV/GPa for SrF2. At atmospheric pressure, the emission spectrum of BaF2:Eu(2+) comprises two peaks at 2.20 and 2.75 eV from the impurity trapped exciton (ITE) and the self-trapped exciton (STE), respectively. As the pressure is increased, both emission peaks shift to higher energies, and the shifting rate is slowed by the phase transition from the cubic to orthorhombic phase at 4 GPa. Due to the phase transition at 4-5 GPa pressure, the ITE emission disappears gradually, and the STE emission is gradually replaced by the 4f(6)5d(1) --> 4f(7) transition of Eu(2+). Above 5 GPa, the pressure behavior of the 4f(6)5d(1) --> 4f(7) transition of Eu(2+) in BaF2:Eu(2+) is the same as the normal emission of Eu(2+) in CaF2 and SrF2 phosphors.

  10. Baseline pressure errors (BPEs) extensively influence intracranial pressure scores: results of a prospective observational study

    PubMed Central

    2014-01-01

    Background Monitoring of intracranial pressure (ICP) is a cornerstone in the surveillance of neurosurgical patients. The ICP is measured against a baseline pressure (i.e. zero - or reference pressure). We have previously reported that baseline pressure errors (BPEs), manifested as spontaneous shift or drifts in baseline pressure, cause erroneous readings of mean ICP in individual patients. The objective of this study was to monitor the frequency and severity of BPEs. To this end, we performed a prospective, observational study monitoring the ICP from two separate ICP sensors (Sensors 1 and 2) placed in close proximity in the brain. We characterized BPEs as differences in mean ICP despite near to identical ICP waveform in Sensors 1 and 2. Methods The study enrolled patients with aneurysmal subarachnoid hemorrhage in need of continuous ICP monitoring as part of their intensive care management. The two sensors were placed close to each other in the brain parenchyma via the same burr hole. The monitoring was performed as long as needed from a clinical perspective and the ICP recordings were stored digitally for analysis. For every patient the mean ICP as well as the various ICP wave parameters of the two sensors were compared. Results Sixteen patients were monitored median 164 hours (ranges 70 – 364 hours). Major BPEs, as defined by marked differences in mean ICP despite similar ICP waveform, were seen in 9 of them (56%). The BPEs were of magnitudes that had the potential to alter patient management. Conclusions Baseline Pressure Errors (BPEs) occur in a significant number of patients undergoing continuous ICP monitoring and they may alter patient management. The current practice of measuring ICP against a baseline pressure does not comply with the concept of State of the Art. Monitoring of the ICP waves ought to become the new State of the Art as they are not influenced by BPEs. PMID:24472296

  11. Long term effects of guar gum on metabolic control, serum cholesterol and blood pressure levels in type 2 (non-insulin-dependent) diabetic patients with high blood pressure.

    PubMed

    Uusitupa, M; Tuomilehto, J; Karttunen, P; Wolf, E

    1984-01-01

    A double-blind, placebo-controlled trial was carried out in 17 Type 2 (non-insulin-dependent) diabetic patients, treated with diet therapy alone to study the effects of guar gum on metabolic control, serum lipids, and blood pressure levels. Thirteen of the patients had drug treatment for hypertension. Guar gum was taken with meals three times a day, and the dose was gradually increased to 21 g per day. A slight, but not significant improvement was found in the metabolic control of the patients after the guar gum treatment compared to the placebo. Serum total cholesterol was 11% (p greater than 0.01) lower after the guar gum but no significant differences were found in HDL-cholesterol or serum triglycerides during the guar gum treatment compared to the placebo. Diastolic blood pressure level was significantly lower during the guar gum treatment compared to placebo. No difference was observed in systolic blood pressure levels between the guar gum and placebo treatments. The reduction of diastolic blood pressure was independent of changes in fasting blood glucose level or body weight, but could in part be due to simultaneous reduction in serum cholesterol concentration. The changes associated with guar gum supplementation suggest a reduction in the risk for cardiovascular complications in diabetic patients.

  12. Observations of a pressurized hydraulic hose under lateral liquid impacts

    NASA Astrophysics Data System (ADS)

    Stewart, C. D.; Gorman, D. G.

    The effects of 'pin-hole' failure of one pressurized hydraulic hose on its neighbour are investigated. A pressurized test hose was inserted into a custom testing apparatus and subjected to a series of ten short duration liquid impacts simulating the pin-hole failure of an initial hose. Subsequent displacements of the hose were filmed and plotted with respect to time. Three distinct pattern groups emerged which were used to explain the resultant damage to the hose. It was observed that the middle pattern, corresponding to impacts 6 and 7, appears to be the point where the very damaging hydraulic penetration mechanism became dominant and the outer layer of the hose failed. On completion of the ten impact series it was observed that a small hole on the outer surface of the hose gave way to a relatively large damaged area in the strength bearing inner braid material.

  13. Graphene Squeeze-Film Pressure Sensors.

    PubMed

    Dolleman, Robin J; Davidovikj, Dejan; Cartamil-Bueno, Santiago J; van der Zant, Herre S J; Steeneken, Peter G

    2016-01-13

    The operating principle of squeeze-film pressure sensors is based on the pressure dependence of a membrane's resonance frequency, caused by the compression of the surrounding gas which changes the resonator stiffness. To realize such sensors, not only strong and flexible membranes are required, but also minimization of the membrane's mass is essential to maximize responsivity. Here, we demonstrate the use of a few-layer graphene membrane as a squeeze-film pressure sensor. A clear pressure dependence of the membrane's resonant frequency is observed, with a frequency shift of 4 MHz between 8 and 1000 mbar. The sensor shows a reproducible response and no hysteresis. The measured responsivity of the device is 9000 Hz/mbar, which is a factor 45 higher than state-of-the-art MEMS-based squeeze-film pressure sensors while using a 25 times smaller membrane area.

  14. Modeling Thermal Pressurization Around Shallow Dikes Using Temperature-Dependent Hydraulic Properties: Implications for Deformation Around Intrusions

    NASA Astrophysics Data System (ADS)

    Townsend, Meredith R.

    2018-01-01

    Pressurization and flow of groundwater around igneous intrusions depend in part on the hydraulic diffusivity of the host rocks and processes that enhance diffusivity, such as fracturing, or decrease diffusivity, such as mineral precipitation during chemical alteration. Characterizing and quantifying the coupled effects of alteration, pore pressurization, and deformation have significant implications for deformation around intrusions, geothermal energy, contact metamorphism, and heat transfer at mid-ocean ridges. Fractures around dikes at Ship Rock, New Mexico, indicate that pore pressures in the host rocks exceeded hydrostatic conditions by at least 15 MPa following dike emplacement. Hydraulic measurements and petrographic analysis indicate that mineral precipitation clogged the pores of the host rock, reducing porosity from 0.25 to <0.10 and reducing permeability by 5 orders of magnitude. Field data from Ship Rock are used to motivate and constrain numerical models for thermal pore fluid pressurization adjacent to a meter-scale dike, using temperature-dependent hydraulic properties in the host rock as a proxy for porosity loss by mineral precipitation during chemical alteration. Reduction in permeability by chemical alteration has a negligible effect on pressurization. However, reduction in porosity by mineral precipitation increases fluid pressure by constricting pore volume and is identified as a potentially significant source of pressure. A scaling relationship is derived to determine when porosity loss becomes important; if permeability is low enough, pressurization by porosity loss outweighs pressurization by thermal expansion of fluids.

  15. Pressure and temperature dependences of the ionic conductivities of the thallous halidesTlCl, TlBr, and TlI

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

    Samara, G.A.

    1981-01-15

    Detailed studies of the pressure and temperature dependences of the ionic conductivities of TlCl and TlBr have allowed determination of the lattice volume relaxations and energies associated with the formation and motion of Schottky defects in these crystals. The volume relaxations deduced from the conductivity are found to be comparable in magnitude with values calculated from the strain energy model and a dynamical model. The association energy of Tl/sup +/ vacancies and divalent impurities was also determined for TlBr. A particularly important result is the finding that for these CsCl-type crystals the relaxation of the lattice associated with vacancy formationmore » is outward. Earlier studies on ionic crystals having the NaCl structure have yielded a similar result. This outward relaxation thus appears to be a general result for ionic crystals of both the NaCl and CsCl types (and possibly other ionic lattice types), in disagreement with earlier theoretical calculations which show that the relaxation should be inward for all models of ionic vacancies investigated. The conductivity of TlI was studied in both the (low temperature and pressure) orthorhombic phase as well as in the cubic CsCl-type phase. There is a large electronic contribution to the conductivity in the orthorhombic phase. An interesting result for all three materials is the observation in the cubic phase of a pressure-induced transition from ionic to electronic conduction. This is in qualitative agreement with what is known about the pressure dependences of the electronic structure of these materials.« less

  16. Pressure and phase dependence of the stereochemical course in hot tritium for hydrogen and chlorine-38 for chlorine substitution in meso- and rac-1,2-dichloro-1,2-difluoroethane

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

    Machulla, H J; Stocklin, G

    1974-03-28

    The pressure dependence of the stereochemical course in hot homolytic T- for-H and /sup 38/ Cl-for-Cl substitution in mesoand rac-1,2-dichloro-l,2- difluoroethane has been studied from 10 to 10/sup 4/ Torr. Distinct differences are observed between the yield vs. density dependence of the retained and the inverted product. For both recoil tritium and chlorine, substitution with inversion of configuration is almost negligible in the gas phase and its yields remained constant over the entire pressure range studied. Typical pressure effects are observed, however, for substitution with retention of configuration, particularly for recoil chlorine. While the change from the high-pressure gas phasemore » to the liquid leaves T-for-H substitution almost unaffected, /sup 38/Cl-for- Cl substitution exhibits a strong phase effect. The absolute yields of the retained product increase by a factor of 2.5, that of the invented product by about 20, almost identical in both diastereomeric substrates. The density dependence of the HCl and HF elimination products is also different for recoil tritium and chlorine; in the latter case the yields follow the increasing trend observed for substitution. While for recoil tritium the predominant substitution channel seems to be a direct replacement with retention of configuration, even in the liquid phase, /sup 38/Cl-for-Cl substitution at higher densities cannot be satisfactorily explained on the basis of the impact model nor by caged radical combination. Alternatively, substitution via a caged complex is discussed. (auth)« less

  17. Origin of the pressure-dependent Tc valley in superconducting simple cubic phosphorus

    NASA Astrophysics Data System (ADS)

    Wu, Xianxin; Jeschke, Harald O.; Di Sante, Domenico; von Rohr, Fabian O.; Cava, Robert J.; Thomale, Ronny

    2018-03-01

    Motivated by recent experiments, we investigate the pressure-dependent electronic structure and electron-phonon (e-ph) coupling for simple cubic phosphorus by performing first-principles calculations within the full potential linearized augmented plane-wave method. As a function of increasing pressure, our calculations show a valley feature in Tc, followed by an eventual decrease for higher pressures. We demonstrate that this Tc valley at low pressures is due to two nearby Lifshitz transitions, as we analyze the band-resolved contributions to the e-ph coupling. Below the first Lifshitz transition, the phonon hardening and shrinking of the γ Fermi surface with s -orbital character results in a decreased Tc with increasing pressure. After the second Lifshitz transition, the appearance of δ Fermi surfaces with 3 d -orbital character generate strong e-ph interband couplings in α δ and β δ channels, and hence lead to an increase of Tc. For higher pressures, the phonon hardening finally dominates, and Tc decreases again. Our study reveals that the intriguing Tc valley discovered in experiment can be attributed to Lifshitz transitions, while the plateau of Tc detected at intermediate pressures appears to be beyond the scope of our analysis. This strongly suggests that aside from e-ph coupling, electronic correlations along with plasmonic contributions may be relevant for simple cubic phosphorus. Our findings hint at the notion that increasing pressure can shift the low-energy orbital weight towards d character, and as such even trigger an enhanced importance of orbital-selective electronic correlations despite an increase of the overall bandwidth.

  18. Observation of a New High-Pressure Solid Phase in Dynamically Compressed Aluminum

    NASA Astrophysics Data System (ADS)

    Polsin, D. N.

    2017-10-01

    Aluminum is ideal for testing theoretical first-principles calculations because of the relative simplicity of its atomic structure. Density functional theory (DFT) calculations predict that Al transforms from an ambient-pressure, face-centered-cubic (fcc) crystal to the hexagonal close-packed (hcp) and body-centered-cubic (bcc) structures as it is compressed. Laser-driven experiments performed at the University of Rochester's Laboratory for Laser Energetics and the National Ignition Facility (NIF) ramp compressed Al samples to pressures up to 540 GPa without melting. Nanosecond in-situ x-ray diffraction was used to directly measure the crystal structure at pressures where the solid-solid phase transformations of Al are predicted to occur. Laser velocimetry provided the pressure in the Al. Our results show clear evidence of the fcc-hcp and hpc-bcc transformations at 216 +/- 9 GPa and 321 +/- 12 GPa, respectively. This is the first experimental in-situ observation of the bcc phase in compressed Al and a confirmation of the fcc-hcp transition previously observed under static compression at 217 GPa. The observations indicate these solid-solid phase transitions occur on the order of tens of nanoseconds time scales. In the fcc-hcp transition we find the original texture of the sample is preserved; however, the hcp-bcc transition diminishes that texture producing a structure that is more polycrystalline. The importance of this dynamic is discussed. The NIF results are the first demonstration of x-ray diffraction measurements at two different pressures in a single laser shot. This material is based upon work supported by the Department of Energy National Nuclear Security Administration under Award Number DE-NA0001944.

  19. Temperature- and pressure-dependent structural transformation of methane hydrates in salt environments

    NASA Astrophysics Data System (ADS)

    Shin, Donghoon; Cha, Minjun; Yang, Youjeong; Choi, Seunghyun; Woo, Yesol; Lee, Jong-Won; Ahn, Docheon; Im, Junhyuck; Lee, Yongjae; Han, Oc Hee; Yoon, Ji-Ho

    2017-03-01

    Understanding the stability of volatile species and their compounds under various surface and subsurface conditions is of great importance in gaining insights into the formation and evolution of planetary and satellite bodies. We report the experimental results of the temperature- and pressure-dependent structural transformation of methane hydrates in salt environments using in situ synchrotron X-ray powder diffraction, solid-state nuclear magnetic resonance, and Raman spectroscopy. We find that under pressurized and concentrated brine solutions methane hydrate forms a mixture of type I clathrate hydrate, ice, and hydrated salts. Under a low-pressure condition, however, the methane hydrates are decomposed through a rapid sublimation of water molecules from the surface of hydrate crystals, while NaCl · 2H2O undergoes a phase transition into a crystal growth of NaCl via the migration of salt ions. In ambient pressure conditions, the methane hydrate is fully decomposed in brine solutions at temperatures above 252 K, the eutectic point of NaCl · 2H2O.

  20. Characterisation of an ion source on the Helix MC Plus noble gas mass spectrometer - pressure dependent mass discrimination

    NASA Astrophysics Data System (ADS)

    Zhang, X.

    2017-12-01

    Characterisation of an ion source on the Helix MC Plusnoble gas mass spectrometer - pressure dependent mass discrimination Xiaodong Zhang* dong.zhang@anu.edu.au Masahiko Honda Masahiko.honda@anu.edu.au Research School of Earth Sciences, The Australian National University, Canberra, Australia To obtain reliable measurements of noble gas elemental and isotopic abundances in a geological sample it is essential that the mass discrimination (instrument-induced isotope fractionation) of the mass spectrometer remain constant over the working range of noble gas partial pressures. It is known, however, that there are pressure-dependent variations in sensitivity and mass discrimination in conventional noble gas mass spectrometers [1, 2, 3]. In this study, we discuss a practical approach to ensuring that the pressure effect in the Helix MC Plus high resolution, multi-collector noble gas mass spectrometer is minimised. The isotopic composition of atmospheric Ar was measured under a range of operating conditions to test the effects of different parameters on Ar mass discrimination. It was found that the optimised ion source conditions for pressure independent mass discrimination for Ar were different from those for maximised Ar sensitivity. The optimisation can be achieved by mainly adjusting the repeller voltage. It is likely that different ion source settings will be required to minimise pressure-dependent mass discrimination for different noble gases. A recommended procedure for tuning an ion source to reduce pressure dependent mass discrimination will be presented. References: Honda M., et al., Geochim. Cosmochim. Acta, 57, 859 -874, 1993. Burnard P. G., and Farley K. A., Geochemistry Geophysics Geosystems, Volume 1, 2000GC00038, 2000. Mabry J., et al., Journal of Analytical Atomic Spectrometry, 27, 1012 - 1017, 2012.

  1. Observed antiprotons and energy dependent confinement of cosmic rays: A conflict?

    NASA Technical Reports Server (NTRS)

    Stephens, S. A.

    1985-01-01

    In the frame work of energy dependent confinement for cosmic rays, the energy spectrum inside the source is flatter than that observed. Antiproton observation suggests large amount of matter is being traversed by cosmic rays in some sources. As a result, secondary particles are produced in abundance. Their spectra was calculated and it is shown that the energy dependent confinement model is in conflict with some observations.

  2. The Body Mass Index, Blood Pressure, and Fasting Blood Glucose in Patients With Methamphetamine Dependence.

    PubMed

    Lv, Dezhao; Zhang, Meijuan; Jin, Xuru; Zhao, Jiyun; Han, Bin; Su, Hang; Zhang, Jie; Zhang, Xiangyang; Ren, Wenwei; He, Jincai

    2016-03-01

    Methamphetamine (MA) is a prevalently abused psychostimulant in the world. Previously published studies and case reports indicated potential associations between MA and body mass index (BMI) and cardiovascular factors (eg, blood pressure and fasting blood glucose). However, these associations have not been studied clearly. This study aimed to investigate BMI and cardiovascular factors in the MA-dependent patients.A total of 1019 MA-dependent patients were recruited between February 2, 2008 and March 11, 2013. A case report was used to gather information on sociocharacteristics and drug-dependent history. Meanwhile, a number of 1019 age- and sex-matched controls' information were collected from the physical examination center. We measured BMI, blood pressure, and fasting blood glucose among the participants.MA-dependent patients had significantly lower BMI (20.4 ± 0.1 vs 23.9 ± 0.1 kg/m, P < 0.001), lower fasting blood glucose (5.0 ± 0.01 vs 5.2 ± 0.01 mmol/L, P < 0.001) and higher systolic blood pressure (122.1 ± 0.4 vs 114.8 ± 0.4 mmHg, P < 0.001) compared with the control group after adjustment of possible confounders. Additional, we only found the duration of MA use was independently associated with BMI (B = -0.08, P = 0.04).This study demonstrated that MA dependence was associated with BMI and cardiovascular factors. In addition, we found a negative association between duration of MA use and BMI.

  3. Non-linear pressure/temperature-dependence of high pressure thermal inactivation of proteolytic Clostridium botulinum type B in foods.

    PubMed

    Maier, Maximilian B; Lenz, Christian A; Vogel, Rudi F

    2017-01-01

    The effect of high pressure thermal (HPT) processing on the inactivation of spores of proteolytic type B Clostridium botulinum TMW 2.357 in four differently composed low-acid foods (green peas with ham, steamed sole, vegetable soup, braised veal) was studied in an industrially feasible pressure range and temperatures between 100 and 120°C. Inactivation curves exhibited rapid inactivation during compression and decompression followed by strong tailing effects. The highest inactivation (approx. 6-log cycle reduction) was obtained in braised veal at 600 MPa and 110°C after 300 s pressure-holding time. In general, inactivation curves exhibited similar negative exponential shapes, but maximum achievable inactivation levels were lower in foods with higher fat contents. At high treatment temperatures, spore inactivation was more effective at lower pressure levels (300 vs. 600 MPa), which indicates a non-linear pressure/temperature-dependence of the HPT spore inactivation efficiency. A comparison of spore inactivation levels achievable using HPT treatments versus a conventional heat sterilization treatment (121.1°C, 3 min) illustrates the potential of combining high pressures and temperatures to replace conventional retorting with the possibility to reduce the process temperature or shorten the processing time. Finally, experiments using varying spore inoculation levels suggested the presence of a resistant fraction comprising approximately 0.01% of a spore population as reason for the pronounced tailing effects in survivor curves. The loss of the high resistance properties upon cultivation indicates that those differences develop during sporulation and are not linked to permanent modifications at the genetic level.

  4. Discriminating different type waves from pressure and ground motion observation in the seafloor by DONET cabled observation network.

    NASA Astrophysics Data System (ADS)

    Araki, E.; Kawaguchi, K.; Kaneda, Y.

    2011-12-01

    We developed and deployed seafloor cabled observatory called "Dense Ocean-floor Network for Earthquake and Tsunamis (DONET)" in the Nankai Trough, south of Japan. The main purpose of the DONET network is to observe large earthquake such as Tonankai earthquake in the deployed seafloor and associate Tsunamis in real-time to help disaster mitigation, and as well to monitor inter-seismic crustal activities such as micro earthquakes, very low frequency earthquakes, and slower crustal deformation. In each DONET seafloor observatory, high-sensitive broadband set of instruments for seismic and seafloor pressure monitoring, consisted from Guralp CMG3T broadband seismometer, Metrozet TSA100S accelerometer, Paroscientific 8B7000-2 pressure gauge, a deep-sea differential pressure gauge, a hydrophone, and a seawater thermometer, are installed. The density of seafloor observatories are 20 observatories distributed in 15-30 km interval which is optimized for monitoring of events in the plate boundary beneath the network. DONET may be regarded as a large-scale, high sensitive high density seismic array for monitoring teleseismic events in the Philippine Sea and the Pacific Ocean. The DONET seafloor observatories are situated in wide range of seafloor depth between 1800m and 4500m, from the seafloor basin about 50 km off Japanese Island through the slope of accerecionary prism to the deep trench axis 150 km off the coast, that may also regarded as a vertical array in the 4.5km thick ocean. This variation of depths helps identify T-phases from the array record. In data analysis, it is necessary to identify propagation mode of each observed wave which may often be mixed together. In our design of DONET observation system, we took care to help identification of seismic phase by obtaining both ground motion and seafloor pressure in the same location. This is simply achieved by combining seafloor pressure gauges and seismometer in a single observatory package, but care was taken to

  5. Pressure Dependence of Excitation Cross Sections for Resonant Levels of Rare Gases

    NASA Astrophysics Data System (ADS)

    Stewart, Michael D.; Chilton, J. Ethan; Lin, Chun C.

    2000-06-01

    In the rare gases, the excited n'p^5ns and n'p^5nd levels with J = 1 are optically coupled to ground as well as lower lying p levels. Resonant photons emitted when the atom decays to ground can be reabsorbed by another ground-state atom. At low gas pressures this reabsorption occurs infrequently, but at higher pressures becomes increasingly likely until the resonant transition is completely suppressed. This enhances the cascade transitions into lower p levels, resulting in pressure dependent optical emission cross sections. This reabsorption process can be understood quantitatively with a model developed by Heddle et al(D. W. O. Heddle and N. J. Samuel, J. Phys. B 3), 1593 (1970).. The radiation from transitions into the nonresonant levels often lie in the ir, while the resonant radiation is always in the uv spectral region. Using a Fourier-transform spectrometer, one can measure the cross sections for the ir transitions as a function of pressure. The Heddle model can be fit to these data with the use of theoretical values for the Einstein A coefficients. This provides a test of the accuracy of calculated A values. Discussion will include cross section measurements for Ne, Ar, and Kr excited by electron impact over a range of gas pressures.

  6. Effect of dipeptidyl peptidase-4 inhibition on circadian blood pressure during the development of salt-dependent hypertension in rats

    PubMed Central

    Sufiun, Abu; Rafiq, Kazi; Fujisawa, Yoshihide; Rahman, Asadur; Mori, Hirohito; Nakano, Daisuke; Kobori, Hiroyuki; Ohmori, Koji; Masaki, Tsutomu; Kohno, Masakazu; Nishiyama, Akira

    2015-01-01

    A growing body of evidence has indicated that dipeptidyl peptidase-4 (DPP-4) inhibitors have antihypertensive effects. Here, we aim to examine the effect of vildagliptin, a DPP-4-specific inhibitor, on blood pressure and its circadian-dipping pattern during the development of salt-dependent hypertension in Dahl salt-sensitive (DSS) rats. DSS rats were treated with a high-salt diet (8% NaCl) plus vehicle or vildagliptin (3 or 10 mg kg−1 twice daily by oral gavage) for 7 days. Blood pressure was measured by the telemetry system. High-salt diet for 7 days significantly increased the mean arterial pressure (MAP), systolic blood pressure (SBP) and were also associated with an extreme dipping pattern of blood pressure in DSS rats. Treatment with vildagliptin dose-dependently decreased plasma DPP-4 activity, increased plasma glucagon-like peptide 1 (GLP-1) levels and attenuated the development of salt-induced hypertension. Furthermore, vildagliptin significantly increased urine sodium excretion and normalized the dipping pattern of blood pressure. In contrast, intracerebroventricular infusion of vildagliptin (50, 500 or 2500 μg) did not alter MAP and heart rate in DSS rats. These data suggest that salt-dependent hypertension initially develops with an extreme blood pressure dipping pattern. The DPP-4 inhibitor, vildagliptin, may elicit beneficial antihypertensive effects, including the improvement of abnormal circadian blood pressure pattern, by enhancing urinary sodium excretion. PMID:25588850

  7. Pressure dependence of the optical phonon frequencies and the transverse effective charge in AlSb

    NASA Astrophysics Data System (ADS)

    Ves, S.; Strössner, K.; Cardona, M.

    1986-02-01

    The first order Raman scattering by TO and LO phonons has been measured in AlSb under hydrostatic' pressures up to its phase transition. The Raman frequencies increase nearly linear while the transverse effective charge e ∗T are compared with estimates based on pseudopotential and on LCAO calculation. In order to obtain from the measured pressure dependence the corresponding volume coefficients the bulk modulus B O and its pressure derivative BOˌ = {dBO}/{dP} was measured by energy-dispersive X-ray diffraction (B O = 55.1 GPa and BOˌ = 4.55 ).

  8. Pressure dependence of the optical properties of the charge-density-wave compound LaTe2

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

    Lavagnini, M.; Sacchetti, A.; Degiorgi, L.

    2009-12-14

    We report the pressure dependence of the optical response of LaTe{sub 2}, which is deep in the charge-density-wave (CDW) ground state even at 300 K. The reflectivity spectrum is collected in the mid-infrared spectral range at room temperature and at pressures between 0 and 7 GPa. We extract the energy scale due to the single particle excitation across the CDW gap and the Drude weight. We establish that the gap decreases upon compressing the lattice, while the Drude weight increases. This signals a reduction in the quality of nesting upon applying pressure, therefore inducing a lesser impact of the CDWmore » condensate on the electronic properties of LaTe{sub 2}. The consequent suppression of the CDW gap leads to a release of additional charge carriers, manifested by the shift of weight from the gap feature into the metallic component of the optical response. On the contrary, the power-law behavior, seen in the optical conductivity at energies above the gap excitation and indicating a weakly interacting limit within the Tomonaga-Luttinger liquid scenario, seems to be only moderately dependent on pressure.« less

  9. Clutch pressure estimation for a power-split hybrid transmission using nonlinear robust observer

    NASA Astrophysics Data System (ADS)

    Zhou, Bin; Zhang, Jianwu; Gao, Ji; Yu, Haisheng; Liu, Dong

    2018-06-01

    For a power-split hybrid transmission, using the brake clutch to realize the transition from electric drive mode to hybrid drive mode is an available strategy. Since the pressure information of the brake clutch is essential for the mode transition control, this research designs a nonlinear robust reduced-order observer to estimate the brake clutch pressure. Model uncertainties or disturbances are considered as additional inputs, thus the observer is designed in order that the error dynamics is input-to-state stable. The nonlinear characteristics of the system are expressed as the lookup tables in the observer. Moreover, the gain matrix of the observer is solved by two optimization procedures under the constraints of the linear matrix inequalities. The proposed observer is validated by offline simulation and online test, the results have shown that the observer achieves significant performance during the mode transition, as the estimation error is within a reasonable range, more importantly, it is asymptotically stable.

  10. Some observations of tip-vortex cavitation

    NASA Astrophysics Data System (ADS)

    Arndt, R. E. A.; Arakeri, V. H.; Higuchi, H.

    1991-08-01

    Cavitation has been observed in the trailing vortex system of an elliptic platform hydrofoil. A complex dependence on Reynolds number and gas content is noted at inception. Some of the observations can be related to tension effects associated with the lack of sufficiently large-sized nuclei. Inception measurements are compared with estimates of pressure in the vortex obtained from LDV measurements of velocity within the vortex. It is concluded that a complete correlation is not possible without knowledge of the fluctuating levels of pressure in tip-vortex flows. When cavitation is fully developed, the observed tip-vortex trajectory flows. When cavitation is fully developed, the observed tip-vortex trajectory shows a surprising lack of dependence on any of the physical parameters varied, such as angle of attack, Reynolds number, cavitation number, and dissolved gas content.

  11. Implementation into earthquake sequence simulations of a rate- and state-dependent friction law incorporating pressure solution creep

    NASA Astrophysics Data System (ADS)

    Noda, H.

    2016-05-01

    Pressure solution creep (PSC) is an important elementary process in rock friction at high temperatures where solubilities of rock-forming minerals are significantly large. It significantly changes the frictional resistance and enhances time-dependent strengthening. A recent microphysical model for PSC-involved friction of clay-quartz mixtures, which can explain a transition between dilatant and non-dilatant deformation (d-nd transition), was modified here and implemented in dynamic earthquake sequence simulations. The original model resulted in essentially a kind of rate- and state-dependent friction (RSF) law, but assumed a constant friction coefficient for clay resulting in zero instantaneous rate dependency in the dilatant regime. In this study, an instantaneous rate dependency for the clay friction coefficient was introduced, consistent with experiments, resulting in a friction law suitable for earthquake sequence simulations. In addition, a term for time-dependent strengthening due to PSC was added which makes the friction law logarithmically rate-weakening in the dilatant regime. The width of the zone in which clasts overlap or, equivalently, the interface porosity involved in PSC plays a role as the state variable. Such a concrete physical meaning of the state variable is a great advantage in future modelling studies incorporating other physical processes such as hydraulic effects. Earthquake sequence simulations with different pore pressure distributions demonstrated that excess pore pressure at depth causes deeper rupture propagation with smaller slip per event and a shorter recurrence interval. The simulated ruptures were arrested a few kilometres below the point of pre-seismic peak stress at the d-nd transition and did not propagate spontaneously into the region of pre-seismic non-dilatant deformation. PSC weakens the fault against slow deformation and thus such a region cannot produce a dynamic stress drop. Dynamic rupture propagation further down to

  12. New Laboratory Observations of Thermal Pressurization Weakening

    NASA Astrophysics Data System (ADS)

    Badt, N.; Tullis, T. E.; Hirth, G.

    2017-12-01

    Dynamic frictional weakening due to pore fluid thermal pressurization has been studied under elevated confining pressure in the laboratory, using a rotary-shear apparatus having a sample with independent pore pressure and confining pressure systems. Thermal pressurization is directly controlled by the permeability of the rocks, not only for the initiation of high-speed frictional weakening but also for a subsequent sequence of high-speed sliding events. First, the permeability is evaluated at different effective pressures using a method where the pore pressure drop and the flow-through rate are compared using Darcy's Law as well as a pore fluid oscillation method, the latter method also permitting measurement of the storage capacity. Then, the samples undergo a series of high-speed frictional sliding segments at a velocity of 2.5 mm/s, under an applied confining pressure and normal stress of 45 MPa and 50 MPa, respectively, and an initial pore pressure of 25 MPa. Finally the rock permeability and storage capacity are measured again to assess the evolution of the rock's pore fluid properties. For samples with a permeability of 10-20 m2 thermal pressurization promotes a 40% decrease in strength. However, after a sequence of three high-speed sliding events, the magnitude of weakening diminishes progressively from 40% to 15%. The weakening events coincide with dilation of the sliding interface. Moreover, the decrease in the weakening degree with progressive fast-slip events suggest that the hydraulic diffusivity may increase locally near the sliding interface during thermal pressurization-enhanced slip. This could result from stress- or thermally-induced damage to the host rock, which would perhaps increase both permeability and storage capacity, and so possibly decrease the susceptibility of dynamic weakening due to thermal pressurization in subsequent high-speed sliding events.

  13. Pressure dependence of the monoclinic phase in (1–x)Pb(Mg 1/3Nb 2/3)O 3-xPbTiO₃ solid solutions

    DOE PAGES

    Ahart, Muhtar; Sinogeikin, Stanislav; Shebanova, Olga; ...

    2012-12-26

    We combine high-pressure x-ray diffraction, high-pressure Raman scattering, and optical microscopy to investigate a series of (1–x)Pb(Mg 1/3Nb 2/3)O 3-xPbTiO₃ (PMN-xPT) solid solutions (x=0.2, 0.3, 0.33, 0.35, 0.37, 0.4) in diamond anvil cells up to 20 GPa at 300 K. The Raman spectra show a peak centered at 380 cm⁻¹ starting above 6 GPa for all samples, in agreement with previous observations. X-ray diffraction measurements are consistent with this spectral change indicating a structural phase transition; we find that the triplet at the pseudocubic (220) Bragg peak merges into a doublet above 6 GPa. Our results indicate that the morphotropicmore » phase boundary region (x=0.33–0.37) with the presence of monoclinic symmetry persists up to 7 GPa. The pressure dependence of ferroelectric domains in PMN-0.32PT single crystals was observed using a polarizing optical microscope. The domain wall density decreases with pressure and the domains disappear at a modest pressure of 3 GPa. We propose a pressure-composition phase diagram for PMN-xPT solid solutions.« less

  14. Competition and coexistence of polar and non-polar states in Sr1-x Ca x TiO3: an investigation using pressure dependent Raman spectroscopy

    NASA Astrophysics Data System (ADS)

    Tyagi, Shekhar; Sharma, Gaurav; Sathe, Vasant G.

    2018-03-01

    The competition and cooperation between ferroelectric and anti-ferro-distortion (AFD) instabilities are studied using pressure dependent Raman spectroscopy on polycrystalline powder samples of Sr1-x Ca x TiO3(x  =  0.0, 0.06, 0.25, 0.35). For x  =  0.0 composition, a broad polar mode is detected in the Raman spectra above 6 GPa, while for x  =  0.06 composition, the polar modes appear well above 9 GPa where the AFD modes showed strong suppression. In x  =  0.25 and 0.35 composition, the application of small pressure resulted in the appearance of strong AFD modes suppressing the polar modes. At elevated pressures, re-entrant polar modes are observed along with the broad AFD modes and some new peaks are also observed, signifying the lowering of local symmetry. The reappearance of polar modes is found to be related to pressure induced symmetry disorder at local level, suggesting its electronic origin. The re-entrant polar modes observed at higher pressure values are found to be significantly broad and asymmetric in nature, signifying the development of ferroelectric micro regions/nano domains coexisting with AFD. The lower symmetry at local length scale provides a conducive atmosphere for coexisting AFD and FE instabilities.

  15. The Observed Properties of Liquid Helium at the Saturated Vapor Pressure

    NASA Astrophysics Data System (ADS)

    Donnelly, Russell J.; Barenghi, Carlo F.

    1998-11-01

    The equilibrium and transport properties of liquid 4He are deduced from experimental observations at the saturated vapor pressure. In each case, the bibliography lists all known measurements. Quantities reported here include density, thermal expansion coefficient, dielectric constant, superfluid and normal fluid densities, first, second, third, and fourth sound velocities, specific heat, enthalpy, entropy, surface tension, ion mobilities, mutual friction, viscosity and kinematic viscosity, dispersion curve, structure factor, thermal conductivity, latent heat, saturated vapor pressure, thermal diffusivity and Prandtl number of helium I, and displacement length and vortex core parameter in helium II.

  16. Coexistence pressure for a martensitic transformation from theory and experiment: Revisiting the bcc-hcp transition of iron under pressure

    DOE PAGES

    Zarkevich, N. A.; Johnson, D. D.

    2015-05-12

    We revisit results from decades of pressure experiments on the bcc ↔ hcp transformations in iron, which are sensitive to non-hydrostatic conditions and sample size. We emphasize the role of martensitic stress in the observed pressure hysteresis and address the large spread in values for onset pressures of the nucleating phase. From electronic-structure calculations, we find a bcc ↔ hcp equilibrium coexistence pressure of 8.4 GPa. Accounting for non-hydrostatic martensitic stress and a stress-dependent transition barrier, we suggest a pressure inequality for better comparison to experiment and observed hysteresis. We construct the equation of state for bcc and hcp phasesmore » under hydrostatic pressure, and compare to experiments and previous calculations.« less

  17. Pressure dependence of the electro-optic response function in partially exposed polymer dispersed ferroelectric liquid crystals

    NASA Technical Reports Server (NTRS)

    Parmar, D. S.; Holmes, H. K.

    1993-01-01

    Ferroelectric liquid crystals in a new configuration, termed partially exposed polymer dispersed ferroelectric liquid crystal (PEPDFLC), respond to external pressures and demonstrate pressure-induced electro-optic switching response. When the PEPDFLC thin film is sandwiched between two transparent conducting electrodes, one a glass plate and the other a flexible sheet such as polyvenylidene fluoride, the switching characteristics of the thin film are a function of the pressure applied to the flexible transparent electrode and the bias voltage across the electrodes. Response time measurements reveal a linear dependence of the change in electric field with external pressure.

  18. New Developments in Nickel-Hydrogen Dependent Pressure Vessel (DPV) Cell and Battery Design

    NASA Technical Reports Server (NTRS)

    Caldwell, Dwight B.; Fox, Chris L.; Miller, Lee E.

    1997-01-01

    THe Dependent Pressure Vessel (DPV) Nickel-Hydrogen (NiH2) design is being developed as an advanced battery for military and commercial, aerospace and terrestrial applications. The DPV cell design offers high specific energy and energy density as well as reduced cost, while retaining the established Individual Pressure Vessel (IPV) technology flight heritage and database. This advanced DPV design also offers a more efficient mechanical, electrical and thermal cell and battery configuration and a reduced part count. The DPV battery design promotes compact, minimum volume packaging and weight efficiency, and delivers cost and weight savings with minimal design risk.

  19. Pressure dependence of the absolute rate constant for the reaction OH + C2H2 from 228 to 413K

    NASA Technical Reports Server (NTRS)

    Michael, J. V.; Nava, D. F.; Borokowski, R. P.; Payne, W. A.; Stief, L. J.

    1980-01-01

    The pressure dependence of absolute rate constants for the reaction of OH + C2H2 yields products has been examined at five temperatures ranging from 228 to 413 K. The experimental techniques which was used is flash photolysis-resonance fluoresence. OH was produced by water photolysis and hydroxyl resonance fluorescent photons were measured by multiscaling techniques. The results indicate that the low pressure bimolecular rate constant is 4 x 10 the the minus 13th power cu cm molecule (-1) s(-1) over the temperature range studied. A substantial increase in the bimolecular rate constant with an increase in pressure was observed at all temperatures except 228 K. This indicates the importance of initial adduct formation and subsequent stablization. The high pressure results are well represented by the Arrhenius expression (k sub bi) sub infinity = (6.83 + or - 1.19) x 10 to the minus 12th power exp(-646 + or - 47/T)cu cm molecule (-1) s(-1). The results are compared to previous investigated and are theoretically discussed. The implications of these results on modeling of terrestrial and planetary atmospheres and also in combustion chemistry are discussed.

  20. Observation of Live Ticks (Haemaphysalis flava) by Scanning Electron Microscopy under High Vacuum Pressure

    PubMed Central

    Ishigaki, Yasuhito; Nakamura, Yuka; Oikawa, Yosaburo; Yano, Yasuhiro; Kuwabata, Susumu; Nakagawa, Hideaki; Tomosugi, Naohisa; Takegami, Tsutomu

    2012-01-01

    Scanning electron microscopes (SEM), which image sample surfaces by scanning with an electron beam, are widely used for steric observations of resting samples in basic and applied biology. Various conventional methods exist for SEM sample preparation. However, conventional SEM is not a good tool to observe living organisms because of the associated exposure to high vacuum pressure and electron beam radiation. Here we attempted SEM observations of live ticks. During 1.5×10−3 Pa vacuum pressure and electron beam irradiation with accelerated voltages (2–5 kV), many ticks remained alive and moved their legs. After 30-min observation, we removed the ticks from the SEM stage; they could walk actively under atmospheric pressure. When we tested 20 ticks (8 female adults and 12 nymphs), they survived for two days after SEM observation. These results indicate the resistance of ticks against SEM observation. Our second survival test showed that the electron beam, not vacuum conditions, results in tick death. Moreover, we describe the reaction of their legs to electron beam exposure. These findings open the new possibility of SEM observation of living organisms and showed the resistance of living ticks to vacuum condition in SEM. These data also indicate, for the first time, the usefulness of tick as a model system for biology under extreme condition. PMID:22431980

  1. Sustained acute voltage-dependent blood pressure decrease with prolonged carotid baroreflex activation in therapy-resistant hypertension.

    PubMed

    Alnima, Teba; Scheffers, Ingrid; De Leeuw, Peter W; Winkens, Bjorn; Jongen-Vancraybex, Heidi; Tordoir, Jan H M; Schmidli, Jürg; Mohaupt, Markus G; Allemann, Yves; Kroon, Abraham A

    2012-08-01

    Chronic carotid baroreflex stimulation (Rheos system) has been shown to effectively reduce blood pressure in patients with resistant hypertension. Upon acute stimulation blood pressure also falls as a function of voltage. the aim of this study is to evaluate whether this voltage-dependent blood pressure decrease is preserved after long-term carotid baroreflex stimulation. Forty-five patients implanted with Rheos underwent a voltage response test (VRT) before the start of carotid baroreflex activation (1m), as well as after 4 (4m) and 13 months (13 m) of device implantation. After switching off the device for 10 min (0 V), we started the VRT by increasing voltage from 1 to 6 V, by 1-V steps every 5 min. Blood pressure and heart rate were measured at the end of every step. At 1m, mean blood pressure was 178/101 mmHg at 0 V and fell to 142/83 mmHg at 6 V. Heart rate fell from 75 to 65 beats/min. At 4m and 13 m mean blood pressure was significantly lower compared to 1m when VRT started at 0 V (170/96 and 161/93 mmHg, respectively). However, pattern of blood pressure decrease during VRT was comparable with this at 1m. Maximum SBP reduction during VRT did not change with long-term therapy. Acute voltage-dependent blood pressure and heart rate decrease with electrical baroreflex stimulation is preserved after at least 1 year of continuous activation in patients with resistant hypertension. This indicates that response adaptation and nerve fatigue are very unlikely in long-term carotid baroreflex activation.

  2. Possibility of a quasi-liquid layer of As on GaAs substrate grown by MBE as observed by enhancement of Ga desorption at high As pressure

    NASA Astrophysics Data System (ADS)

    Asai, K.; Feng, J. M.; Vaccaro, P. O.; Fujita, K.; Ohachi, T.

    2000-06-01

    The As vapor pressure dependence of the Ga desorption rate during molecular beam epitaxy (MBE) growth on GaAs( n11)A ( n=1-4 hereafter) substrates was studied by photoluminescence (PL) measurements at 12 K for undoped AlGaAs/GaAs asymmetric double quantum wells (ADQWs). Reflection high energy electron diffraction (RHEED) oscillation measurements on a GaAs(100) surface were also used. Two K-cells of As solid sources (corresponding to beam equivalent pressures (BEPs) of 9.0×10 -6 and 4.5×10 -5 Torr) were used to change the As pressure rapidly. The Ga flux and substrate temperature were kept constant at 0.76 ML/s and 12 K, respectively, while the As flux changed from 7.6 (BEP 9.0×10 -6 Torr) to 32 ML/s (4.5×10 -5 Torr). With increasing As pressure, two separated PL peaks for the wide well (WW) of high index substrates were observed. This peak separation is attributed to a reduced well depth from an increasing Ga desorption rate. The energy differences of the PL peak depending on the off-angle from (111)A to (100) plane indicates an orientation-dependent Ga desorption rate. Moreover, amongst all ( n11)A and (100) planes, the Ga desorption rate was smallest from the (111)A surface. The increase of Ga desorption from the surface at high As pressures probably arose from an increasing coverage with a quasi-liquid layer (QLL).

  3. The effect of baseline pressure errors on an intracranial pressure-derived index: results of a prospective observational study

    PubMed Central

    2014-01-01

    Background In order to characterize the intracranial pressure-volume reserve capacity, the correlation coefficient (R) between the ICP wave amplitude (A) and the mean ICP level (P), the RAP index, has been used to improve the diagnostic value of ICP monitoring. Baseline pressure errors (BPEs), caused by spontaneous shifts or drifts in baseline pressure, cause erroneous readings of mean ICP. Consequently, BPEs could also affect ICP indices such as the RAP where in the mean ICP is incorporated. Methods A prospective, observational study was carried out on patients with aneurysmal subarachnoid hemorrhage (aSAH) undergoing ICP monitoring as part of their surveillance. Via the same burr hole in the scull, two separate ICP sensors were placed close to each other. For each consecutive 6-sec time window, the dynamic mean ICP wave amplitude (MWA; measure of the amplitude of the single pressure waves) and the static mean ICP, were computed. The RAP index was computed as the Pearson correlation coefficient between the MWA and the mean ICP for 40 6-sec time windows, i.e. every subsequent 4-min period (method 1). We compared this approach with a method of calculating RAP using a 4-min moving window updated every 6 seconds (method 2). Results The study included 16 aSAH patients. We compared 43,653 4-min RAP observations of signals 1 and 2 (method 1), and 1,727,000 6-sec RAP observations (method 2). The two methods of calculating RAP produced similar results. Differences in RAP ≥0.4 in at least 7% of observations were seen in 5/16 (31%) patients. Moreover, the combination of a RAP of ≥0.6 in one signal and <0.6 in the other was seen in ≥13% of RAP-observations in 4/16 (25%) patients, and in ≥8% in another 4/16 (25%) patients. The frequency of differences in RAP >0.2 was significantly associated with the frequency of BPEs (5 mmHg ≤ BPE <10 mmHg). Conclusions Simultaneous monitoring from two separate, close-by ICP sensors reveals significant differences in RAP that

  4. The Influence of Observation Length on the Dependability of Data

    ERIC Educational Resources Information Center

    David Ferguson, Tyler; Briesch, Amy M.; Volpe, Robert J.; Daniels, Brian

    2012-01-01

    Although direct observation is one of the most frequently used assessment methods by school psychologists, studies have shown that the number of observations needed to obtain a dependable estimate of student behavior may be impractical. Because direct observation may be used to inform important decisions about students, it is crucial that data be…

  5. Observation of the pressure effect in simulations of droplets splashing on a dry surface

    NASA Astrophysics Data System (ADS)

    Boelens, A. M. P.; Latka, A.; de Pablo, J. J.

    2018-06-01

    At atmospheric pressure, a drop of ethanol impacting on a solid surface produces a splash. Reducing the ambient pressure below its atmospheric value suppresses this splash. The origin of this so-called pressure effect is not well understood, and this study presents an in-depth comparison between various theoretical models that aim to predict splashing and simulations. In this paper, the pressure effect is explored numerically by resolving the Navier-Stokes equations at a 3-nm resolution. In addition to reproducing numerous experimental observations, it is found that different models all provide elements of what is observed in the simulations. The skating droplet model correctly predicts the existence and scaling of a gas film under the droplet, the lamella formation theory is able to correctly predict the scaling of the lamella ejection velocity as a function of the impact velocity for liquids with different viscosity, and lastly, the dewetting theory's hypothesis of a lift force acting on the liquid sheet after ejection is consistent with our results.

  6. Temperature- and pressure-dependent infrared spectroscopy of 1-butyl-3-methylimidazolium trifluoromethanesulfonate: A dipolar coupling theory analysis

    NASA Astrophysics Data System (ADS)

    Burba, Christopher M.; Chang, Hai-Chou

    2018-03-01

    Continued growth and development of ionic liquids requires a thorough understanding of how cation and anion molecular structure defines the liquid structure of the materials as well as the various properties that make them technologically useful. Infrared spectroscopy is frequently used to assess molecular-level interactions among the cations and anions of ionic liquids because the intramolecular vibrational modes of the ions are sensitive to the local potential energy environments in which they reside. Thus, different interaction modes among the ions may lead to different spectroscopic signatures in the vibrational spectra. Charge organization present in ionic liquids, such as 1-butyl-3-methylimidazolium trifluoromethanesulfonate ([C4mim]CF3SO3), is frequently modeled in terms of a quasicrystalline structure. Highly structured quasilattices enable the dynamic coupling of vibrationally-induced dipole moments to produce optical dispersion and transverse optical-longitudinal optical (TO-LO) splitting of vibrational modes of the ionic liquid. According to dipolar coupling theory, the degree of TO-LO splitting is predicted to have a linear dependence on the number density of the ionic liquid. Both temperature and pressure will affect the number density of the ionic liquid and, therefore, the amount of TO-LO splitting for this mode. Therefore, we test these relationships through temperature- and pressure-dependent FT-IR spectroscopic studies of [C4mim]CF3SO3, focusing on the totally symmetric Ssbnd O stretching mode for the anion, νs(SO3). Increased temperature decreases the amount of TO-LO splitting for νs(SO3), whereas elevated pressure is found to increase the amount of band splitting. In both cases, the experimental observations follow the general predictions of dipolar coupling theory, thereby supporting the quasilattice model for this ionic liquid.

  7. Gas-pressure dependence of terahertz-pulse generation in a laser-generated nitrogen plasma

    NASA Astrophysics Data System (ADS)

    Löffler, T.; Roskos, H. G.

    2002-03-01

    Far-infrared (terahertz) pulses can be generated by photoionization of electrically biased gases with amplified laser pulses [T. Löffler, F. Jacob, and H. G. Roskos, Appl. Phys. Lett. 77, 453 (2000)]. The efficiency of the generation process can be significantly increased when the absolute gas pressure is raised because it is then possible to apply higher bias fields close to the dielectric breakdown field of the gas which increases with the pressure. The dependence of the THz output on the optical pump power does not show any indication of saturation, making the plasma emitter an interesting source for THz pulses especially in conjunction with terawatt laser systems.

  8. Options for Dealing with Pressure Dependence of Pulse Wave Velocity as a Measure of Arterial Stiffness: An Update of Cardio-Ankle Vascular Index (CAVI) and CAVI0.

    PubMed

    Spronck, Bart; Delhaas, Tammo; Butlin, Mark; Reesink, Koen D; Avolio, Alberto P

    2018-03-01

    Pulse wave velocity (PWV), a marker of arterial stiffness, is known to change instantaneously with changes in blood pressure. In this mini-review, we discuss two main approaches for handling the blood pressure dependence of PWV: (1) converting PWV into a pressure-independent index, and (2) correcting PWV per se for the pressure dependence. Under option 1, we focus on cardio-ankle vascular index (CAVI). CAVI is essentially a form of stiffness index β - CAVI is estimated for a (heart-to-ankle) trajectory, whereas β is estimated for a single artery from pressure and diameter measurements. Stiffness index β, and therefore also CAVI, have been shown to theoretically exhibit a slight residual blood pressure dependence due to the use of diastolic blood pressure instead of a fixed reference blood pressure. Additionally, CAVI exhibits pressure dependence due to the use of an estimated derivative of the pressure-diameter relationship. In this mini-review, we will address CAVI's blood pressure dependence theoretically, but also statistically. Furthermore, we review corrected indices (CAVI 0 and β 0 ) that theoretically do not show a residual blood pressure dependence. Under option 2, three ways of correcting PWV are reviewed: (1) using an exponential relationship between pressure and cross-sectional area, (2) by statistical model adjustment, and (3) through reference values or rule of thumb. Method 2 requires a population to be studied to characterise the statistical model, and method 3 requires a representative reference study. Given these limitations, method 1 seems preferable for correcting PWV per se for its blood pressure dependence. In summary, several options are available to handle the blood pressure dependence of PWV. If a blood pressure-independent index is sought, CAVI 0 is theoretically preferable over CAVI. If correcting PWV per se is required, using an exponential pressure-area relationship provides the user with a method to correct PWV on an individual

  9. Measurement of vacuum pressure with a magneto-optical trap: A pressure-rise method

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

    Moore, Rowan W. G.; Lee, Lucie A.; Findlay, Elizabeth A.

    2015-09-15

    The lifetime of an atom trap is often limited by the presence of residual background gases in the vacuum chamber. This leads to the lifetime being inversely proportional to the pressure. Here, we use this dependence to estimate the pressure and to obtain pressure rate-of-rise curves, which are commonly used in vacuum science to evaluate the performance of a system. We observe different rates of pressure increase in response to different levels of outgassing in our system. Therefore, we suggest that this is a sensitive method which will find useful applications in cold atom systems, in particular, where the inclusionmore » of a standard vacuum gauge is impractical.« less

  10. Frequency-dependent baroreflex control of blood pressure and heart rate during physical exercise.

    PubMed

    Spadacini, Giammario; Passino, Claudio; Leuzzi, Stefano; Valle, Felice; Piepoli, Massimo; Calciati, Alessandro; Sleight, Peter; Bernardi, Luciano

    2006-02-15

    It is widely recognised that during exercise vagal heart rate control is markedly impaired but blood pressure control may or may not be retained. We hypothesised that this uncertainty arose from the differing responses of the vagus (fast) and sympathetic (slow) arms of the autonomic effectors, and to differing sympatho-vagal balance at different exercise intensities. We studied 12 normals at rest, during moderate (50% maximal heart rate) and submaximal (80% maximal heart rate) exercise. The carotid baroreceptors were stimulated by sinusoidal neck suction at the frequency of the spontaneous high- (during moderate exercise) and low-frequency (during submaximal) fluctuations in heart period and blood pressure. The increases in these oscillations induced by neck suction were measured by autoregressive spectral analysis. At rest neck stimulation increased variability at low frequency (RR: from 6.99+/-0.24 to 8.87+/-0.18 ln-ms2; systolic pressure: from 3.05+/-1.7 to 4.09+/-0.17 ln-mm Hg2) and high frequency (RR: from 4.67+/-0.25 to 6.79+/-0.31 ln-ms2; systolic pressure: from 1.93+/-0.2 to 2.67+/-0.125 ln-mm Hg2) (all p<0.001). During submaximal exercise RR variability decreased but systolic pressure variability rose (p<0.01 vs rest); during submaximal exercise low-frequency neck stimulation increased the low-frequency fluctuations in blood pressure (2.35+/-0.51 to 4.25+/-0.38 ln-mm Hg2, p<0.05) and RR. Conversely, neck suction at high frequency was ineffective on systolic pressure, and had only minor effects on RR interval during moderate exercise. During exercise baroreflex control is active on blood pressure, but the efferent response on blood pressure and heart rate is only detected during low frequency stimulation, indicating a frequency-dependent effect.

  11. On the pressure and temperature dependent ductile, brittle nature of SmS1-xSex semiconductor

    NASA Astrophysics Data System (ADS)

    Shriya, S.; Khan, E.; Khenata, R.; Varshney, Dinesh

    2018-04-01

    The high-pressure structural phase transition and pressure as well temperature induced elastic properties of rocksalt to CsCl structures of SmS1-xSex (x = 0, 0.11, 0.44, 1) compound have been performed using effective interionic interaction potential with emphasis on charge transfer interactions and covalent contribution. Estimated values of phase transition pressure and the volume discontinuity in pressure-volume phase diagram indicate the structural phase transition from ZnS to NaCl structure. From the investigations of elastic constants the pressure (temperature) dependent volume collapse/expansion, melting temperature TM, Hardness (HV), Poisson's ratio ν and Pugh ratio ϕ (= BT/GH) the SmS1-xSex (x = 0, 0.11, 0.44, 1) lattice infers mechanical stiffening, thermal softening, and ductile (brittle) nature.

  12. Redox Signaling via Oxidative Inactivation of PTEN Modulates Pressure-Dependent Myogenic Tone in Rat Middle Cerebral Arteries

    PubMed Central

    Gebremedhin, Debebe; Terashvili, Maia; Wickramasekera, Nadi; Zhang, David X.; Rau, Nicole; Miura, Hiroto; Harder, David R.

    2013-01-01

    The present study examined the level of generation of reactive oxygen species (ROS) and roles of inactivation of the phosphatase PTEN and the PI3K/Akt signaling pathway in response to an increase in intramural pressure-induced myogenic cerebral arterial constriction. Step increases in intraluminal pressure of cannulated cerebral arteries induced myogenic constriction and concomitant formation of superoxide (O2 .−) and its dismutation product hydrogen peroxide (H2O2) as determined by fluorescent HPLC analysis, microscopic analysis of intensity of dihydroethidium fluorescence and attenuation of pressure-induced myogenic constriction by pretreatment with the ROS scavenger 4,hydroxyl-2,2,6,6-tetramethylpiperidine1-oxyl (tempol) or Mito-tempol or MitoQ in the presence or absence of PEG-catalase. An increase in intraluminal pressure induced oxidation of PTEN and activation of Akt. Pharmacological inhibition of endogenous PTEN activity potentiated pressure-dependent myogenic constriction and caused a reduction in NPo of a 238 pS arterial KCa channel current and an increase in [Ca2+]i level in freshly isolated cerebral arterial muscle cells (CAMCs), responses that were attenuated by Inhibition of the PI3K/Akt pathway. These findings demonstrate an increase in intraluminal pressure induced increase in ROS production triggered redox-sensitive signaling mechanism emanating from the cross-talk between oxidative inactivation of PTEN and activation of the PI3K/Akt signaling pathway that involves in the regulation of pressure-dependent myogenic cerebral arterial constriction. PMID:23861911

  13. Redox signaling via oxidative inactivation of PTEN modulates pressure-dependent myogenic tone in rat middle cerebral arteries.

    PubMed

    Gebremedhin, Debebe; Terashvili, Maia; Wickramasekera, Nadi; Zhang, David X; Rau, Nicole; Miura, Hiroto; Harder, David R

    2013-01-01

    The present study examined the level of generation of reactive oxygen species (ROS) and roles of inactivation of the phosphatase PTEN and the PI3K/Akt signaling pathway in response to an increase in intramural pressure-induced myogenic cerebral arterial constriction. Step increases in intraluminal pressure of cannulated cerebral arteries induced myogenic constriction and concomitant formation of superoxide (O2 (.-)) and its dismutation product hydrogen peroxide (H2O2) as determined by fluorescent HPLC analysis, microscopic analysis of intensity of dihydroethidium fluorescence and attenuation of pressure-induced myogenic constriction by pretreatment with the ROS scavenger 4,hydroxyl-2,2,6,6-tetramethylpiperidine1-oxyl (tempol) or Mito-tempol or MitoQ in the presence or absence of PEG-catalase. An increase in intraluminal pressure induced oxidation of PTEN and activation of Akt. Pharmacological inhibition of endogenous PTEN activity potentiated pressure-dependent myogenic constriction and caused a reduction in NPo of a 238 pS arterial KCa channel current and an increase in [Ca(2+)]i level in freshly isolated cerebral arterial muscle cells (CAMCs), responses that were attenuated by Inhibition of the PI3K/Akt pathway. These findings demonstrate an increase in intraluminal pressure induced increase in ROS production triggered redox-sensitive signaling mechanism emanating from the cross-talk between oxidative inactivation of PTEN and activation of the PI3K/Akt signaling pathway that involves in the regulation of pressure-dependent myogenic cerebral arterial constriction.

  14. Rapid thermal responsive conductive hybrid cryogels with shape memory properties, photothermal properties and pressure dependent conductivity.

    PubMed

    Deng, Zexing; Guo, Yi; Ma, Peter X; Guo, Baolin

    2018-09-15

    Stimuli responsive cryogels with multi-functionality have potential application for electrical devices, actuators, sensors and biomedical devices. However, conventional thermal sensitive poly(N-isopropylacrylamide) cryogels show slow temperature response speed and lack of multi-functionality, which greatly limit their practical application. Herein we present conductive fast (2 min for both deswelling and reswelling behavior) thermally responsive poly(N-isopropylacrylamide) cryogels with rapid shape memory properties (3 s for shape recovery), near-infrared (NIR) light sensitivity and pressure dependent conductivity, and further demonstrated their applications as temperature sensitive on-off switch, NIR light sensitive on-off switch, water triggered shape memory on-off switch and pressure dependent device. These cryogels were first prepared in dimethyl sulfoxide below its melting temperature in ice bath and subsequently put into aniline or pyrrole solution to in situ deposition of conducting polyaniline or polypyrrole nanoparticles. The continuous macroporous sponge-like structure provides cryogels with rapid responsivity both in deswelling, reswelling kinetics and good elasticity. After incorporating electrically conductive polyaniline or polypyrrole nanoaggregates, the hybrid cryogels exhibit desirable conductivity, photothermal property, pressure dependent conductivity and good cytocompatibility. These multifunctional hybrid cryogels make them great potential as stimuli responsive electrical device, tissue engineering scaffolds, drug delivery vehicle and electronic skin. Copyright © 2018 Elsevier Inc. All rights reserved.

  15. In situ observations of a high-pressure phase of H2O ice

    USGS Publications Warehouse

    Chou, I.-Ming; Blank, J.G.; Goncharov, A.F.; Mao, Ho-kwang; Hemley, R.J.

    1998-01-01

    A previously unknown solid phase of H2O has been identified by its peculiar growth patterns, distinct pressure-temperature melting relations, and vibrational Raman spectra. Morphologies of ice crystals and their pressure-temperature melting relations were directly observed in a hydrothermal diamond-anvil cell for H2O bulk densities between 1203 and 1257 kilograms per cubic meter at temperatures between -10??and 50??C. Under these conditions, four different ice forms were observed to melt: two stable phases, ice V and ice VI, and two metastable phases, ice IV and the new ice phase. The Raman spectra and crystal morphology are consistent with a disordered anisotropic structure with some similarities to ice VI.

  16. Using the Care Dependency Scale for identifying patients at risk for pressure ulcer.

    PubMed

    Dijkstra, Ate; Kazimier, Hetty; Halfens, Ruud J G

    2015-11-01

    The aim of this study was to evaluate risk screening for pressure ulcer by using the Care Dependency Scale (CDS) for patients receiving home care or admitted to a residential or nursing home in the Netherlands. Pressure ulcer is a serious and persistent problem for patients throughout the Western world. Pressure ulcer is among the most common adverse events in nursing practice and when a pressure ulcer occurs it has many consequences for patients and healthcare professionals. Cross-sectional design. The convenience sample consisted of 13,633 study participants, of whom 2639 received home care from 15 organisations, 4077 were patients from 67 residential homes and 6917 were admitted in 105 nursing homes. Data were taken from the Dutch National Prevalence Survey of Care Problems that was carried out in April 2012 in Dutch healthcare settings. For the three settings, cut-off points above 80% sensitivity were established, while in the residential home sample an almost 60% combined specificity score was identified. The CDS items 'Body posture' (home care), 'Getting dressed and undressed' (residential homes) and 'Mobility' (nursing homes) were the most significant variables which affect PU. The CDS is able to distinguish between patients at risk for pressure ulcer development and those not at risk in both home care and residential care settings. In nursing homes, the usefulness of the CDS for pressure ulcer detection is limited. © 2015 John Wiley & Sons Ltd.

  17. Temperature-(208-318 K) and pressure-(18-696 Torr) dependent rate coefficients for the reaction between OH and HNO3

    NASA Astrophysics Data System (ADS)

    Dulitz, Katrin; Amedro, Damien; Dillon, Terry J.; Pozzer, Andrea; Crowley, John N.

    2018-02-01

    Rate coefficients (k5) for the title reaction were obtained using pulsed laser photolytic generation of OH coupled to its detection by laser-induced fluorescence (PLP-LIF). More than 80 determinations of k5 were carried out in nitrogen or air bath gas at various temperatures and pressures. The accuracy of the rate coefficients obtained was enhanced by in situ measurement of the concentrations of both HNO3 reactant and NO2 impurity. The rate coefficients show both temperature and pressure dependence with a rapid increase in k5 at low temperatures. The pressure dependence was weak at room temperature but increased significantly at low temperatures. The entire data set was combined with selected literature values of k5 and parameterised using a combination of pressure-dependent and -independent terms to give an expression that covers the relevant pressure and temperature range for the atmosphere. A global model, using the new parameterisation for k5 rather than those presently accepted, indicated small but significant latitude- and altitude-dependent changes in the HNO3 / NOx ratio of between -6 and +6 %. Effective HNO3 absorption cross sections (184.95 and 213.86 nm, units of cm2 molecule-1) were obtained as part of this work: σ213.86 = 4.52-0.12+0.23 × 10-19 and σ184.95 = 1.61-0.04+0.08 × 10-17.

  18. Polarization-dependent infrared reflectivity study of Sr 2.5 Ca 11.5 Cu 24 O 41 under pressure: Charge dynamics, charge distribution, and anisotropy

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

    Frank, S.; Huber, A.; Ammerahl, U.

    2014-12-18

    We present a polarization-dependent infrared reflectivity study of the spin-ladder compound Sr₂̣₅Ca₁₁̣₅Cu₂₄O₄₁ under pressure. The optical response is strongly anisotropic, with the highest reflectivity along the ladders/chains ( E∥c) revealing a metallic character. For the polarization direction perpendicular to the ladder plane, an insulating behavior is observed. With increasing pressure the optical conductivity for E∥c shows a strong increase, which is most pronounced below 2000cm⁻¹. According to the spectral weight analysis of the E∥c optical conductivity the hole concentration in the ladders increases with increasing pressure and tends to saturate at high pressure. At ~7.5 GPa the number of holesmore » per Cu atom in the ladders has increased by Δδ=0.09(±0.01), and the Cu valence in the ladders has reached the value +2.33. Thus, the optical data suggest that Sr₂̣₅Ca₁₁̣₅Cu₂₄O₄₁ remains electronically highly anisotropic up to high pressure, also at low temperatures.« less

  19. NOS3 genotype-dependent correlation between blood pressure and physical activity.

    PubMed

    Kimura, Tomomi; Yokoyama, Tetsuji; Matsumura, Yasuhiro; Yoshiike, Nobuo; Date, Chigusa; Muramatsu, Masaaki; Tanaka, Heizo

    2003-02-01

    Endothelium-dependent vasorelaxation plays an important role in reduction of blood pressure and is mediated through release of nitric oxide (NO), which is generated by constitutively expressed endothelial nitric oxide synthase (NOS3). Exercise also augments NO release and has been recommended for primary prevention and improvement of hypertension, but individual responses are highly variable. We therefore postulated that genetic polymorphisms of NOS3 might interact with physical activity level to differentially influence blood pressure level. We genotyped 832 healthy Japanese (mean age of 54.4+/-8.6 years, 372 men and 460 women) for a polymorphism of NOS3 in intron 4 (ecNOS4a/b), using the polymerase chain reaction method, and scored their habitual physical activity level by using the rate of energy expenditure per resting metabolic rate through an interview according to a semiquantitative assessment method. Only in the subjects who had the rarer a allele (aa+ba type), systolic blood pressure was found to be inversely correlated with physical activity level (P for linear trend=0.0496, for interaction=0.0071). Eventually, this polymorphism was significantly associated with the prevalence of systolic hypertension only in the subjects who were in the lowest tertile of physical activity level (OR=2.4, 95% CI, 1.1 to 5.6, P for interaction=0.0474). In the present study, we found a significant interaction between the genotype and physical activity level on systolic blood pressure. These results might allow a better understanding of the mechanism to improve hypertension by exercise and to thereby reduce the risk of cardiovascular disease.

  20. Pressure dependence of transverse acoustic phonon energy in ferropericlase across the spin transition.

    PubMed

    Fukui, Hiroshi; Baron, Alfred Q R; Ishikawa, Daisuke; Uchiyama, Hiroshi; Ohishi, Yasuo; Tsuchiya, Taku; Kobayashi, Hisao; Matsuzaki, Takuya; Yoshino, Takashi; Katsura, Tomoo

    2017-06-21

    We investigated transverse acoustic (TA) phonons in iron-bearing magnesium oxide (ferropericlase) up to 56 GPa using inelastic x-ray scattering (IXS). The results show that the energy of the TA phonon far from the Brillouin zone center suddenly increases with increasing pressure above the spin transition pressure of ferropericlase. Ab initio calculations revealed that the TA phonon energy far from the Brillouin zone center is higher in the low-spin state than in the high spin state; that the TA phonon energy depend weakly on pressure; and that the energy gap between the TA and the lowest-energy-optic phonons is much narrower in the low-spin state than in the high-spin state. This allows us to conclude that the anomalous behavior of the TA mode in the present experiments is the result of gap narrowing due to the spin transition and explains contradictory results in previous experimental studies.

  1. Polaron physics and crossover transition in magnetite probed by pressure-dependent infrared spectroscopy.

    PubMed

    Ebad-Allah, J; Baldassarre, L; Sing, M; Claessen, R; Brabers, V A M; Kuntscher, C A

    2013-01-23

    The optical properties of magnetite at room temperature were studied by infrared reflectivity measurements as a function of pressure up to 8 GPa. The optical conductivity spectrum consists of a Drude term, two sharp phonon modes, a far-infrared band at around 600 cm(-1) and a pronounced mid-infrared absorption band. With increasing pressure both absorption bands shift to lower frequencies and the phonon modes harden in a linear fashion. Based on the shape of the MIR band, the temperature dependence of the dc transport data, and the occurrence of the far-infrared band in the optical conductivity spectrum, the polaronic coupling strength in magnetite at room temperature should be classified as intermediate. For the lower energy phonon mode an abrupt increase of the linear pressure coefficient occurs at around 6 GPa, which could be attributed to minor alterations of the charge distribution among the different Fe sites.

  2. Pressure dependence of the refractive index and dielectric constant in a fluoroperovskite, KMgF3

    NASA Astrophysics Data System (ADS)

    Uchino, Kenji; Nomura, Shoichiro; Vedam, K.; Newnham, Robert E.; Cross, Leslie E.

    1984-06-01

    The hydrostatic-pressure dependence of the refractive index and the low-frequency dielectric constant of a perovskite-type single crystal, KMgF3, have been determined at room temperature. The refractive index n for λ=589.3 nm increases monotonously in proportion to pressure p with a slope of ∂n∂p=2.46×10-4kbar-1. On the other hand, the dielectric constant at 10 kHz decreases with increasing pressure, from which the electric-displacement-related electrostrictive coefficient Qh (=Q11+2Q12) is calculated as 0.24 m4 C-2. These data are compared with the ∂n∂p values and the Qh coefficients of various alkali fluorides and perovskite oxides.

  3. Reliability of laser Doppler flowmetry curve reading for measurement of toe and ankle pressures: intra- and inter-observer variation.

    PubMed

    Høyer, C; Paludan, J P D; Pavar, S; Biurrun Manresa, J A; Petersen, L J

    2014-03-01

    To assess the intra- and inter-observer variation in laser Doppler flowmetry curve reading for measurement of toe and ankle pressures. A prospective single blinded diagnostic accuracy study was conducted on 200 patients with known or suspected peripheral arterial disease (PAD), with a total of 760 curve sets produced. The first curve reading for this study was performed by laboratory technologists blinded to clinical clues and previous readings at least 3 months after the primary data sampling. The pressure curves were later reassessed following another period of at least 3 months. Observer agreement in diagnostic classification according to TASC-II criteria was quantified using Cohen's kappa. Reliability was quantified using intra-class correlation coefficients, coefficients of variance, and Bland-Altman analysis. The overall agreement in diagnostic classification (PAD/not PAD) was 173/200 (87%) for intra-observer (κ = .858) and 175/200 (88%) for inter-observer data (κ = .787). Reliability analysis confirmed excellent correlation for both intra- and inter-observer data (ICC all ≥.931). The coefficients of variance ranged from 2.27% to 6.44% for intra-observer and 2.39% to 8.42% for inter-observer data. Subgroup analysis showed lower observer-variation for reading of toe pressures in patients with diabetes and/or chronic kidney disease than patients not diagnosed with these conditions. Bland-Altman plots showed higher variation in toe pressure readings than ankle pressure readings. This study shows substantial intra- and inter-observer agreement in diagnostic classification and reading of absolute pressures when using laboratory technologists as observers. The study emphasises that observer variation for curve reading is an important factor concerning the overall reproducibility of the method. Our data suggest diabetes and chronic kidney disease have an influence on toe pressure reproducibility. Copyright © 2013 European Society for Vascular Surgery. Published

  4. [Topic efficacy of ialuronic acid associated with argentic sulphadiazine (Connettivina Plus) in the treatment of pressure sores: a prospective observational cohort study].

    PubMed

    Paghetti, Angela; Bellingeri, Andrea; Pomponio, Giovanni; Sansoni, Julita; Paladino, Dario

    2009-01-01

    The aim of this observational study was to evaluate the efficacy, tolerability and methods of application of ialuronic acid associated with argentic sulphadiazine (Connettivina Plus) in routine clinical activity, on a target of "complex" patients with pressure sores, for the most realistic assessment possible. The study comprised 127 patients hospitalized between January 2006 and December 2007, who received ialuronic acid associated with argentic sulphadiazine in addition to the standard treatment. Inclusion criteria were th presence of at least one stage 2 or 3 pressure sore (NPUAP '89 classification), pressure sore that the researcher had already decided to treat using ialuronic acid associated with argentic sulphadiazine , according to hospital protocol, area of the lesion less than 25cm2, patient age 18 years or more, informed patient consensus. Patients with these characteristics were , however, excluded if they did not provide written consent or if they had one of the following: presence of pressure sores with escara, concomitant neoplastic disease, concomitant insulin-dependent diabetes or other pathologies that interfere with skin regeneration, allergic diasthesis (acclaimed or presumed) to ialuronic acid - argentic sulphadiazine, inability / refusal to undergo all the subsequent controls required by the study. Improvement or complete healing of the pressure sores was observed in 67% of patients at early follow-up (10 days), increasing to 76% and 87% at 20 and 35 day controls respectively. The Push tool further improved in patients who carried on treatment. Use of ialuronic acid associated with argentic sulphadiazine was effective for treating grade 2-3 pressure sores in patients with chronic lesions and its efficacy was confirmed in association with both advanced and traditional types of medication.

  5. Copernicus observations of C I: pressures and carbon abundances in diffuse interstellar clouds

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

    Jenkins, E.B.; Jura, M.; Loewenstein, M.

    1983-07-01

    Using the Copernicus satellite, we observed ultraviolet absorption lines of interstellar neutral carbon atoms toward 27 stars. In addition to deriving column densities of C I (both in its ground state and the two excited fine-structure levels), we used our equivalent widths to revise the f-values of some of the C I transitions measured by other investigators. We also observed H/sub 2/ from the J = 4 level so that we could compare the rotational excitation of H/sub 2/ with the fine-structure excitation of C I. From the amount of fine-structure excitation of C I in each case, we havemore » derived information on the thermal gas pressures within the diffuse clouds. Most clouds have p/k between 10/sup 3/ cm/sup -3/ K and 10/sup 4/ cm/sup -3/ K, but we found that at least 6% of the C I-bearing material is at p/k>10/sup 4/ cm/sup -3/ K, and one-third of the gas has upper limits for pressure below 10/sup 3/ cm/sup -3/ K, assuming temperatures are not appreciably below 20 K. An analysis of radial velocities for the absorption lines showed no distinctive trends for the kinematics of high- or low-pressure gas components. From the apparent lack of acceleration of high-pressure clouds, we conclude that it is unlikely that streaming intercloud material is causing significant ram pressurization. We have compared our results with the predictions for pressure fluctuations caused by supernova explosions in the theory of McKee and Ostriker.« less

  6. TIME DEPENDENT NONEQUILIBRIUM IONIZATION OF TRANSITION REGION LINES OBSERVED WITH IRIS

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

    Martínez-Sykora, Juan; Pontieu, Bart De; Hansteen, Viggo H.

    The properties of nonstatistical equilibrium ionization of silicon and oxygen ions are analyzed in this work. We focus on five solar targets (quiet Sun; coronal hole; plage; quiescent active region, AR; and flaring AR) as observed with the Interface Region Imaging Spectrograph (IRIS). IRIS is best suited for this work owing to the high cadence (up to 0.5 s), high spatial resolution (up to 0.″32), and high signal-to-noise ratios for O iv λ1401 and Si iv λ1402. We find that the observed intensity ratio between lines of three times ionized silicon and oxygen ions depends on their total intensity and that this correlationmore » varies depending on the region observed (quiet Sun, coronal holes, plage, or active regions) and on the specific observational objects present (spicules, dynamic loops, jets, microflares, or umbra). In order to interpret the observations, we compare them with synthetic profiles taken from 2D self-consistent radiative MHD simulations of the solar atmosphere, where the statistical equilibrium or nonequilibrium treatment of silicon and oxygen is applied. These synthetic observations show vaguely similar correlations to those in the observations, i.e., between the intensity ratios and their intensities, but only in the nonequilibrium case do we find that (some of) the observations can be reproduced. We conclude that these lines are formed out of statistical equilibrium. We use our time-dependent nonequilibrium ionization simulations to describe the physical mechanisms behind these observed properties.« less

  7. Effects of pressure distribution on parallel circular porous plates with combined effect of piezo-viscous dependency and non-Newtonian couple stress fluid

    NASA Astrophysics Data System (ADS)

    Vijayakumar, B.; Kesavan, Sundarammal

    2018-04-01

    Piezo-viscous effect i.e., Viscosity-pressure dependency has an important part in the applications of fluid flows like fluid lubrication, micro fluidics and geophysics. In this paper, the joint effects of piezo-viscous dependency and non-Newtonian couple stresses on the performance of circular porous plate’s squeeze film bearing have been studied. The results for pressure with various values of viscosity-pressure parameters are numerically calculated and compared with iso-viscous couple stress and Newtonian lubricants. Due to piezo-viscous effect, the pressure with piezo-viscous Non-Newtonian is significantly higher than the pressure with iso-viscous Newtonian and iso-viscous Non-Newtonian fluid.

  8. Anomalous pressure dependence of magnetic ordering temperature in Tb revealed by resistivity measurements to 141 GPa. Comparison with Gd and Dy

    DOE PAGES

    Lim, J.; Fabbris, G.; Haskel, D.; ...

    2015-05-26

    In previous studies the pressure dependence of the magnetic ordering temperature T o of Dy was found to exhibit a sharp increase above its volume collapse pressure of 73 GPa, appearing to reach temperatures well above ambient at 157 GPa. In a search for a second such lanthanide, electrical resistivity measurements were carried out on neighboring Tb to 141 GPa over the temperature range 3.8 - 295 K. Below Tb’s volume collapse pressure of 53 GPa, the pressure dependence T o(P) mirrors that of both Dy and Gd. However, at higher pressures T o(P) for Tb becomes highly anomalous. Thismore » result, together with the very strong suppression of superconductivity by dilute Tb ions in Y, suggests that extreme pressure transports Tb into an unconventional magnetic state with an anomalously high magnetic ordering temperature.« less

  9. Excitation Location and Seasonal Variation of Transoceanic Infragravity Waves Observed at an Absolute Pressure Gauge Array

    NASA Astrophysics Data System (ADS)

    Tonegawa, T.; Fukao, Y.; Shiobara, H.; Sugioka, H.; Ito, A.; Yamashita, M.

    2018-01-01

    An array of 10 absolute pressure gauges (APGs) deployed in deep water 50 km east of Aogashima, an island in southern Japan, observed several isolated signals in the infragravity wave (IGW) frequency band (0.002-0.03 Hz) during boreal summer, whereas relatively high IGW energy persisted during boreal winter. The isolated IGW shows dispersion with a delay time of 4-5 days as a function of frequency. Here we estimate the excitation locations of IGWs for the two seasons with estimated incoming direction of IGW, calculation of transoceanic IGW trajectories and propagation times, and spatiotemporal variations of significant wave heights from WAVEWATCH III. In boreal summer, the isolated IGWs are primarily caused by IGW energies excited at the shoreline of South America, based on the following three observations: IGWs observed at the array originated from the east: the easterly ray path from the array reaches South America: and an event-like IGWs were observed at the array when a storm approaches eastward to the shoreline of South America, in which the observed delay time of 4-5 days was also supported by the frequency-dependent calculation of IGW propagation times. In boreal winter, the incessant IGWs consist of transoceanic IGW energies leaked from the shoreline, primarily from North America, and secondly from South America and the western Aleutian Islands.

  10. Charge dependence of the plasma travel length in atmospheric-pressure plasma

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

    Yambe, Kiyoyuki; Konda, Kohmei; Masuda, Seiya

    Plasma plume is generated using a quartz tube, helium gas, and foil electrode by applying AC high voltage under the atmosphere. The plasma plume is released into the atmosphere from inside of the quartz tube and is seen as the continuous movement of the plasma bullet. The travel length of plasma bullet is defined from plasma energy and force due to electric field. The drift velocity of plasma bullet has the upper limit under atmospheric-pressure because the drift velocity is determined from the balance between electric field and resistive force due to collisions between plasma and air. The plasma plumemore » charge depends on the drift velocity. Consequently, in the laminar flow of helium gas flow state, the travel length of the plasma plume logarithmically depends on the plasma plume charge which changes with both the electric field and the resistive force.« less

  11. Monocyte-derived extracellular Nampt-dependent biosynthesis of NAD+ protects the heart against pressure overload

    PubMed Central

    Yano, Masamichi; Akazawa, Hiroshi; Oka, Toru; Yabumoto, Chizuru; Kudo-Sakamoto, Yoko; Kamo, Takehiro; Shimizu, Yu; Yagi, Hiroki; Naito, Atsuhiko T.; Lee, Jong-Kook; Suzuki, Jun-ichi; Sakata, Yasushi; Komuro, Issei

    2015-01-01

    Nicotinamide phosphoribosyltransferase (Nampt) catalyzes the rate-limiting step in the salvage pathway for nicotinamide adenine dinucleotide (NAD+) biosynthesis, and thereby regulates the deacetylase activity of sirtuins. Here we show accommodative regulation of myocardial NAD+ by monocyte-derived extracellular Nampt (eNampt), which is essential for hemodynamic compensation to pressure overload. Although intracellular Nampt (iNampt) expression was decreased in pressure-overloaded hearts, myocardial NAD+ concentration and Sirt1 activity were preserved. In contrast, iNampt was up-regulated in spleen and monocytes, and circulating eNampt protein and nicotinamide mononucleotide (NMN), a key precursor of NAD+, were significantly increased. Pharmacological inhibition of Nampt by FK866 or depletion of monocytes/macrophages by clodronate liposomes disrupted the homeostatic mechanism of myocardial NAD+ levels and NAD+-dependent Sirt1 activity, leading to susceptibility to cardiomyocyte apoptosis and cardiac decompensation in pressure-overloaded mice. These biochemical and hemodynamic defects were prevented by systemic administration of NMN. Our studies uncover a crucial role of monocyte-derived eNampt in myocardial adaptation to pressure overload, and highlight a potential intervention controlling myocardial NAD+ against heart failure. PMID:26522369

  12. Polarized pressure dependence of the anisotropic dielectric functions of highly oriented poly(p-phenylene vinylene)

    NASA Astrophysics Data System (ADS)

    Morandi, V.; Galli, M.; Marabelli, F.; Comoretto, D.

    2010-04-01

    In this work, we combined an experimental technique and a detailed data analysis to investigate the influence of an applied pressure on the anisotropic dielectric functions of highly oriented poly(p-phenylene vinylene) (PPV). The dielectric constants were derived from polarized reflectance spectra recorded through a diamond anvil cell up to 50 kbar. The presence of the diamond anvils strongly affects measured spectra requiring the development in an optical model able to take all spurious effects into account. A parametric procedure was then applied to derive the complex dielectric constants for both polarizations as a function of pressure. A detailed analysis of their pressure dependence allows addressing the role of intermolecular interactions and electron-phonon coupling in highly oriented PPV.

  13. The functional dependence of canopy conductance on water vapor pressure deficit revisited

    NASA Astrophysics Data System (ADS)

    Fuchs, Marcel; Stanghellini, Cecilia

    2018-03-01

    Current research seeking to relate between ambient water vapor deficit (D) and foliage conductance (g F ) derives a canopy conductance (g W ) from measured transpiration by inverting the coupled transpiration model to yield g W = m - n ln(D) where m and n are fitting parameters. In contrast, this paper demonstrates that the relation between coupled g W and D is g W = AP/D + B, where P is the barometric pressure, A is the radiative term, and B is the convective term coefficient of the Penman-Monteith equation. A and B are functions of g F and of meteorological parameters but are mathematically independent of D. Keeping A and B constant implies constancy of g F . With these premises, the derived g W is a hyperbolic function of D resembling the logarithmic expression, in contradiction with the pre-set constancy of g F . Calculations with random inputs that ensure independence between g F and D reproduce published experimental scatter plots that display a dependence between g W and D in contradiction with the premises. For this reason, the dependence of g W on D is a computational artifact unrelated to any real effect of ambient humidity on stomatal aperture and closure. Data collected in a maize field confirm the inadequacy of the logarithmic function to quantify the relation between canopy conductance and vapor pressure deficit.

  14. Generalized Doppler and aberration kernel for frequency-dependent cosmological observables

    NASA Astrophysics Data System (ADS)

    Yasini, Siavash; Pierpaoli, Elena

    2017-11-01

    We introduce a frequency-dependent Doppler and aberration transformation kernel for the harmonic multipoles of a general cosmological observable with spin weight s , Doppler weight d and arbitrary frequency spectrum. In the context of cosmic microwave background (CMB) studies, the frequency-dependent formalism allows to correct for the motion-induced aberration and Doppler effects on individual frequency maps with different masks. It also permits to deboost background radiations with non-blackbody frequency spectra, like extragalactic foregrounds and CMB spectra with primordial spectral distortions. The formalism can also be used to correct individual E and B polarization modes and account for motion-induced E/B mixing of polarized observables with d ≠1 at different frequencies. We apply the generalized aberration kernel on polarized and unpolarized specific intensity at 100 and 217 GHz and show that the motion-induced effects typically increase with the frequency of observation. In all-sky CMB experiments, the frequency-dependence of the motion-induced effects for a blackbody spectrum are overall negligible. However in a cut-sky analysis, ignoring the frequency dependence can lead to percent level error in the polarized and unpolarized power spectra over all angular scales. In the specific cut-sky used in our analysis (b >4 5 ° ,fsky≃14 % ), and for the dipole-inferred velocity β =0.00123 typically attributed to our peculiar motion, the Doppler and aberration effects can change polarized and unpolarized power spectra of specific intensity in the CMB rest frame by 1 - 2 % , but we find the polarization cross-leakage between E and B modes to be negligible.

  15. Surface pressure field mapping using luminescent coatings

    NASA Technical Reports Server (NTRS)

    Mclachlan, B. G.; Kavandi, J. L.; Callis, J. B.; Gouterman, M.; Green, E.; Khalil, G.; Burns, D.

    1993-01-01

    In recent experiments we demonstrated the feasibility of using the oxygen dependence of luminescent molecules for surface pressure measurement in aerodynamic testing. This technique is based on the observation that for many luminescent molecules the light emitted increases as the oxygen partial pressure, and thus the air pressure, the molecules see decreases. In practice the surface to be observed is coated with an oxygen permeable polymer containing a luminescent molecule and illuminated with ultraviolet radiation. The airflow induced surface pressure field is seen as a luminescence intensity distribution which can be measured using quantitative video techniques. Computer processing converts the video data into a map of the surface pressure field. The experiments consisted of evaluating a trial luminescent coating in measuring the static surface pressure field over a two-dimensional NACA-0012 section model airfoil for Mach numbers ranging from 0.3 and 0.66. Comparison of the luminescent coating derived pressures were made to those obtained from conventional pressure taps. The method along with the experiment and its results will be described.

  16. Observation of Quartz Cathode-Luminescence in a Low Pressure Plasma Discharge

    NASA Technical Reports Server (NTRS)

    Foster, John E.

    2004-01-01

    Intense, steady-state cathode-luminescence has been observed from exposure of quartz powder to a low pressure rf-excited argon plasma discharge. The emission spectra (400 to 850 nm) associated with the powder luminescence were documented as a function of bias voltage using a spectrometer. The emission was broad-band, essentially washing out the line spectra features of the argon plasma discharge.

  17. Atmospheric reaction of Cl + methacrolein: a theoretical study on the mechanism, and pressure- and temperature-dependent rate constants.

    PubMed

    Sun, Cuihong; Xu, Baoen; Zhang, Shaowen

    2014-05-22

    Methacrolein is a major degradation product of isoprene, the reaction of methacrolein with Cl atoms may play some roles in the degradation of isoprene where these species are relatively abundant. However, the energetics and kinetics of this reaction, which govern the reaction branching, are still not well understood so far. In the present study, two-dimensional potential energy surfaces were constructed to analyze the minimum energy path of the barrierless addition process between Cl and the C═C double bond of methacrolein, which reveals that the terminal addition intermediate is directly formed from the addition reaction. The terminal addition intermediate can further yield different products among which the reaction paths abstracting the aldehyde hydrogen atom and the methyl hydrogen atom are dominant reaction exits. The minimum reaction path for the direct aldehydic hydrogen atom abstraction is also obtained. The reaction kinetics was calculated by the variational transition state theory in conjunction with the master equation method. From the theoretical model we predicted that the overall rate constant of the Cl + methacrolein reaction at 297 K and atmospheric pressure is koverall = 2.3× 10(-10) cm(3) molecule(-1) s(-1), and the branching ratio of the aldehydic hydrogen abstraction is about 12%. The reaction is pressure dependent at P < 10 Torr with the high pressure limit at about 100 Torr. The calculated results could well account for the experimental observations.

  18. ELECTRON MICROSCOPIC OBSERVATION OF SPECIMENS UNDER CONTROLLED GAS PRESSURE

    PubMed Central

    Heide, Hans Gunther

    1962-01-01

    A technique for encasing specimens in a thin gas layer during their observation in the Siemens Elmiskop I is described. All gases can be employed at pressures up to one atmosphere. Destruction of specimens can occur in the beam; all organic specimens are particularly liable to decompose. The conditions under which this can be avoided are given. A useful application of the technique allows one to prevent specimens from drying out, as they normally do in vacuum. A further application uses the controlled removal of carbon for thinning organic layers and for selective etching of organic materials. PMID:13905967

  19. 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> gradient 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> gradient magnitudes and the resulting sediment bed response to be <span class="hlt">observed</span> with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994JGR....9921511B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994JGR....9921511B"><span>Pickup protons and <span class="hlt">pressure</span>-balanced structures: Voyager 2 <span class="hlt">observations</span> in merged interaction regions near 35 AU</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Burlaga, L. F.; Ness, N. F.; Belcher, J. W.; Szabo, A.; Isenberg, P. A.; Lee, M. A.</p> <p>1994-11-01</p> <p>Five <span class="hlt">pressure</span>-balanced structures, each with a scale of the order of a few hundredths of an astonomical unit (AU), were identified in two merged interaction regions (MIRs) near 35 AU in the Voyager 2 plasma and magnetic field data. They include a tangential discontinuity, simple and complex magnetic holes, slow correlated variations among the plasma and magnetic field parameters, and complex uncorrelated variations among the parameters. The changes in the magnetic <span class="hlt">pressure</span> in these events are balanced by changes in the <span class="hlt">pressure</span> of interstellar pickup protons. Thus the pickup protons probably play a major role in the dynamics of the MIRs. The solar wind proton and electron <span class="hlt">pressures</span> are relatively unimportant in the MIRs at 35 AU and beyond. The region near 35 AU is transition region: the Sun is the source of the magnetic field, but the interstellar medium in source of pickups protons. Relative to the solar wind proton guyroadius, the thicknesses of the discontinuities and simple magnetic holes <span class="hlt">observed</span> near 35 AU are at least an order of magnitude greater than those <span class="hlt">observed</span> at 1 AU. However, the thicknesses of the tangential discontinuity and simple magnetic holes <span class="hlt">observed</span> near 35 AU (in units of the pickup proton Larmor radius) are comparable to those <span class="hlt">observed</span> at 1 AU (in units of the solar wind proton gyroradius). Thus the gyroradius of interstellar pickup protons controls the thickness of current sheets near 35 AU. We determine the interstellar pickup proton <span class="hlt">pressure</span> in the PBSs. Using a model for the pickup proton temperature, we estimate that the average interstellar pickup proton <span class="hlt">pressure</span>, temperature, and density in the MIRs at 35 AU are (0.53 +/- 0.14) x 10-12 erg/cu cm, (5.8 +/- 0.4) x 106 K and (7 +/- 2) x 10-4/cu cm.</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('https://www.ncbi.nlm.nih.gov/pubmed/10835248','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/10835248"><span>Modeling conductive heat transfer during high-<span class="hlt">pressure</span> thawing processes: determination of latent heat as a function of <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>Denys, S; Van Loey, A M; Hendrickx, M E</p> <p>2000-01-01</p> <p>A numerical heat transfer model for predicting product temperature profiles during high-<span class="hlt">pressure</span> thawing processes was recently proposed by the authors. In the present work, the predictive capacity of the model was considerably improved by taking into account the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the latent heat of the product that was used (Tylose). The effect of <span class="hlt">pressure</span> on the latent heat of Tylose was experimentally determined by a series of freezing experiments conducted at different <span class="hlt">pressure</span> levels. By combining a numerical heat transfer model for freezing processes with a least sum of squares optimization procedure, the corresponding latent heat at each <span class="hlt">pressure</span> level was estimated, and the obtained <span class="hlt">pressure</span> relation was incorporated in the original high-<span class="hlt">pressure</span> thawing model. Excellent agreement with the experimental temperature profiles for both high-<span class="hlt">pressure</span> freezing and thawing was <span class="hlt">observed</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvB..97v0401B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvB..97v0401B"><span>Detuning the honeycomb of α -RuCl3 : <span class="hlt">Pressure-dependent</span> optical studies reveal broken symmetry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Biesner, Tobias; Biswas, Sananda; Li, Weiwu; Saito, Yohei; Pustogow, Andrej; Altmeyer, Michaela; Wolter, Anja U. B.; Büchner, Bernd; Roslova, Maria; Doert, Thomas; Winter, Stephen M.; Valentí, Roser; Dressel, Martin</p> <p>2018-06-01</p> <p>The honeycomb Mott insulator α -RuCl3 loses its low-temperature magnetic order by <span class="hlt">pressure</span>. We report clear evidence for a dimerized structure at P >1 GPa and <span class="hlt">observe</span> the breakdown of the relativistic jeff picture in this regime strongly affecting the electronic properties. A <span class="hlt">pressure</span>-induced Kitaev quantum spin liquid cannot occur in this broken symmetry state. We shed light on the new phase by broadband infrared spectroscopy of the low-temperature properties of α -RuCl3 and ab initio density functional theory calculations, both under hydrostatic <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1248806','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1248806"><span>Structural phase diagram for ultra-thin epitaxial Fe 3O 4 / MgO(0 01) films: thickness and oxygen <span class="hlt">pressure</span> <span class="hlt">dependence</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>Alraddadi, S.; Hines, W.; Yilmaz, T.</p> <p>2016-02-19</p> <p>A systematic investigation of the thickness and oxygen <span class="hlt">pressure</span> <span class="hlt">dependence</span> for the structural properties of ultra-thin epitaxial magnetite (Fe 3O 4) films has been carried out; for such films, the structural properties generally differ from those for the bulk when the thickness ≤10 nm. Iron oxide ultra-thin films with thicknesses varying from 3 nm to 20 nm were grown on MgO (001) substrates using molecular beam epitaxy under different oxygen <span class="hlt">pressures</span> ranging from 1 × 10 -7 torr to 1 × 10 -5 torr. The crystallographic and electronic structures of the films were characterized using low energy electron diffraction (LEED)more » and x-ray photoemission spectroscopy (XPS), respectively. Moreover, the quality of the epitaxial Fe 3O 4 ultra-thin films was judged by magnetic measurements of the Verwey transition, along with complementary XPS spectra. We <span class="hlt">observed</span> that under the same growth conditions the stoichiometry of ultra-thin films under 10 nm transforms from the Fe 3O 4 phase to the FeO phase. In this work, a phase diagram based on thickness and oxygen <span class="hlt">pressure</span> has been constructed to explain the structural phase transformation. It was found that high-quality magnetite films with thicknesses ≤20 nm formed within a narrow range of oxygen <span class="hlt">pressure</span>. An optimal and controlled growth process is a crucial requirement for the accurate study of the magnetic and electronic properties for ultra-thin Fe 3O 4 films. Furthermore, these results are significant because they may indicate a general trend in the growth of other oxide films, which has not been previously <span class="hlt">observed</span> or considered.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JOM...tmp..150D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JOM...tmp..150D"><span><span class="hlt">Pressure</span> <span class="hlt">Dependence</span> of the Peierls Stress in Aluminum</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dang, Khanh; Spearot, Douglas</p> <p>2018-03-01</p> <p>The effect of <span class="hlt">pressure</span> applied normal to the {111} slip plane on the Peierls stress in Al is studied via atomistic simulations. Edge, screw, 30°, and 60° straight dislocations are created using the Volterra displacement fields for isotropic elasticity. For each dislocation character angle, the Peierls stress is calculated based on the change in the internal energy, which is an invariant measure of the dislocation driving force. It is found that the Peierls stress for dislocations under zero <span class="hlt">pressure</span> is in general agreement with previous results. For screw and 60° dislocations, the Peierls stress versus <span class="hlt">pressure</span> relationship has maximum values associated with stacking fault widths that are multiples of the Peierls period. For the edge dislocation, the Peierls stress decreases with increasing <span class="hlt">pressure</span> from tension to compression. Compared with the Mendelev potential, the Peierls stress calculated from the Mishin potential is more sensitive to changes in <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SPIE.9373E..0LL','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SPIE.9373E..0LL"><span>Water-soluble CdTe nanocrystals under high <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>Lin, Yan-Cheng</p> <p>2015-02-01</p> <p>The application of static high <span class="hlt">pressure</span> provides a method for precisely controlling and investigating many fundamental and unique properties of semiconductor nanocrystals (NCs). This study systematically investigates the high-<span class="hlt">pressure</span> photoluminescence (PL) and time-resolved carrier dynamics of thiol-capped CdTe NCs of different sizes, at different concentrations, and in various stress environments. The zincblende-to-rocksalt phase transition in thiol-capped CdTe NCs is <span class="hlt">observed</span> at a <span class="hlt">pressure</span> far in excess of the bulk phase transition <span class="hlt">pressure</span>. Additionally, the process of transformation <span class="hlt">depends</span> strongly on NC size, and the phase transition <span class="hlt">pressure</span> increases with NC size. These peculiar phenomena are attributed to the distinctive bonding of thiols to the NC surface. In a nonhydrostatic environment, considerable flattening of the PL energy of CdTe NCs powder is <span class="hlt">observed</span> above 3.0 GPa. Furthermore, asymmetric and double-peak PL emissions are obtained from a concentrated solution of CdTe NCs under hydrostatic <span class="hlt">pressure</span>, implying the feasibility of <span class="hlt">pressure</span>-induced interparticle coupling.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1919099T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1919099T"><span>Tsunami simulation method initiated from waveforms <span class="hlt">observed</span> by ocean bottom <span class="hlt">pressure</span> sensors for real-time tsunami forecast; Applied for 2011 Tohoku Tsunami</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tanioka, Yuichiro</p> <p>2017-04-01</p> <p>After tsunami disaster due to the 2011 Tohoku-oki great earthquake, improvement of the tsunami forecast has been an urgent issue in Japan. National Institute of Disaster Prevention is installing a cable network system of earthquake and tsunami <span class="hlt">observation</span> (S-NET) at the ocean bottom along the Japan and Kurile trench. This cable system includes 125 <span class="hlt">pressure</span> sensors (tsunami meters) which are separated by 30 km. Along the Nankai trough, JAMSTEC already installed and operated the cable network system of seismometers and <span class="hlt">pressure</span> sensors (DONET and DONET2). Those systems are the most dense <span class="hlt">observation</span> network systems on top of source areas of great underthrust earthquakes in the world. Real-time tsunami forecast has <span class="hlt">depended</span> on estimation of earthquake parameters, such as epicenter, depth, and magnitude of earthquakes. Recently, tsunami forecast method has been developed using the estimation of tsunami source from tsunami waveforms <span class="hlt">observed</span> at the ocean bottom <span class="hlt">pressure</span> sensors. However, when we have many <span class="hlt">pressure</span> sensors separated by 30km on top of the source area, we do not need to estimate the tsunami source or earthquake source to compute tsunami. Instead, we can initiate a tsunami simulation from those dense tsunami <span class="hlt">observed</span> data. <span class="hlt">Observed</span> tsunami height differences with a time interval at the ocean bottom <span class="hlt">pressure</span> sensors separated by 30 km were used to estimate tsunami height distribution at a particular time. In our new method, tsunami numerical simulation was initiated from those estimated tsunami height distribution. In this paper, the above method is improved and applied for the tsunami generated by the 2011 Tohoku-oki great earthquake. Tsunami source model of the 2011 Tohoku-oki great earthquake estimated using <span class="hlt">observed</span> tsunami waveforms, coseimic deformation <span class="hlt">observed</span> by GPS and ocean bottom sensors by Gusman et al. (2012) is used in this study. The ocean surface deformation is computed from the source model and used as an initial condition of tsunami</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhyB..536..522M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhyB..536..522M"><span><span class="hlt">Pressure</span>-induced itinerant electron metamagnetism in UCo0.995Os0.005Al ferromagnet</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mushnikov, N. V.; Andreev, A. V.; Arnold, Z.</p> <p>2018-05-01</p> <p>The effect of external hydrostatic <span class="hlt">pressure</span> on magnetic properties is studied for the UCo0.995Os0.005Al single crystal. At ambient <span class="hlt">pressure</span>, the ground state is ferromagnetic. Even lowest applied <span class="hlt">pressure</span> 0.11 GPa is sufficient to suppress ferromagnetism. A sharp metamagnetic transition is <span class="hlt">observed</span> only in magnetic fields along the c axis of the crystal, similar to previously studied itinerant electron metamagnet UCoAl. Temperature <span class="hlt">dependence</span> of the susceptibility for various <span class="hlt">pressures</span> shows a broad maximum at Tmax 20 K. The experimental data are analyzed with the theory of itinerant electron metamagnetism, which considers anisotropic thermal fluctuations of the uranium magnetic moment. The <span class="hlt">observed</span> <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the susceptibility at Tmax and the temperature for the disappearance of the first-order metamagnetic transition are explained with the theory.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2730749','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2730749"><span>Hydrostatic <span class="hlt">pressure-dependent</span> changes in cyclic AMP signaling in optic nerve head astrocytes from Caucasian and African American donors</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Chen, Lin; Hernandez, M. Rosario</p> <p>2009-01-01</p> <p>Purpose Investigate the effect of hydrostatic <span class="hlt">pressure</span> (HP) on 3′, 5′-cyclic adenosine monophosphate (cAMP) levels and downstream signaling in cultures of normal optic nerve head (ONH) astrocytes from Caucasian American (CA) and African American (AA) donors. Methods Intracellular cAMP levels were assayed after exposing ONH astrocytes to HP for varying times. Quantitative RT–PCR was used to determine the expression levels of selected cAMP pathway genes in human ONH astrocytes after HP treatment. Western blots were used to measure changes in the phosphorylation state of cAMP response element binding protein (CREB) in astrocytes subjected to HP, ATP, and phosphodiesterase or kinase inhibitors. Results The basal intracellular cAMP level is similar among AA and CA astrocytes. After exposure to HP for 15 min and 30 min in the presence of a phosphodiesterase inhibitor a further increase of intracellular cAMP was <span class="hlt">observed</span> in AA astrocytes, but not in CA astrocytes. Consistent with activation of the cAMP-<span class="hlt">dependent</span> protein kinase pathway, CREB phosphorylation (Ser-133) was increased to a greater extent in AA than in CA astrocytes after 3 h of HP. Exposure to elevated HP for 3–6 h differentially altered the expression levels of selected cAMP pathway genes (ADCY3, ADCY9, PTHLH, PDE7B) in AA compared to CA astrocytes. Treatment with ATP increased more CREB phosphorylation in CA than in AA astrocytes, suggesting differential Ca2+ signaling in these populations. Conclusions Activation of the cAMP-<span class="hlt">dependent</span> signaling pathway by <span class="hlt">pressure</span> may be an important contributor to increased susceptibility to elevated intraocular <span class="hlt">pressure</span> and glaucoma in AA, a population at higher risk for the disease. PMID:19710943</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1915734M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1915734M"><span>Investigation of the spatial variability and possible origins of wind-induced air <span class="hlt">pressure</span> fluctuations responsible for <span class="hlt">pressure</span> pumping</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mohr, Manuel; Laemmel, Thomas; Maier, Martin; Zeeman, Matthias; Longdoz, Bernard; Schindler, Dirk</p> <p>2017-04-01</p> <p>The exchange of greenhouse gases between the soil and the atmosphere is highly relevant for the climate of the Earth. Recent research suggests that wind-induced air <span class="hlt">pressure</span> fluctuations can alter the soil gas transport and therefore soil gas efflux significantly. Using a newly developed method, we measured soil gas transport in situ in a well aerated forest soil. Results from these measurements showed that the commonly used soil gas diffusion coefficient is enhanced up to 30% during periods of strong wind-induced air <span class="hlt">pressure</span> fluctuations. The air <span class="hlt">pressure</span> fluctuations above the forest floor are only induced at high above-canopy wind speeds (> 5 m s-1) and lie in the frequency range 0.01-0.1 Hz. Moreover, the amplitudes of air <span class="hlt">pressure</span> fluctuations in this frequency range show a clear quadratic <span class="hlt">dependence</span> on mean above-canopy wind speed. However, the origin of these wind-induced <span class="hlt">pressure</span> fluctuations is still unclear. Airflow measurements and high-precision air <span class="hlt">pressure</span> measurements were conducted at three different vegetation-covered sites (conifer forest, deciduous forest, grassland) to investigate the spatial variability of dominant air <span class="hlt">pressure</span> fluctuations, their origin and vegetation-<span class="hlt">dependent</span> characteristics. At the conifer forest site, a vertical profile of air <span class="hlt">pressure</span> fluctuations was measured and an array consisting of five <span class="hlt">pressure</span> sensors were installed at the forest floor. At the grassland site, the air <span class="hlt">pressure</span> measurements were compared with wind <span class="hlt">observations</span> made by ground-based LIDAR and spatial temperature <span class="hlt">observations</span> from a fibre-optic sensing network (ScaleX Campaign 2016). Preliminary results show that at all sites the amplitudes of relevant air <span class="hlt">pressure</span> fluctuations increase with increasing wind speed. Data from the array measurements reveal that there are no time lags between the air <span class="hlt">pressure</span> signals of different heights, but a time lag existed between the air <span class="hlt">pressure</span> signals of the sensors distributed laterally on the forest floor</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19880012120','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19880012120"><span><span class="hlt">Pressure</span> induced ageing of polymers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Emri, I.; Knauss, W. G.</p> <p>1988-01-01</p> <p>The nonlinearly viscoelastic response of an amorphous homopolymer is considered under aspects of time <span class="hlt">dependent</span> free volume behavior. In contrast to linearly viscoelastic solids, this model couples shear and volume deformation through a shift function which influences the rate of molecular relaxation or creep. Sample computations produce all those qualitative features one <span class="hlt">observes</span> normally in uniaxial tension including the rate <span class="hlt">dependent</span> formation of a yield point as a consequence of the history of an imposed <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25380152','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25380152"><span>Cocoa consumption dose-<span class="hlt">dependently</span> improves flow-mediated dilation and arterial stiffness decreasing blood <span class="hlt">pressure</span> in healthy individuals.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Grassi, Davide; Desideri, Giovambattista; Necozione, Stefano; di Giosia, Paolo; Barnabei, Remo; Allegaert, Leen; Bernaert, Herwig; Ferri, Claudio</p> <p>2015-02-01</p> <p>Cocoa flavonoids exert beneficial vascular effects and reduce the risk of cardiovascular morbidity and mortality. Nevertheless, the involved mechanisms have not been clarified and no study has yet focused on the dose-response effects. We aimed to investigate the effects of different doses of cocoa flavonoids on flow-mediated dilation (FMD), endothelin-1 (ET-1), pulse wave velocity (PWV), and SBP and DBP. According to a randomized, double-blind, controlled, cross-over design, 20 healthy volunteers (1.5% improvement in FMD in 20 individuals: 0.99 at alpha = 0.05) were assigned to receive either five treatments with daily intake of 10 g cocoa (0, 80, 200, 500 and 800 mg cocoa flavonoids/day) in five periods lasting 1 week each. Cocoa dose-<span class="hlt">dependently</span> increased FMD from 6.2% (control) to 7.3, 7.6, 8.1 and 8.2% after the different flavonoid doses, respectively (P < 0.0001). Compared with the control, even 80  mg cocoa flavonoids per day increased FMD (P < 0.0001). Cocoa dose-<span class="hlt">dependently</span> decreased PWV (P < 0.0001). Cocoa intake decreased office blood <span class="hlt">pressure</span> (BP) (SBP: -4.8 ± 1.03  mmHg, P < 0.0001; DBP: -3.03 ± 1.07 mmHg, P = 0.0011). With respect to control, cocoa ingestion decreased 24-h (P = 0.05) and daytime (P = 0.038) SBP, and 24-h (P = 0.0064), daytime (P = 0.0088) and night-time (P = 0.0352) pulse <span class="hlt">pressure</span>. Compared with the control, cocoa dose-<span class="hlt">dependently</span> decreased ET-1 levels [from 17.1 (control) to 15.2, 14.5, 14.2 and 14.1 pg/ml, after the different flavonoid doses, respectively (P for treatment <0.05)]. Compared with the control, significant changes were <span class="hlt">observed</span> for all doses of flavonoids (ET-1; P < 0.05). Our study showed for the first time that cocoa dose-<span class="hlt">dependently</span> improved FMD and decreased PWV and ET-1 also by ameliorating office and monitored BP. Our findings are clinically relevant, suggesting cocoa, with very low calorie intake, might be reasonably incorporated into a dietary</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25581554','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25581554"><span>Does the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of kinetic isotope effects report usefully on dynamics in enzyme H-transfer reactions?</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hoeven, Robin; Heyes, Derren J; Hay, Sam; Scrutton, Nigel S</p> <p>2015-08-01</p> <p>The temperature <span class="hlt">dependence</span> of kinetic isotope effects (KIEs) has emerged as the main experimental probe of enzymatic H-transfer by quantum tunnelling. Implicit in the interpretation is a presumed role for dynamic coupling of H-transfer chemistry to the protein environment, the so-called 'promoting motions/vibrations hypothesis'. This idea remains contentious, and others have questioned the importance and/or existence of promoting motions/vibrations. New experimental methods of addressing this problem are emerging, including use of mass-modulated enzymes and time-resolved spectroscopy. The <span class="hlt">pressure</span> <span class="hlt">dependence</span> of KIEs has been considered as a potential probe of quantum tunnelling reactions, because semi-classical KIEs, which are defined by differences in zero-point vibrational energy, are relatively insensitive to kbar changes in <span class="hlt">pressure</span>. Reported combined <span class="hlt">pressure</span> and temperature (p-T) <span class="hlt">dependence</span> studies of H-transfer reactions are, however, limited. Here, we extend and review the available p-T studies that have utilized well-defined experimental systems in which quantum mechanical tunnelling is established. These include flavoproteins, quinoproteins, light-activated enzymes and chemical model systems. We show that there is no clear general trend between the p-T <span class="hlt">dependencies</span> of the KIEs in these systems. Given the complex nature of p-T studies, we conclude that computational simulations using determined (e.g. X-ray) structures are also needed alongside experimental measurements of reaction rates/KIEs to guide the interpretation of p-T effects. In providing new insight into H-transfer/environmental coupling, combined approaches that unite both atomistic understanding with experimental rate measurements will require careful evaluation on a case-by-case basis. Although individually informative, we conclude that p-T studies do not provide the more generalized insight that has come from studies of the temperature <span class="hlt">dependence</span> of KIEs. © 2015 The Authors. FEBS Journal</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014APS..MARA26008G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014APS..MARA26008G"><span><span class="hlt">Observation</span> of antiferromagnetic order collapse in the <span class="hlt">pressurized</span> insulator LaMnPO</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guo, Jing; Simonson, Jack; Sun, Liling; Wu, Qi; Guo, Peiwen; Zhang, Chao; Gu, Dachun; Kotliar, Gabriel; Aronson, Meigan; Zhao, Zhongxian</p> <p>2014-03-01</p> <p>The emergence of superconductivity in the iron pnictide or cuprate high temperature superconductors usually accompanies the suppression of a long-ranged antiferromagnetic (AFM) order state in a corresponding parent compound by doping or <span class="hlt">pressurizing</span>. A great deal of effort by doping has been made to find superconductivity in Mn-based compounds, which are thought to bridge the gap between the two families of high temperature superconductors, but the AFM order was not successfully suppressed. Here we report the first <span class="hlt">observations</span> of the <span class="hlt">pressure</span>-induced elimination of long-ranged AFM order at ~ 34 GPa and a crossover from an AFM insulating to an AFM metallic state at ~ 20 GPa in LaMnPO single crystals that are iso-structural to the LaFeAsO superconductor by in-situ high <span class="hlt">pressure</span> resistance and ac susceptibility measurements. These findings are of importance to explore potential superconductivity in Mn-based compounds and to shed new light on the underlying mechanism of high temperature superconductivity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013NatSR...3E2555G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013NatSR...3E2555G"><span><span class="hlt">Observation</span> of antiferromagnetic order collapse in the <span class="hlt">pressurized</span> insulator LaMnPO</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guo, Jing; Simonson, J. W.; Sun, Liling; Wu, Qi; Gao, Peiwen; Zhang, Chao; Gu, Dachun; Kotliar, Gabriel; Aronson, Meigan; Zhao, Zhongxian</p> <p>2013-08-01</p> <p>The emergence of superconductivity in the iron pnictide or cuprate high temperature superconductors usually accompanies the suppression of a long-ranged antiferromagnetic (AFM) order state in a corresponding parent compound by doping or <span class="hlt">pressurizing</span>. A great deal of effort by doping has been made to find superconductivity in Mn-based compounds, which are thought to bridge the gap between the two families of high temperature superconductors, but the AFM order was not successfully suppressed. Here we report the first <span class="hlt">observations</span> of the <span class="hlt">pressure</span>-induced elimination of long-ranged AFM order at ~ 34 GPa and a crossover from an AFM insulating to an AFM metallic state at ~ 20 GPa in LaMnPO single crystals that are iso-structural to the LaFeAsO superconductor by in-situ high <span class="hlt">pressure</span> resistance and ac susceptibility measurements. These findings are of importance to explore potential superconductivity in Mn-based compounds and to shed new light on the underlying mechanism of high temperature superconductivity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23989921','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23989921"><span><span class="hlt">Observation</span> of antiferromagnetic order collapse in the <span class="hlt">pressurized</span> insulator LaMnPO.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Guo, Jing; Simonson, J W; Sun, Liling; Wu, Qi; Gao, Peiwen; Zhang, Chao; Gu, Dachun; Kotliar, Gabriel; Aronson, Meigan; Zhao, Zhongxian</p> <p>2013-01-01</p> <p>The emergence of superconductivity in the iron pnictide or cuprate high temperature superconductors usually accompanies the suppression of a long-ranged antiferromagnetic (AFM) order state in a corresponding parent compound by doping or <span class="hlt">pressurizing</span>. A great deal of effort by doping has been made to find superconductivity in Mn-based compounds, which are thought to bridge the gap between the two families of high temperature superconductors, but the AFM order was not successfully suppressed. Here we report the first <span class="hlt">observations</span> of the <span class="hlt">pressure</span>-induced elimination of long-ranged AFM order at ~ 34 GPa and a crossover from an AFM insulating to an AFM metallic state at ~ 20 GPa in LaMnPO single crystals that are iso-structural to the LaFeAsO superconductor by in-situ high <span class="hlt">pressure</span> resistance and ac susceptibility measurements. These findings are of importance to explore potential superconductivity in Mn-based compounds and to shed new light on the underlying mechanism of high temperature superconductivity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvB..96x5130H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvB..96x5130H"><span>Anisotropic <span class="hlt">dependence</span> of the magnetic transition on uniaxial <span class="hlt">pressure</span> in the Kondo semiconductors Ce T2A l10 (T =Ru and Os)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hayashi, K.; Umeo, K.; Takeuchi, T.; Kawabata, J.; Muro, Y.; Takabatake, T.</p> <p>2017-12-01</p> <p>We have measured the strain, magnetization, and specific heat of the antiferromagnetic (AFM) Kondo semiconductors Ce T2A l10 (T =Ru and Os) under uniaxial <span class="hlt">pressures</span> applied along the orthorhombic axes. We found a linear <span class="hlt">dependence</span> of TN on the b -axis parameter for both compounds under uniaxial <span class="hlt">pressure</span> P ∥b and hydrostatic <span class="hlt">pressure</span>. This relation indicates that the distance between the Ce-T layers along the b axis is the key structural parameter determining TN. Furthermore, the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the spin-flop transition field indicates that Ce-Ce interchain interactions stabilize the AFM state with the ordered moments pointing to the c axis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030062124&hterms=Hydrostatic+pressure&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DHydrostatic%2Bpressure','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030062124&hterms=Hydrostatic+pressure&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DHydrostatic%2Bpressure"><span>Composition <span class="hlt">Dependence</span> of the Hydrostatic <span class="hlt">Pressure</span> Coefficients of the Bandgap of ZnSe(1-x)Te(x) Alloys</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wu, J.; Yu, K. M.; Walukiewicz, W.; Shan, W.; Ager, J. W., III; Haller, E. E.; Miotkowski, I.; Ramdas, A. K.; Su, Ching-Hua</p> <p>2003-01-01</p> <p>Optical absorption experiments have been performed using diamond anvil cells to measure the hydrostatic <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the fundamental bandgap of ZnSe(sub 1-xTe(sub x) alloys over the entire composition range. The first and second-order <span class="hlt">pressure</span> coefficients are obtained as a function of composition. Starting from the ZnSe side, the magnitude of both coefficients increases slowly until x approx. 0.7, where the ambient-<span class="hlt">pressure</span> bandgap reaches a minimum. For larger values of x the coefficients rapidly approach the values of ZnTe. The large deviations of the <span class="hlt">pressure</span> coefficients from the linear interpolation between ZnSe and ZnTe are explained in terms of the band anticrossing model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160009374','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160009374"><span>Surface <span class="hlt">Pressure</span> <span class="hlt">Dependencies</span> in the GEOS-Chem-Adjoint System and the Impact of the GEOS-5 Surface <span class="hlt">Pressure</span> on CO2 Model Forecast</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lee, Meemong; Weidner, Richard</p> <p>2016-01-01</p> <p>In the GEOS-Chem Adjoint (GCA) system, the total (wet) surface <span class="hlt">pressure</span> of the GEOS meteorology is employed as dry surface <span class="hlt">pressure</span>, ignoring the presence of water vapor. The Jet Propulsion Laboratory (JPL) Carbon Monitoring System (CMS) research team has been evaluating the impact of the above discrepancy on the CO2 model forecast and the CO2 flux inversion. The JPL CMS research utilizes a multi-mission assimilation framework developed by the Multi-Mission <span class="hlt">Observation</span> Operator (M2O2) research team at JPL extending the GCA system. The GCA-M2O2 framework facilitates mission-generic 3D and 4D-variational assimilations streamlining the interfaces to the satellite data products and prior emission inventories. The GCA-M2O2 framework currently integrates the GCA system version 35h and provides a dry surface <span class="hlt">pressure</span> setup to allow the CO2 model forecast to be performed with the GEOS-5 surface <span class="hlt">pressure</span> directly or after converting it to dry surface <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20160004225&hterms=dependency&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Ddependency','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20160004225&hterms=dependency&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Ddependency"><span>Surface <span class="hlt">Pressure</span> <span class="hlt">Dependencies</span> in the Geos-Chem-Adjoint System and the Impact of the GEOS-5 Surface <span class="hlt">Pressure</span> on CO2 Model Forecast</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lee, Meemong; Weidner, Richard</p> <p>2016-01-01</p> <p>In the GEOS-Chem Adjoint (GCA) system, the total (wet) surface <span class="hlt">pressure</span> of the GEOS meteorology is employed as dry surface <span class="hlt">pressure</span>, ignoring the presence of water vapor. The Jet Propulsion Laboratory (JPL) Carbon Monitoring System (CMS) research team has been evaluating the impact of the above discrepancy on the CO2 model forecast and the CO2 flux inversion. The JPL CMS research utilizes a multi-mission assimilation framework developed by the Multi-Mission <span class="hlt">Observation</span> Operator (M2O2) research team at JPL extending the GCA system. The GCA-M2O2 framework facilitates mission-generic 3D and 4D-variational assimilations streamlining the interfaces to the satellite data products and prior emission inventories. The GCA-M2O2 framework currently integrates the GCA system version 35h and provides a dry surface <span class="hlt">pressure</span> setup to allow the CO2 model forecast to be performed with the GEOS-5 surface <span class="hlt">pressure</span> directly or after converting it to dry surface <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12885646','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12885646"><span>The <span class="hlt">pressure-dependence</span> of the size of extruded vesicles.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Patty, Philipus J; Frisken, Barbara J</p> <p>2003-08-01</p> <p>Variations in the size of vesicles formed by extrusion through small pores are discussed in terms of a simple model. Our model predicts that the radius should decrease as the square root of the applied <span class="hlt">pressure</span>, consistent with data for vesicles extruded under various conditions. The model also predicts <span class="hlt">dependencies</span> on the pore size used and on the lysis tension of the vesicles being extruded that are consistent with our data. The pore size was varied by using track-etched polycarbonate membranes with average pore diameters ranging from 50 to 200 nm. To vary the lysis tension, vesicles made from POPC (1-palmitoyl-2-oleoyl-sn-glycero-3-phosphatidylcholine), mixtures of POPC and cholesterol, and mixtures of POPC and C(16)-ceramide were studied. The lysis tension, as measured by an extrusion-based technique, of POPC:cholesterol vesicles is higher than that of pure POPC vesicles whereas POPC:ceramide vesicles have lower lysis tensions than POPC vesicles.</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('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1303220','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1303220"><span>The <span class="hlt">Pressure-Dependence</span> of the Size of Extruded Vesicles</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Patty, Philipus J.; Frisken, Barbara J.</p> <p>2003-01-01</p> <p>Variations in the size of vesicles formed by extrusion through small pores are discussed in terms of a simple model. Our model predicts that the radius should decrease as the square root of the applied <span class="hlt">pressure</span>, consistent with data for vesicles extruded under various conditions. The model also predicts <span class="hlt">dependencies</span> on the pore size used and on the lysis tension of the vesicles being extruded that are consistent with our data. The pore size was varied by using track-etched polycarbonate membranes with average pore diameters ranging from 50 to 200 nm. To vary the lysis tension, vesicles made from POPC (1-palmitoyl-2-oleoyl-sn-glycero-3-phosphatidylcholine), mixtures of POPC and cholesterol, and mixtures of POPC and C16-ceramide were studied. The lysis tension, as measured by an extrusion-based technique, of POPC:cholesterol vesicles is higher than that of pure POPC vesicles whereas POPC:ceramide vesicles have lower lysis tensions than POPC vesicles. PMID:12885646</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015IJAEO..37..124N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015IJAEO..37..124N"><span>Satellite Earth <span class="hlt">observation</span> data to identify anthropogenic <span class="hlt">pressures</span> in selected protected areas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nagendra, Harini; Mairota, Paola; Marangi, Carmela; Lucas, Richard; Dimopoulos, Panayotis; Honrado, João Pradinho; Niphadkar, Madhura; Mücher, Caspar A.; Tomaselli, Valeria; Panitsa, Maria; Tarantino, Cristina; Manakos, Ioannis; Blonda, Palma</p> <p>2015-05-01</p> <p>Protected areas are experiencing increased levels of human <span class="hlt">pressure</span>. To enable appropriate conservation action, it is critical to map and monitor changes in the type and extent of land cover/use and habitat classes, which can be related to human <span class="hlt">pressures</span> over time. Satellite Earth <span class="hlt">observation</span> (EO) data and techniques offer the opportunity to detect such changes. Yet association with field information and expert interpretation by ecologists is required to interpret, qualify and link these changes to human <span class="hlt">pressure</span>. There is thus an urgent need to harmonize the technical background of experts in the field of EO data analysis with the terminology of ecologists, protected area management authorities and policy makers in order to provide meaningful, context-specific value-added EO products. This paper builds on the DPSIR framework, providing a terminology to relate the concepts of state, <span class="hlt">pressures</span>, and drivers with the application of EO analysis. The type of <span class="hlt">pressure</span> can be inferred through the detection of changes in state (i.e. changes in land cover and/or habitat type and/or condition). Four broad categories of changes in state are identified, i.e. land cover/habitat conversion, land cover/habitat modification, habitat fragmentation and changes in landscape connectivity, and changes in plant community structure. These categories of change in state can be mapped through EO analyses, with the goal of using expert judgement to relate changes in state to causal direct anthropogenic <span class="hlt">pressures</span>. Drawing on expert knowledge, a set of protected areas located in diverse socio-ecological contexts and subject to a variety of <span class="hlt">pressures</span> are analysed to (a) link the four categories of changes in state of land cover/habitats to the drivers (anthropogenic <span class="hlt">pressure</span>), as relevant to specific target land cover and habitat classes; (b) identify (for <span class="hlt">pressure</span> mapping) the most appropriate spatial and temporal EO data sources as well as interpretations from ecologists and field data</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27082434','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27082434"><span>Graphene Membranes for Atmospheric <span class="hlt">Pressure</span> Photoelectron Spectroscopy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Weatherup, Robert S; Eren, Baran; Hao, Yibo; Bluhm, Hendrik; Salmeron, Miquel B</p> <p>2016-05-05</p> <p>Atmospheric <span class="hlt">pressure</span> X-ray photoelectron spectroscopy (XPS) is demonstrated using single-layer graphene membranes as photoelectron-transparent barriers that sustain <span class="hlt">pressure</span> differences in excess of 6 orders of magnitude. The graphene serves as a support for catalyst nanoparticles under atmospheric <span class="hlt">pressure</span> reaction conditions (up to 1.5 bar), where XPS allows the oxidation state of Cu nanoparticles and gas phase species to be simultaneously probed. We thereby <span class="hlt">observe</span> that the Cu(2+) oxidation state is stable in O2 (1 bar) but is spontaneously reduced under vacuum. We further demonstrate the detection of various gas-phase species (Ar, CO, CO2, N2, O2) in the <span class="hlt">pressure</span> range 10-1500 mbar including species with low photoionization cross sections (He, H2). <span class="hlt">Pressure-dependent</span> changes in the apparent binding energies of gas-phase species are <span class="hlt">observed</span>, attributable to changes in work function of the metal-coated grids supporting the graphene. We expect atmospheric <span class="hlt">pressure</span> XPS based on this graphene membrane approach to be a valuable tool for studying nanoparticle catalysis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23556700','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23556700"><span>Distortion product otoacoustic emissions upon ear canal <span class="hlt">pressurization</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zebian, Makram; Schirkonyer, Volker; Hensel, Johannes; Vollbort, Sven; Fedtke, Thomas; Janssen, Thomas</p> <p>2013-04-01</p> <p>The purpose of this study was to quantify the change in distortion product otoacoustic emission (DPOAE) level upon ear canal <span class="hlt">pressurization</span>. DPOAEs were measured on 12 normal-hearing human subjects for ear canal static <span class="hlt">pressures</span> between -200 and +200 daPa in (50 ± 5) daPa steps. A clear <span class="hlt">dependence</span> of DPOAE levels on the <span class="hlt">pressure</span> was <span class="hlt">observed</span>, with levels being highest at the maximum compliance of the middle ear, and decreasing on average by 2.3 dB per 50 daPa for lower and higher <span class="hlt">pressures</span>. Ear canal <span class="hlt">pressurization</span> can serve as a tool for improving the detectability of DPOAEs in the case of middle-ear dysfunction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015RScI...86l3109B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015RScI...86l3109B"><span>Formaldehyde preparation methods for <span class="hlt">pressure</span> and temperature <span class="hlt">dependent</span> laser-induced fluorescence measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Burkert, A.; Müller, D.; Rieger, S.; Schmidl, G.; Triebel, W.; Paa, W.</p> <p>2015-12-01</p> <p>Formaldehyde is an excellent tracer for the early phase of ignition of hydrocarbon fuels and can be used, e.g., for characterization of single droplet ignition. However, due to its fast thermal decomposition at elevated temperatures and <span class="hlt">pressures</span>, the determination of concentration fields from laser-induced fluorescence (LIF) measurements is difficult. In this paper, we address LIF measurements of this important combustion intermediate using a calibration cell. Here, formaldehyde is created from evaporation of paraformaldehyde. We discuss three setups for preparation of formaldehyde/air mixtures with respect to their usability for well-defined heating of formaldehyde/air mixtures. The "basic setup" uses a resist heater around the measurement cell for investigation of formaldehyde near vacuum conditions or formaldehyde/air samples after sequential admixing of air. The second setup, described for the first time in detail here, takes advantage of a constant flow formaldehyde/air regime which uses preheated air to reduce the necessary time for gas heating. We used the constant flow system to measure new <span class="hlt">pressure</span> <span class="hlt">dependent</span> LIF excitation spectra in the 343 nm spectral region (414 absorption band of formaldehyde). The third setup, based on a novel concept for fast gas heating via excitation of SF6 (chemically inert gas) using a TEA (transverse excitation at atmospheric <span class="hlt">pressure</span>) CO2 laser, allows to further minimize both gas heating time and thermal decomposition. Here, an admixture of CO2 is served for real time temperature measurement based on Raman scattering. The applicability of the fast laser heating system has been demonstrated with gas mixtures of SF6 + air, SF6 + N2, as well as SF6 + N2 + CO2 at 1 bar total <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22413078-anomalous-softening-yield-strength-tantalum-high-pressures','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22413078-anomalous-softening-yield-strength-tantalum-high-pressures"><span>Anomalous softening of yield strength in tantalum at high <span class="hlt">pressures</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>Jing, Qiumin, E-mail: j-qm@163.com; Wu, Qiang; Xu, Ji-an</p> <p>2015-02-07</p> <p>The <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the yield strength of tantalum was investigated experimentally up to 101 GPa at room temperature using a diamond anvil cell. A yield strength softening is <span class="hlt">observed</span> between 52 and 84 GPa, whereas a normal trend is <span class="hlt">observed</span> below 52 GPa and above 84 GPa. The onset <span class="hlt">pressure</span> of the softening is in agreement with previous results obtained by the <span class="hlt">pressure</span> gradient method and shock wave experiments. This unusual strength softening in tantalum is not related with structural transformation, preferred orientation, or material damage. Our measurements indicate that microscopic deviatoric strain is the major reason for the <span class="hlt">observed</span> strength softening inmore » tantalum.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1349784-pressure-dependence-carbonate-exchange-npo2-co3-aqueous-solutions','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1349784-pressure-dependence-carbonate-exchange-npo2-co3-aqueous-solutions"><span><span class="hlt">Pressure</span> <span class="hlt">dependence</span> of carbonate exchange with [NpO 2(CO 3) 3] 4– in aqueous solutions</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Pilgrim, Corey D.; Zavarin, Mavrik; Casey, William H.</p> <p>2016-12-13</p> <p>Here, the rates of ligand exchange into the geochemically important [NpO 2(CO 3) 3] 4– aqueous complex are measured as a function of <span class="hlt">pressure</span> in order to complement existing data on the isostructural [UO 2(CO 3) 3] 4– complex. Experiments are conducted at pH conditions where the rate of exchange is independent of the proton concentration. Unexpectedly, the experiments show a distinct difference in the <span class="hlt">pressure</span> <span class="hlt">dependencies</span> of rates of exchange for the uranyl and neptunyl complexes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23736112','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23736112"><span>Effects of antihypertensive drugs on central blood <span class="hlt">pressure</span> in humans: a preliminary <span class="hlt">observation</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Agnoletti, Davide; Zhang, Yi; Borghi, Claudio; Blacher, Jacques; Safar, Michel E</p> <p>2013-08-01</p> <p>Central blood <span class="hlt">pressure</span> (BP) is considered a better predictor of cardiovascular events than brachial BP. Modifications of central, beyond brachial BP, can be assessed by <span class="hlt">pressure</span> amplification, a potential new cardiovascular risk factor. Comparison between drugs' effect on central hemodynamics has been poorly studied. Our aim was to assess the hemodynamic effect of a 12-week treatment with amlodipine 5mg, or candesartan 8mg, or indapamide sustained-release 1.5mg, in comparison with placebo. We analyzed 145 out-patients with essential hypertension in primary prevention enrolled in the Natrilix SR Versus Candesartan and Amlodipine in the Reduction of Systolic Blood <span class="hlt">Pressure</span> in Hypertensive Patients (X-CELLENT) study, a multicenter, randomized, double-blinded, placebo-controlled trial. Arterial stiffness, central BP, <span class="hlt">pressure</span> amplification, and wave reflection were measured by applanation tonometry. Baseline characteristics of patients were homogeneous between groups. After treatment, we found that active drugs produced similar reduction of both central and peripheral BPs, with no significant interdrug differences (all P < 0.05; excluded peripheral pulse <span class="hlt">pressure</span>, compared with placebo). Second, amlodipine (1.9% ± 15.3%), candesartan (3.0% ± 14.6%) and indapamide (4.1% ± 14.4%) all increased pulse <span class="hlt">pressure</span> amplification, but only indapamide was statistically different from placebo (P = 0.02). Finally, no significant changes were <span class="hlt">observed</span> on pulse wave velocity, heart rate, and augmentation index. The 3 antihypertensive drugs similarly reduced peripheral and central BP, as compared with placebo, but a significant increase in pulse <span class="hlt">pressure</span> amplification was obtained only with indapamide, independently of arterial stiffness modifications. 3283161 by BIOPHARMA.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMNH41A1771F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMNH41A1771F"><span>Statistical Features of Deep-ocean Tsunamis Based on 30 Years of Bottom <span class="hlt">Pressure</span> <span class="hlt">Observations</span> in the Northeast Pacific</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fine, I.; Thomson, R.; Chadwick, W. W., Jr.; Davis, E. E.; Fox, C. G.</p> <p>2016-12-01</p> <p>We have used a set of high-resolution bottom <span class="hlt">pressure</span> recorder (BPR) time series collected at Axial Seamount on the Juan de Fuca Ridge beginning in 1986 to examine tsunami waves of seismological origin in the northeast Pacific. These data are a combination of autonomous, internally-recording battery-powered instruments and cabled instruments on the OOI Cabled Array. Of the total of 120 tsunami events catalogued for the coasts of Japan, Alaska, western North America and Hawaii, we found evidence for 38 events in the Axial Seamount BPR records. Many of these tsunamis were not <span class="hlt">observed</span> along the adjacent west coast of the USA and Canada because of the much higher noise level of coastal locations and the lack of digital tide gauge data prior to 2000. We have also identified several tsunamis of apparent seismological origin that were <span class="hlt">observed</span> at coastal stations but not at the deep ocean site. Careful analysis of these <span class="hlt">observations</span> suggests that they were likely of meteorological origin. Analysis of the <span class="hlt">pressure</span> measurements from Axial Seamount, along with BPR measurements from a nearby ODP CORK (Ocean Drilling Program Circulation Obviation Retrofit Kit) borehole and DART (Deep-ocean Assessment and Reporting of Tsunamis) locations, reveals features of deep-ocean tsunamis that are markedly different from features <span class="hlt">observed</span> at coastal locations. Results also show that the energy of deep-ocean tsunamis can differ significantly among the three sets of stations despite their close spatial spacing and that this difference is strongly <span class="hlt">dependent</span> on the direction of the incoming tsunami waves. These deep-ocean <span class="hlt">observations</span> provide the most comprehensive statistics possible for tsunamis in the Pacific Ocean over the past 30 years. New insight into the distribution of tsunami amplitudes and wave energy derived from the deep-ocean sites should prove useful for long-term tsunami prediction and mitigation for coastal communities along the west coast of the USA and Canada.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhPro..72..362M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhPro..72..362M"><span>Combustion of Micro- and Nanothermites under Elevating <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>Monogarov, K.; Pivkina, Alla; Muravyev, N.; Meerov, D.; Dilhan, D.</p> <p></p> <p>Non-equilibrium process of combustion-wave propagation of thermite compositions (Mg/Fe2O3) inside the sealed steel tube have been investigated to study the burning rate at elevating <span class="hlt">pressure</span>. Under confinement the hot gas-phase products, formed during thermite combustion result in considerable overpressure inside the tube that reverses the gas flow and leads to <span class="hlt">pressure</span>-driven preheating effect of the burned-gas permeation. Convective origin of this preheating effect is discussed. The <span class="hlt">pressure</span>-time <span class="hlt">dependency</span> is obtained experimentally. The composition was pressed inside the steel tube in pellets; the size of each part was measured to obtain burning rate - <span class="hlt">pressure</span> <span class="hlt">dependency</span>. Both micro- and nanosized components were used to prepare thermite compositions under study. The significant difference in burning parameters of micron- and nanosized thermites is <span class="hlt">observed</span> and analyzed. Based on obtained results, the combustion mechanism of thermites with the micro- and nanosized components is discussed.</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 <span class="hlt">depending</span> 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 ideal 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 <span class="hlt">observed</span>. 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 ideal 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('https://www.osti.gov/pages/biblio/1332633-high-pressure-studies-potassium-perchlorate','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1332633-high-pressure-studies-potassium-perchlorate"><span>High <span class="hlt">pressure</span> studies of potassium perchlorate</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Pravica, Michael; Wang, Yonggang; Sneed, Daniel; ...</p> <p>2016-07-29</p> <p>Two experiments are reported on KClO 4 at extreme conditions. A static high <span class="hlt">pressure</span> Raman study was first conducted to 18.9 GPa. Evidence for at least two new phases was <span class="hlt">observed</span>: one between 2.4 and 7.7 GPa (possibly sluggish), and the second near 11.7 GPa. Then, the X-ray induced decomposition rate of potassium perchlorate (KClO 4 hv→ KCl + 2O 2) was studied up to 15.2 GPa. The time-<span class="hlt">dependent</span> growth of KCl and O 2 was monitored. The decomposition rate slowed at higher <span class="hlt">pressures</span>. As a result, we present the first direct evidence for O 2 crystallization at higher <span class="hlt">pressures</span>,more » demonstrating that O 2 molecules aggregate at high <span class="hlt">pressure</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23365621','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23365621"><span>Application of seemingly unrelated regression in medical data with intermittently <span class="hlt">observed</span> time-<span class="hlt">dependent</span> covariates.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Keshavarzi, Sareh; Ayatollahi, Seyyed Mohammad Taghi; Zare, Najaf; Pakfetrat, Maryam</p> <p>2012-01-01</p> <p>BACKGROUND. In many studies with longitudinal data, time-<span class="hlt">dependent</span> covariates can only be measured intermittently (not at all <span class="hlt">observation</span> times), and this presents difficulties for standard statistical analyses. This situation is common in medical studies, and methods that deal with this challenge would be useful. METHODS. In this study, we performed the seemingly unrelated regression (SUR) based models, with respect to each <span class="hlt">observation</span> time in longitudinal data with intermittently <span class="hlt">observed</span> time-<span class="hlt">dependent</span> covariates and further compared these models with mixed-effect regression models (MRMs) under three classic imputation procedures. Simulation studies were performed to compare the sample size properties of the estimated coefficients for different modeling choices. RESULTS. In general, the proposed models in the presence of intermittently <span class="hlt">observed</span> time-<span class="hlt">dependent</span> covariates showed a good performance. However, when we considered only the <span class="hlt">observed</span> values of the covariate without any imputations, the resulted biases were greater. The performances of the proposed SUR-based models in comparison with MRM using classic imputation methods were nearly similar with approximately equal amounts of bias and MSE. CONCLUSION. The simulation study suggests that the SUR-based models work as efficiently as MRM in the case of intermittently <span class="hlt">observed</span> time-<span class="hlt">dependent</span> covariates. Thus, it can be used as an alternative to MRM.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSM11B2309V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM11B2309V"><span>Tracking a Solar Wind Dynamic <span class="hlt">Pressure</span> Pulses' Impact Through the Magnetosphere Using the Heliophysics System Observatory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vidal-Luengo, S.; Moldwin, M.</p> <p>2017-12-01</p> <p>During northward Interplanetary Magnetic Field (IMF) Bz conditions, the magnetosphere acts as a closed "cavity" and reacts to solar wind dynamic <span class="hlt">pressure</span> pulses more simply than during southward IMF conditions. Effects of solar wind dynamic <span class="hlt">pressure</span> have been <span class="hlt">observed</span> as geomagnetic lobe compressions <span class="hlt">depending</span> on the characteristics of the <span class="hlt">pressure</span> pulse and the spacecraft location. One of the most important aspects of this study is the incorporation of simultaneous <span class="hlt">observations</span> by different missions, such as WIND, CLUSTER, THEMIS, MMS, Van Allen Probes and GOES as well as magnetometer ground stations that allow us to map the magnetosphere response at different locations during the propagation of a <span class="hlt">pressure</span> pulse. In this study we used the SYM-H as an indicator of dynamic <span class="hlt">pressure</span> pulses occurrence from 2007 to 2016. The selection criteria for events are: (1) the increase in the index must be bigger than 10 [nT] and (2) the rise time must be in less than 5 minutes. Additionally, the events must occur under northward IMF and at the same time at least one spacecraft has to be located in the magnetosphere nightside. Using this methodology we found 66 <span class="hlt">pressure</span> pulse events for analysis. Most of them can be classified as step function <span class="hlt">pressure</span> pulses or as sudden impulses (increase followed immediately by a decrease of the dynamic <span class="hlt">pressure</span>). Under these two categories the results show some systematic signatures <span class="hlt">depending</span> of the location of the spacecraft. For both kind of <span class="hlt">pressure</span> pulse signatures, compressions are <span class="hlt">observed</span> on the dayside. However, on the nightside compressions and/or South-then-North magnetic signatures can be <span class="hlt">observed</span> for step function like <span class="hlt">pressure</span> pulses, meanwhile for the sudden impulse kind of <span class="hlt">pressure</span> pulses the magnetospheric response seems to be less global and more <span class="hlt">dependent</span> on the local conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PhRvL.111d3602W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PhRvL.111d3602W"><span><span class="hlt">Dependence</span> of the Radiation <span class="hlt">Pressure</span> on the Background Refractive Index</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Webb, Kevin J.</p> <p>2013-07-01</p> <p>The 1978 experiments by Jones and Leslie showing that the radiation <span class="hlt">pressure</span> on a mirror <span class="hlt">depends</span> on the background medium refractive index have yet to be adequately explained using a force model and have provided a leading challenge to the Abraham form of the electromagnetic momentum. Those experimental results are predicted for the first time using a force representation that incorporates the Abraham momentum by utilizing the power calibration method employed in the Jones and Leslie experiments. With an extension of the same procedure, the polarization and angle independence of the experimental data are also explained by this model. Prospects are good for this general form of the electromagnetic force density to be effective in predicting other experiments with macroscopic materials. Furthermore, the rigorous representation of material dispersion makes the representation important for metamaterials that operate in the vicinity of homogenized material resonances.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920059644&hterms=taylor&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D90%26Ntt%3Dtaylor%2Bt%2Bb','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920059644&hterms=taylor&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D90%26Ntt%3Dtaylor%2Bt%2Bb"><span>Atmosphere and climate studies of Mars using the Mars <span class="hlt">Observer</span> <span class="hlt">pressure</span> modulator infrared radiometer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mccleese, D. J.; Haskins, R. D.; Schofield, J. T.; Zurek, R. W.; Leovy, C. B.; Paige, D. A.; Taylor, F. W.</p> <p>1992-01-01</p> <p>Studies of the climate and atmosphere of Mars are limited at present by a lack of meteorological data having systematic global coverage with good horizontal and vertical resolution. The Mars <span class="hlt">Observer</span> spacecraft in a low, nearly circular, polar orbit will provide an excellent platform for acquiring the data needed to advance significantly our understanding of the Martian atmosphere and its remarkable variability. The Mars <span class="hlt">Observer</span> <span class="hlt">pressure</span> modulator infrared radiometer (PMIRR) is a nine-channel limb and nadir scanning atmospheric sounder which will <span class="hlt">observe</span> the atmosphere of Mars globally from 0 to 80 km for a full Martian year. PMIRR employs narrow-band radiometric channels and two <span class="hlt">pressure</span> modulation cells to measure atmospheric and surface emission in the thermal infrared. PMIRR infrared and visible measurements will be combined to determine the radiative balance of the polar regions, where a sizeable fraction of the global atmospheric mass annually condenses onto and sublimes from the surface. Derived meteorological fields, including diabatic heating and cooling and the vertical variation of horizontal winds, are computed from the globally mapped fields retrieved from PMIRR data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1705493','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1705493"><span><span class="hlt">Dependence</span> of Intramyocardial <span class="hlt">Pressure</span> and Coronary Flow on Ventricular Loading and Contractility: A Model 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>Borsje, Petra; Arts, Theo; van De Vosse, Frans N.</p> <p>2006-01-01</p> <p>The phasic coronary arterial inflow during the normal cardiac cycle has been explained with simple (waterfall, intramyocardial pump) models, emphasizing the role of ventricular <span class="hlt">pressure</span>. To explain changes in isovolumic and low afterload beats, these models were extended with the effect of three-dimensional wall stress, nonlinear characteristics of the coronary bed, and extravascular fluid exchange. With the associated increase in the number of model parameters, a detailed parameter sensitivity analysis has become difficult. Therefore we investigated the primary relations between ventricular <span class="hlt">pressure</span> and volume, wall stress, intramyocardial <span class="hlt">pressure</span> and coronary blood flow, with a mathematical model with a limited number of parameters. The model replicates several experimental <span class="hlt">observations</span>: the phasic character of coronary inflow is virtually independent of maximum ventricular <span class="hlt">pressure</span>, the amplitude of the coronary flow signal varies about proportionally with cardiac contractility, and intramyocardial <span class="hlt">pressure</span> in the ventricular wall may exceed ventricular <span class="hlt">pressure</span>. A parameter sensitivity analysis shows that the normalized amplitude of coronary inflow is mainly determined by contractility, reflected in ventricular <span class="hlt">pressure</span> and, at low ventricular volumes, radial wall stress. Normalized flow amplitude is less sensitive to myocardial coronary compliance and resistance, and to the relation between active fiber stress, time, and sarcomere shortening velocity. PMID:17048105</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17048105','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17048105"><span><span class="hlt">Dependence</span> of intramyocardial <span class="hlt">pressure</span> and coronary flow on ventricular loading and contractility: a model study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bovendeerd, Peter H M; Borsje, Petra; Arts, Theo; van De Vosse, Frans N</p> <p>2006-12-01</p> <p>The phasic coronary arterial inflow during the normal cardiac cycle has been explained with simple (waterfall, intramyocardial pump) models, emphasizing the role of ventricular <span class="hlt">pressure</span>. To explain changes in isovolumic and low afterload beats, these models were extended with the effect of three-dimensional wall stress, nonlinear characteristics of the coronary bed, and extravascular fluid exchange. With the associated increase in the number of model parameters, a detailed parameter sensitivity analysis has become difficult. Therefore we investigated the primary relations between ventricular <span class="hlt">pressure</span> and volume, wall stress, intramyocardial <span class="hlt">pressure</span> and coronary blood flow, with a mathematical model with a limited number of parameters. The model replicates several experimental <span class="hlt">observations</span>: the phasic character of coronary inflow is virtually independent of maximum ventricular <span class="hlt">pressure</span>, the amplitude of the coronary flow signal varies about proportionally with cardiac contractility, and intramyocardial <span class="hlt">pressure</span> in the ventricular wall may exceed ventricular <span class="hlt">pressure</span>. A parameter sensitivity analysis shows that the normalized amplitude of coronary inflow is mainly determined by contractility, reflected in ventricular <span class="hlt">pressure</span> and, at low ventricular volumes, radial wall stress. Normalized flow amplitude is less sensitive to myocardial coronary compliance and resistance, and to the relation between active fiber stress, time, and sarcomere shortening velocity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28134672','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28134672"><span>Effects of room environment and nursing experience on clinical blood <span class="hlt">pressure</span> measurement: an <span class="hlt">observational</span> study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Meng; Zhang, Xuemei; Chen, Fei; Dong, Birong; Chen, Aiqing; Zheng, Dingchang</p> <p>2017-04-01</p> <p>This study aimed to examine the effects of measurement room environment and nursing experience on the accuracy of manual auscultatory blood <span class="hlt">pressure</span> (BP) measurement. A training database with 32 Korotkoff sounds recordings from the British Hypertension Society was played randomly to 20 <span class="hlt">observers</span> who were divided into four groups according to the years of their nursing experience (i.e. ≥10 years, 1-9 years, nursing students with frequent training, and those without any medical background; five <span class="hlt">observers</span> in each group). All the <span class="hlt">observers</span> were asked to determine manual auscultatory systolic blood <span class="hlt">pressure</span> (SBP) and diastolic blood <span class="hlt">pressure</span> (DBP) both in a quiet clinical assessment room and in a noisy nurse station area. This procedure was repeated on another day, yielding a total of four measurements from each <span class="hlt">observer</span> (i.e. two room environments and two repeated determinations on 2 separate days) for each Korotkoff sound. The measurement error was then calculated against the reference answer, with the effects of room environment and nursing experience of the <span class="hlt">observer</span> investigated. Our results showed that there was no statistically significant difference for BPs measured under both quiet and noisy environments (P>0.80 for both SBP and DBP). However, there was a significant effect on the measurement accuracy between the <span class="hlt">observer</span> groups (P<0.001 for both SBP and DBP). The nursing students performed best with overall SBP and DBP errors of -0.8±2.4 and 0.1±1.8 mmHg, respectively. The SBP measurement error from the nursing students was significantly smaller than that for each of the other three groups (all P<0.001). Our results indicate that frequent nursing trainings are important for nurses to achieve accurate manual auscultatory BP measurement.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3610305','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3610305"><span>A multi-scale cardiovascular system model can account for the load-<span class="hlt">dependence</span> of the end-systolic <span class="hlt">pressure</span>-volume relationship</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>2013-01-01</p> <p>Background The end-systolic <span class="hlt">pressure</span>-volume relationship is often considered as a load-independent property of the heart and, for this reason, is widely used as an index of ventricular contractility. However, many criticisms have been expressed against this index and the underlying time-varying elastance theory: first, it does not consider the phenomena underlying contraction and second, the end-systolic <span class="hlt">pressure</span> volume relationship has been experimentally shown to be load-<span class="hlt">dependent</span>. Methods In place of the time-varying elastance theory, a microscopic model of sarcomere contraction is used to infer the <span class="hlt">pressure</span> generated by the contraction of the left ventricle, considered as a spherical assembling of sarcomere units. The left ventricle model is inserted into a closed-loop model of the cardiovascular system. Finally, parameters of the modified cardiovascular system model are identified to reproduce the hemodynamics of a normal dog. Results Experiments that have proven the limitations of the time-varying elastance theory are reproduced with our model: (1) preload reductions, (2) afterload increases, (3) the same experiments with increased ventricular contractility, (4) isovolumic contractions and (5) flow-clamps. All experiments simulated with the model generate different end-systolic <span class="hlt">pressure</span>-volume relationships, showing that this relationship is actually load-<span class="hlt">dependent</span>. Furthermore, we show that the results of our simulations are in good agreement with experiments. Conclusions We implemented a multi-scale model of the cardiovascular system, in which ventricular contraction is described by a detailed sarcomere model. Using this model, we successfully reproduced a number of experiments that have shown the failing points of the time-varying elastance theory. In particular, the developed multi-scale model of the cardiovascular system can capture the load-<span class="hlt">dependence</span> of the end-systolic <span class="hlt">pressure</span>-volume relationship. PMID:23363818</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('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2776685','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2776685"><span>NO-<span class="hlt">dependent</span> blood <span class="hlt">pressure</span> regulation in RGS2-deficient mice</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Obst, Michael; Tank, Jens; Plehm, Ralph; Blumer, Kendall J.; Diedrich, Andrè; Jordan, Jens; Luft, Friedrich C.; Gross, Volkmar</p> <p>2009-01-01</p> <p>The regulator of G protein signaling (RGS) 2, a GTPase-activating protein, is activated via the nitric oxide (NO)-cGMP pathway and thereby may influence blood <span class="hlt">pressure</span> regulation. To test that notion, we measured mean arterial blood <span class="hlt">pressure</span> (MAP) and heart rate (HR) with telemetry in Nω-nitro-L-arginine methyl ester (L-NAME, 5 mg L-NAME/10 ml tap water)-treated RGS2-deficient (RGS2−/−) and RGS2-sufficient (RGS2+/+) mice and assessed autonomic function. Without L-NAME, RGS2−/− mice showed during day and night a similar increase of MAP compared with controls. L-NAME treatment increased MAP in both strains. nNOS is involved in this L-NAME-<span class="hlt">dependent</span> blood <span class="hlt">pressure</span> increase, since 7-nitroindazole increased MAP by 8 and 9 mmHg (P < 0.05) in both strains. The L-NAME-induced MAP increase of 14–15 mmHg during night was similar in both strains. However, the L-NAME-induced MAP increase during the day was smaller in RGS2−/− than in RGS2+/+ (11 ± 1 vs. 17 ± 2 mmHg; P < 0.05). Urinary norepinephrine and epinephrine excretion was higher in RGS2−/− than in RGS2+/+ mice. The MAP decrease after prazosin was more pronounced in L-NAME-RGS2−/−. HR variability parameters [root mean square of successive differences (RMSSD), low-frequency (LF) power, and high-frequency (HF) power] and baroreflex sensitivity were increased in RGS2−/−. Atropine and atropine plus metoprolol markedly reduced RMSSD, LF, and HF. Our data suggest an interaction between RGS2 and the NO-cGMP pathway. The blunted L-NAME response in RGS2−/− during the day suggests impaired NO signaling. The MAP increases during the active phase in RGS2−/− mice may be related to central sympathetic activation and increased vascular adrenergic responsiveness. PMID:16269576</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JPhCS.751a2008B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JPhCS.751a2008B"><span><span class="hlt">Dependence</span> of optimal separative power of the “high-speed” Iguasu centrifuge on <span class="hlt">pressure</span> of working gas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bogovalov, S. V.; Borman, V. D.; Borisevich, V. D.; Davidenko, O. V.; Tronin, I. V.; Tronin, V. N.</p> <p>2016-09-01</p> <p>The results of optimization calculations of the separative power of the ’’high-speed” Iguasu gas centrifuge are presented. Iguasu gas centrifuge has the rotational speed of 1000 m/s, the rotor length of 1 m. The <span class="hlt">dependence</span> of the optimal separative power on the <span class="hlt">pressure</span> of the working gas on the rotor wall was obtained using the numerical simulations. It is shown, that maximum of the optimal separative power corresponds to the <span class="hlt">pressure</span> of 1100 mmHg. Maximum value of separative power is 31.9 SWU.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22113399','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22113399"><span>Protocol <span class="hlt">dependence</span> of mechanical properties in granular systems.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Inagaki, S; Otsuki, M; Sasa, S</p> <p>2011-11-01</p> <p>We study the protocol <span class="hlt">dependence</span> of the mechanical properties of granular media by means of computer simulations. We control a protocol of realizing disk packings in a systematic manner. In 2D, by keeping material properties of the constituents identical, we carry out compaction with various strain rates. The disk packings exhibit the strain rate <span class="hlt">dependence</span> of the critical packing fraction above which the <span class="hlt">pressure</span> becomes non-zero. The <span class="hlt">observed</span> behavior contrasts with the well-studied jamming transitions for frictionless disk packings. We also <span class="hlt">observe</span> that the elastic moduli of the disk packings <span class="hlt">depend</span> on the strain rate logarithmically. Our results suggest that there exists a time-<span class="hlt">dependent</span> state variable to describe macroscopic material properties of disk packings, which <span class="hlt">depend</span> on its protocol.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11927200','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11927200"><span>Accuracy of blood <span class="hlt">pressure</span> measurement and anthropometry among volunteer <span class="hlt">observers</span> in a large community survey.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Adams, Claire; Burke, Valerie; Beilin, Lawrie J</p> <p>2002-04-01</p> <p>The Busselton Survey is a population survey that is held about every three years. In 1994-1995 a re-survey was held of all past participants and 8,502 attended. Financial constraints precluded employing staff for data collection for blood <span class="hlt">pressure</span> and anthropometry, these therefore were collected by unpaid lay volunteers. Quality control by a health professional was critical to the assessment and maintenance of accuracy in these measurements. For blood <span class="hlt">pressure</span> three readings were taken simultaneously by a quality control person and the volunteer using a dual stethoscope. Duplicate anthropometric measurements were taken by a criterion anthropometrist and the volunteer. Inter and intra-<span class="hlt">observer</span> technical errors of measurement (TEM) were calculated. Sixty-two volunteers were trained to take BP measurements; of these, 38 collected data, and 63 were trained in anthropometry; of these, 30 were suitable as measurers. Training was conducted on a group and individual basis by the quality assurance person for the study both in the Perth metropolitan area and rural Busselton. The TEM for SBP was 1.6 mm Hg (SD 1.0 mm Hg) and 1.5 mm Hg (SD 0.8) for DBP. For skin-folds intra-<span class="hlt">observer</span> TEM ranged from 0.6 mm to 1.0 mm. Between-<span class="hlt">observer</span> TEM ranged from 2.1 mm to 5.4 mm. For limb and waist circumferences, intra-<span class="hlt">observer</span> TEM ranged from 0.3 cm to 1.6 cm. Between-<span class="hlt">observer</span> TEM for circumferences ranged from 0.5 cm to 1.9 cm. Unpaid volunteer measurers can, if carefully trained and supervised, provide acceptable blood <span class="hlt">pressure</span> data and anthropometry in large population surveys.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1386649-pressure-dependence-oxygen-isotope-exchange-rates-between-solution-apical-oxygen-atoms-uo2-oh-ion','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1386649-pressure-dependence-oxygen-isotope-exchange-rates-between-solution-apical-oxygen-atoms-uo2-oh-ion"><span>The <span class="hlt">Pressure</span> <span class="hlt">Dependence</span> of Oxygen Isotope Exchange Rates Between Solution and Apical Oxygen Atoms on the [UO2(OH)4]2- Ion</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>Harley, Steven J.; Ohlin, C. André; Johnson, Rene L.</p> <p>2011-04-06</p> <p>Under <span class="hlt">pressure</span>: The <span class="hlt">pressure</span> <span class="hlt">dependence</span> of isotope exchange rate was determined for apical oxygen atoms in the [UO2(OH)4]2-(aq) ion (see picture). The results can be interpreted to indicate an associative character of the reaction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JaJAP..57e8001I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JaJAP..57e8001I"><span>Miniature microwave plasmas generated in high <span class="hlt">pressure</span> argon</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Inoue, Kenichi; Stauss, Sven; Kim, Jaeho; Ito, Tsuyohito; Terashima, Kazuo</p> <p>2018-05-01</p> <p>Miniature microwave plasmas with diameters of approximately 1 mm were generated in high-<span class="hlt">pressure</span> argon (0.1–5.0 MPa) using a microgap electrode. The microwave power required to sustain plasmas was 1–10 W, <span class="hlt">depending</span> on the <span class="hlt">pressure</span>. Strong electron-neutral bremsstrahlung emission, indicating an electron temperature of approximately 12000 K, was <span class="hlt">observed</span> at high <span class="hlt">pressures</span> (>1 MPa), and electron densities estimated from Stark broadening revealed high values on the order of 1023 m‑3. The analysis confirmed that the coefficient for the <span class="hlt">pressure</span> shift of the Ar I line at 696.5 nm reported by Copley and Camm can be extended to 5 MPa.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18848568','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18848568"><span>Bacteriophage T5 DNA ejection under <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>Leforestier, A; Brasilès, S; de Frutos, M; Raspaud, E; Letellier, L; Tavares, P; Livolant, F</p> <p>2008-12-19</p> <p>The transfer of the bacteriophage genome from the capsid into the host cell is a key step of the infectious process. In bacteriophage T5, DNA ejection can be triggered in vitro by simple binding of the phage to its purified Escherichia coli receptor FhuA. Using electrophoresis and cryo-electron microscopy, we measure the extent of DNA ejection as a function of the external osmotic <span class="hlt">pressure</span>. In the high <span class="hlt">pressure</span> range (7-16 atm), the amount of DNA ejected decreases with increasing <span class="hlt">pressure</span>, as theoretically predicted and <span class="hlt">observed</span> for lambda and SPP1 bacteriophages. In the low and moderate <span class="hlt">pressure</span> range (2-7 atm), T5 exhibits an unexpected behavior. Instead of a unique ejected length, multiple populations coexist. Some phages eject their complete genome, whereas others stop at some nonrandom states that do not <span class="hlt">depend</span> on the applied <span class="hlt">pressure</span>. We show that contrarily to what is <span class="hlt">observed</span> for the phages SPP1 and lambda, T5 ejection cannot be explained as resulting from a simple <span class="hlt">pressure</span> equilibrium between the inside and outside of the capsid. Kinetics parameters and/or structural characteristics of the ejection machinery could play a determinant role in T5 DNA ejection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1371020-pressure-dependent-structure-null-scattering-alloy-ti-zr','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1371020-pressure-dependent-structure-null-scattering-alloy-ti-zr"><span><span class="hlt">Pressure-dependent</span> structure of the null-scattering alloy Ti 0.676 Zr 0.324</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>Zeidler, Anita; Guthrie, Malcolm; Salmon, Philip S.</p> <p>2015-05-13</p> <p>The room temperature structure of the alloy Ti0.676Zr0.324Ti0.676Zr0.324 was measured by X-ray diffraction under compression at <span class="hlt">pressures</span> up to ~30GPa. This alloy is used as a construction material in high <span class="hlt">pressure</span> neutron-scattering research and has a mean coherent neutron scattering length of zero, that is, it is a so-called null-scattering alloy. A broad phase transition was <span class="hlt">observed</span> from a hexagonal close-packed α-phase to a hexagonal ω-phase, which started at a <span class="hlt">pressure</span> of ≲12GPa≲12GPa and was completed by ~25GPa. The data for the α-phase were fitted by using a third-order Birch–Murnaghan equation of state, giving an isothermal bulk modulus B0=87(4)GPaB0=87(4)GPa andmore » <span class="hlt">pressure</span> derivative B'0=6.6(8)B0'=6.6(8). The results will help to ensure that accurate structural information can be gained from in situ high <span class="hlt">pressure</span> neutron diffraction work on amorphous and liquid materials where the Ti0.676Zr0.324Ti0.676Zr0.324 alloy is used as a gasket material.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15645764','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15645764"><span>[Having trouble with <span class="hlt">pressure</span> ulcers care?].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mizuno, Masako; Noda, Yasuhiro; Nohara, Yoko; Fujii, Keiko; Sato, Noriko; Renda, Akiyoshi; Yuasa, Takashi; Muramatsu, Shuichi; Furuta, Katsunori</p> <p>2004-12-01</p> <p>Since 1997, we, the community pharmacists, have established this society, Aichi Prefecture Society for the Study of <span class="hlt">Pressure</span> Ulcers Care, in order to furnish drug information about <span class="hlt">pressure</span> ulcers care. Moist atmosphere is required for the healing of <span class="hlt">pressure</span> ulcers. The moist environment that could be regulated <span class="hlt">depends</span> on the physicochemical property of ointment bases. Therefore, ointment should reasonably be chosen to adjust the moisture. Since 2000, we have been committed to providing pharmacists, who work on home care, with a booklet to instruct how to choose ointments for <span class="hlt">pressure</span> ulcers treatment. In 2002, when the Aichi pharmaceutical association held a training conference held at various hospitals using the booklet as a teaching material, hospital pharmacists cooperated by making a field study trip to <span class="hlt">observe</span> <span class="hlt">pressure</span> ulcers treatments. Nowadays researchers at pharmaceutical colleges have also cooperated in studying the efficacy and economical effect of the method of blending different ointments to improve the healing process of <span class="hlt">pressure</span> ulcers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880041333&hterms=superconducting+gravity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dsuperconducting%2Bgravity','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880041333&hterms=superconducting+gravity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dsuperconducting%2Bgravity"><span><span class="hlt">Pressure</span> <span class="hlt">dependence</span> of the electrical properties of GaBi solidified in low gravity</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wu, M. K.; Ashburn, J. R.; Torng, C. J.; Curreri, P. A.; Chu, C. W.</p> <p>1987-01-01</p> <p>Immiscible GaBi alloys were solidified during free fall in the NASA Marshall Space Flight Center drop tower, which provides about 4.5 seconds of low gravity. The electrical resistivity and magnetic susceptibility were measured as a function of <span class="hlt">pressure</span> (up to 18 kbar) and temperature (300 K to 4.2 K) of drop tower (DT) and ground control (GC) samples prepared under identical conditions, except for gravity. At ambient <span class="hlt">pressure</span> the electrical resistance of the DT sample exhibits a broad maximum at 100 K, while that of GC sample decreases rapidly as temperature decreases. Both DT and GC samples become superconducting at 7.7 K. However, a minor second superconducting phase with a transition temperature at 8.3 K is <span class="hlt">observed</span> only in the DT samples.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ZNatA..72..843C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ZNatA..72..843C"><span>The <span class="hlt">Pressure</span> <span class="hlt">Dependence</span> of Structural, Electronic, Mechanical, Vibrational, and Thermodynamic Properties of Palladium-Based Heusler Alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Çoban, Cansu</p> <p>2017-08-01</p> <p>The <span class="hlt">pressure</span> <span class="hlt">dependent</span> behaviour of the structural, electronic, mechanical, vibrational, and thermodynamic properties of Pd2TiX (X=Ga, In) Heusler alloys was investigated by ab initio calculations. The lattice constant, the bulk modulus and its first <span class="hlt">pressure</span> derivative, the electronic band structure and the density of states (DOS), mechanical properties such as elastic constants, anisotropy factor, Young's modulus, etc., the phonon dispersion curves and phonon DOS, entropy, heat capacity, and free energy were obtained under <span class="hlt">pressure</span>. It was determined that the calculated lattice parameters are in good agreement with the literature, the elastic constants obey the stability criterion, and the phonon dispersion curves have no negative frequency which shows that the compounds are stable. The band structures at 0, 50, and 70 GPa showed valence instability at the L point which explains the superconductivity in Pd2TiX (X=Ga, In).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22515476','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22515476"><span>Implementation of <span class="hlt">pressure</span> ulcer prevention best practice recommendations in acute care: an <span class="hlt">observational</span> study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Barker, Anna Lucia; Kamar, Jeannette; Tyndall, Tamara Jane; White, Lyn; Hutchinson, Anastasia; Klopfer, Nicole; Weller, Carolina</p> <p>2013-06-01</p> <p><span class="hlt">Pressure</span> ulcers are a common but preventable problem in hospitals. Implementation of best practice guideline recommendations can prevent ulcers from occurring. This 9-year cohort study reports prevalence data from point prevalence surveys during the <span class="hlt">observation</span> period, and three practice metrics to assess implementation of best practice guideline recommendations: (i) nurse compliance with use of a validated <span class="hlt">pressure</span> ulcer risk assessment and intervention checklist; (ii) accuracy of risk assessment scoring in usual-care nurses and experienced injury prevention nurses; and (iii) use of <span class="hlt">pressure</span> ulcer prevention strategies. The prevalence of hospital-acquired <span class="hlt">pressure</span> ulcers decreased following implementation of an evidence-based prevention programme from 12·6% (2 years preprogramme implementation) to 2·6% (6 years postprogramme implementation) (P < 0·001). Audits between 2003 and 2011 of 4368 patient medical records identified compliance with <span class="hlt">pressure</span> ulcer prevention documentation according to best practice guidelines was high (>84%). A sample of 270 patients formed the sample for the study of risk assessment scoring accuracy and use of prevention strategies. It was found usual-care nurses under-estimated patients' risk of <span class="hlt">pressure</span> ulcer development and under-utilised prevention strategies compared with experienced injury prevention nurses. Despite a significant reduction in prevalence of hospital-acquired <span class="hlt">pressure</span> ulcers and high documentation compliance, use of prevention strategies could further be improved to achieve better patient outcomes. Barriers to the use of prevention strategies by nurses in the acute hospital setting require further examination. This study provides important insights into the knowledge translation of <span class="hlt">pressure</span> ulcer prevention best practice guideline recommendations at The Northern Hospital. © 2012 The Authors. International Wound Journal © 2012 John Wiley & Sons Ltd and Medicalhelplines.com Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25791135','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25791135"><span>Rate-<span class="hlt">dependent</span> elastic hysteresis during the peeling of <span class="hlt">pressure</span> sensitive adhesives.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Villey, Richard; Creton, Costantino; Cortet, Pierre-Philippe; Dalbe, Marie-Julie; Jet, Thomas; Saintyves, Baudouin; Santucci, Stéphane; Vanel, Loïc; Yarusso, David J; Ciccotti, Matteo</p> <p>2015-05-07</p> <p>The modelling of the adherence energy during peeling of <span class="hlt">Pressure</span> Sensitive Adhesives (PSA) has received much attention since the 1950's, uncovering several factors that aim at explaining their high adherence on most substrates, such as the softness and strong viscoelastic behaviour of the adhesive, the low thickness of the adhesive layer and its confinement by a rigid backing. The more recent investigation of adhesives by probe-tack methods also revealed the importance of cavitation and stringing mechanisms during debonding, underlining the influence of large deformations and of the related non-linear response of the material, which also intervenes during peeling. Although a global modelling of the complex coupling of all these ingredients remains a formidable issue, we report here some key experiments and modelling arguments that should constitute an important step forward. We first measure a non-trivial <span class="hlt">dependence</span> of the adherence energy on the loading geometry, namely through the influence of the peeling angle, which is found to be separable from the peeling velocity <span class="hlt">dependence</span>. This is the first time to our knowledge that such adherence energy <span class="hlt">dependence</span> on the peeling angle is systematically investigated and unambiguously demonstrated. Secondly, we reveal an independent strong influence of the large strain rheology of the adhesives on the adherence energy. We complete both measurements with a microscopic investigation of the debonding region. We discuss existing modellings in light of these measurements and of recent soft material mechanics arguments, to show that the adherence energy during peeling of PSA should not be associated to the propagation of an interfacial stress singularity. The relevant deformation mechanisms are actually located over the whole adhesive thickness, and the adherence energy during peeling of PSA should rather be associated to the energy loss by viscous friction and by rate-<span class="hlt">dependent</span> elastic hysteresis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.9546Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.9546Z"><span>Unusual properties of high-compliance porosity extracted from measurements of <span class="hlt">pressure-dependent</span> wave velocities in rocks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zaitsev, Vladimir Y.; Radostin, Andrey V.; Pasternak, Elena; Dyskin, Arcady</p> <p>2016-04-01</p> <p>Conventionally the interpretation of wave velocities and their variations under load is conducted assuming that closable cracks have simple planar shapes, like the popular model of penny-shape cracks. For such cracks, the proportion between complementary variations in different elastic parameters of rocks (such as S- and P-wave velocities) is strictly pre-determined, in particular, it is independent of the crack aspect ratio and rather weakly <span class="hlt">dependent</span> on the Poisson's ratio of the intact rock. Real rocks, however, contain multitude of cracks of different geometry. Faces of such cracks can exhibit complex modes of interaction when closed by external load, which may result in very different ratios between normal- and shear compliances of such defects. In order to describe the reduction of different elastic moduli, we propose a model in which the compliances of crack-like defects are explicitly decoupled and are not predetermined, so that the ratio q between total normal- and shear- compliances imparted to the rock mass (as well as individual values of these compliances) can be estimated from experimental data on reduction of different elastic moduli (e.g., <span class="hlt">pressure</span> <span class="hlt">dependences</span> of P- and S-wave velocities). Physically, the so-extracted ratio q can be interpreted as intrinsic property of individual crack-like defects similar to each other, or as a characteristic of proportion between concentrations of pure normal cracks with very large q and pure shear cracks with q→0. The latter case can correspond, e.g., to saturated cracks in which weakly-compressible liquid prevents crack closing under normal loading. It can be shown that for conventional dry planar cracks, the compliance ratio is q ˜2. The developed model applied to the data on wave-velocity variations with external <span class="hlt">pressure</span> indicates that elastic properties of the real crack-like defects in rocks can differ considerably from the usually assumed ones. Comparison with experimental data on variations P- and S</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=solute&pg=4&id=EJ305849','ERIC'); return false;" href="https://eric.ed.gov/?q=solute&pg=4&id=EJ305849"><span>Textbook Forum: Equilibrium Constants of Chemical Reactions Involving Condensed Phases: <span class="hlt">Pressure</span> <span class="hlt">Dependence</span> and Choice of Standard State.</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>Perlmutter-Hayman, Berta</p> <p>1984-01-01</p> <p>Problems of equilibria in condensed phases (particularly those involving solutes in dilute solutions) are encountered by students in their laboratory work; the thermodynamics of these equilibria is neglected in many textbooks. Therefore, several aspects of this topic are explored, focusing on <span class="hlt">pressure</span> <span class="hlt">dependence</span> and choice of standard state. (JN)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29478971','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29478971"><span>Kidney Mass Reduction Leads to l-Arginine Metabolism-<span class="hlt">Dependent</span> Blood <span class="hlt">Pressure</span> Increase in Mice.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pillai, Samyuktha Muralidharan; Seebeck, Petra; Fingerhut, Ralph; Huang, Ji; Ming, Xiu-Fen; Yang, Zhihong; Verrey, François</p> <p>2018-02-25</p> <p>Uninephrectomy (UNX) is performed for various reasons, including kidney cancer or donation. Kidneys being the main site of l-arginine production in the body, we tested whether UNX mediated kidney mass reduction impacts l-arginine metabolism and thereby nitric oxide production and blood <span class="hlt">pressure</span> regulation in mice. In a first series of experiments, we <span class="hlt">observed</span> a significant increase in arterial blood <span class="hlt">pressure</span> 8 days post-UNX in female and not in male mice. Further experimental series were performed in female mice, and the blood <span class="hlt">pressure</span> increase was confirmed by telemetry. l-citrulline, that is used in the kidney to produce l-arginine, was elevated post-UNX as was also asymmetric dimethylarginine, an inhibitor of nitric oxide synthase that competes with l-arginine and is a marker for renal failure. Interestingly, the UNX-induced blood <span class="hlt">pressure</span> increase was prevented by supplementation of the diet with 5% of the l-arginine precursor, l-citrulline. Because l-arginine is metabolized in the kidney and other peripheral tissues by arginase-2, we tested whether the lack of this metabolic pathway also compensates for decreased l-arginine production in the kidney and/or for local nitric oxide synthase inhibition and consecutive blood <span class="hlt">pressure</span> increase. Indeed, upon uninephrectomy, arginase-2 knockout mice (Arg-2 -/- ) neither displayed an increase in asymmetric dimethylarginine and l-citrulline plasma levels nor a significant increase in blood <span class="hlt">pressure</span>. UNX leads to a small increase in blood <span class="hlt">pressure</span> that is prevented by l-citrulline supplementation or arginase deficiency, 2 measures that appear to compensate for the impact of kidney mass reduction on l-arginine metabolism. © 2018 The Authors. Published on behalf of the American Heart Association, Inc., by Wiley.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870062092&hterms=atmospheric+pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Datmospheric%2Bpressure','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870062092&hterms=atmospheric+pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Datmospheric%2Bpressure"><span>Time and space variability of spectral estimates of atmospheric <span class="hlt">pressure</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Canavero, Flavio G.; Einaudi, Franco</p> <p>1987-01-01</p> <p>The temporal and spatial behaviors of atmospheric <span class="hlt">pressure</span> spectra over the northern Italy and the Alpine massif were analyzed using data on surface <span class="hlt">pressure</span> measurements carried out at two microbarograph stations in the Po Valley, one 50 km south of the Alps, the other in the foothills of the Dolomites. The first 15 days of the study overlapped with the Alpex Intensive <span class="hlt">Observation</span> Period. The <span class="hlt">pressure</span> records were found to be intrinsically nonstationary and were found to display substantial time variability, implying that the statistical moments <span class="hlt">depend</span> on time. The shape and the energy content of spectra <span class="hlt">depended</span> on different time segments. In addition, important differences existed between spectra obtained at the two stations, indicating a substantial effect of topography, particularly for periods less than 40 min.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhRvC..86e4001C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhRvC..86e4001C"><span>Quark-mass <span class="hlt">dependence</span> of two-nucleon <span class="hlt">observables</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Jiunn-Wei; Lee, Tze-Kei; Liu, C.-P.; Liu, Yu-Sheng</p> <p>2012-11-01</p> <p>We study the potential implications of lattice QCD determinations of the S-wave nucleon-nucleon scattering lengths with unphysical light quark masses. If the light quark masses are small enough such that nuclear effective field theory (NEFT) can be used to perform quark-mass extrapolations, then the leading quark-mass <span class="hlt">dependence</span> of not only the effective range and the two-body current, but also all the low-energy deuteron matrix elements up to next-to-leading-order in NEFT can be obtained. As a proof of principle, we compute the quark-mass <span class="hlt">dependence</span> of the deuteron charge radius, magnetic moment, polarizability, and the deuteron photodisintegration cross section using the lattice calculation of the scattering lengths at 354 MeV pion mass by the ``Nuclear Physics with Lattice QCD'' (NPLQCD) collaboration and the NEFT power counting scheme of Beane, Kaplan, and Vuorinen (BKV), even though it is not yet established that the 354 MeV pion mass is within the radius of convergence of the BKV scheme. Once the lattice result with quark mass within the NEFT radius of convergence is obtained, our <span class="hlt">observation</span> can be used to constrain the time variation of isoscalar combination of u and d quark mass mq, to help the anthropic principle study to find the mq range that allows the existence of life, and to provide a weak test of the multiverse conjecture.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPA....7l5009R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPA....7l5009R"><span><span class="hlt">Pressure</span> <span class="hlt">dependence</span> of resistivity and magnetic properties in a Mn1.9Cr0.1Sb alloy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Repaka, D. V. Maheswar; Sharma, Vinay; Chanda, Amit; Mahendiran, R.; Ramanujan, R. V.</p> <p>2017-12-01</p> <p>We report magnetic-field and hydrostatic <span class="hlt">pressure</span> <span class="hlt">dependent</span> electrical resistivity and magnetic properties of a Mn1.9Cr0.1Sb alloy. Upon cooling, the magnetization of Mn1.9Cr0.1Sb exhibits a first-order ferrimagnetic to antiferromagnetic transition at the exchange inversion temperature, TS = 261 K under a 0.1 T magnetic field. Our experimental results show that TS decreases with increasing magnetic field but increase with increasing hydrostatic <span class="hlt">pressure</span>. The <span class="hlt">pressure</span> induced transition is accompanied by a large positive baro-resistance of 30.5% for a hydrostatic <span class="hlt">pressure</span> change of 0.69 GPa. These results show that the lattice parameters as well as the bond distance between Mn-Mn atoms play a crucial role in the magnetic and electronic transport properties of Mn1.9Cr0.1Sb. This sample also exhibits a large inverse magnetocaloric effect with a magnetic entropy change of ΔSm = +6.75 J/kg.K and negative magnetoresistance (44.5%) for a field change of 5 T at TS in ambient <span class="hlt">pressure</span> which may be useful for magnetic cooling and spintronics applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1918095C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1918095C"><span>Fracture propagation during fluid injection experiments in shale at elevated confining <span class="hlt">pressures</span>.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chandler, Mike; Mecklenburgh, Julian; Rutter, Ernest; Fauchille, Anne-Laure; Taylor, Rochelle; Lee, Peter</p> <p>2017-04-01</p> <p>The use of hydraulic fracturing to recover shale-gas has focused attention upon the fundamental fracture properties of gas-bearing shales. Fracture propagation trajectories in these materials <span class="hlt">depend</span> on the interaction between the anisotropic mechanical properties of the shale and the anisotropic in-situ stress field. However, there is a general paucity of available experimental data on their anisotropic mechanical, physical and fluid-flow properties, especially at elevated confining <span class="hlt">pressures</span>. Here we report the results of laboratory-scale fluid injection experiments, for Whitby mudstone and Mancos shale (an interbedded silt and mudstone), as well as Pennant sandstone (a tight sandstone with permeability similar to shales), which is used an isotropic baseline and tight-gas sandstone analogue. Our injection experiments involved the pressurisation of a blind-ending central hole in an initially dry cylindrical sample. Pressurisation was conducted under constant volume-rate control, using silicone oils of various viscosities. The <span class="hlt">dependence</span> of breakdown <span class="hlt">pressure</span> on confining <span class="hlt">pressure</span> was seen to be <span class="hlt">dependent</span> on the rock strength, with the significantly stronger Pennant sandstone exhibiting much lower confining-<span class="hlt">pressure</span> <span class="hlt">dependence</span> of breakdown <span class="hlt">pressure</span> than the weaker shales. In most experiments, a small drop in the injection <span class="hlt">pressure</span> record was <span class="hlt">observed</span> at what is taken to be fracture initiation, and in the Pennant sandstone this was accompanied by a small burst of acoustic energy. Breakdown was found to be rapid and uncontrollable after initiation if injection is continued, but can be limited to a slower (but still uncontrolled) rate by ceasing the injection of fluid after the breakdown initiation in experiments where it could be identified. A simplified 2-dimensional model for explaining these <span class="hlt">observations</span> is presented in terms of the stress intensities at the tip of a pressurised crack. Additionally, we present a suite of supporting mechanical, flow and elastic</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.osti.gov/pages/biblio/1286756-high-pressure-dynamics-hydrated-protein-bioprotective-trehalose-environment','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1286756-high-pressure-dynamics-hydrated-protein-bioprotective-trehalose-environment"><span>High-<span class="hlt">pressure</span> dynamics of hydrated protein in bioprotective trehalose environment</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Diallo, S. O.; Zhang, Q.; O'Neill, H.; ...</p> <p>2014-10-30</p> <p>Here we present a <span class="hlt">pressure-dependence</span> study of the dynamics of lysozyme protein powder immersed in deuterated , α-trehalose environment via quasielastic neutron scattering (QENS). The goal is to assess the baroprotective benefits of trehalose on biomolecules by comparing the findings with those of a trehalose-free reference study. While the mean-square displacement of the trehalose-free protein (hydrated to d D₂O ≃40 w%) as a whole, is reduced by increasing <span class="hlt">pressure</span>, the actual <span class="hlt">observable</span> relaxation dynamics in the picoseconds to nanoseconds time range remains largely unaffected by <span class="hlt">pressure</span> up to the maximum investigated <span class="hlt">pressure</span> of 2.78(2) Kbar. Our <span class="hlt">observation</span> is independent ofmore » whether or not the protein is mixed with the deuterated sugar. This suggests that the hydrated protein s conformational states at atmospheric <span class="hlt">pressure</span> remain unaltered by hydrostatic <span class="hlt">pressures</span>, below 2.78 Kbar. We also found the QENS response to be totally recoverable after ambient <span class="hlt">pressure</span> conditions are restored. Small-angle neutron diffraction measurements confirm that the protein-protein correlation remains undisturbed.We <span class="hlt">observe</span>, however, a clear narrowing of the QENS response as the temperature is decreased from 290 to 230 K in both cases, which we parametrize using the Kohlrausch-Williams-Watts stretched exponential model. Finally, only the fraction of protons that are immobile on the accessible time window of the instrument, referred to as the elastic incoherent structure factor, is <span class="hlt">observably</span> sensitive to <span class="hlt">pressure</span>, increasing only marginally but systematically with increasing <span class="hlt">pressure</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI23B..06W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI23B..06W"><span>The <span class="hlt">Pressure</span> <span class="hlt">Dependence</span> of Thermal Expansion of Core-Forming Alloys: A Key Parameter in Determining the Convective Style of Planetary Cores</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Williams, Q. C.; Manghnani, M. H.</p> <p>2017-12-01</p> <p>The convective style of planetary cores is critically <span class="hlt">dependent</span> on the thermal properties of iron alloys. In particular, the relation between the adiabatic gradient and the melting curve governs whether planetary cores solidify from their top down (when the adiabat is steeper than the melting curve) or the bottom up (the converse). Molten iron alloys, in general, have large, ambient <span class="hlt">pressure</span> thermal expansions: values in excess of 1.2 x 10^-4/K are dictated by data derived from levitated and sessile drop techniques. These high values of the thermal expansion imply that the adiabatic gradients within early planetesimals and present day moons that have comparatively low-<span class="hlt">pressure</span>, iron-rich cores are steep (typically greater than 35 K/GPa at low <span class="hlt">pressures</span>): values, at low <span class="hlt">pressures</span>, that are greater than the slope of the melting curve, and hence show that the cores of small solar system objects probably crystallize from the top-down. Here, we deploy a different manifestation of these large values of thermal expansion to determine the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of thermal expansion in iron-rich liquids: a difficult parameter to experimentally measure, and critical for determining the size range of cores in which top-down core solidification predominates. In particular, the difference between the adiabatic and isothermal bulk moduli of iron liquids is in the 20-30% range at the melting temperature, and scales as the product of the thermal expansion, the Grüneisen parameter, and the temperature. Hence, ultrasonic (and adiabatic) moduli of iron alloy liquids, when coupled with isothermal sink-float measurements, can yield quantitative constraints on the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of thermal expansion. For liquid iron alloys containing 17 wt% Si, we find that the thermal expansion is reduced by 50% over the first 8 GPa of compression. This "squeezing out" of the anomalously high low-<span class="hlt">pressure</span> thermal expansion of iron-rich alloys at relatively modest conditions likely limits the size</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRA..122.9723M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRA..122.9723M"><span>Statistical Study of Relations Between the Induced Magnetosphere, Ion Composition, and <span class="hlt">Pressure</span> Balance Boundaries Around Mars Based On MAVEN <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matsunaga, Kazunari; Seki, Kanako; Brain, David A.; Hara, Takuya; Masunaga, Kei; Mcfadden, James P.; Halekas, Jasper S.; Mitchell, David L.; Mazelle, Christian; Espley, J. R.; Gruesbeck, Jacob; Jakosky, Bruce M.</p> <p>2017-09-01</p> <p>Direct interaction between the solar wind (SW) and the Martian upper atmosphere forms a characteristic region, called the induced magnetosphere between the magnetosheath and the ionosphere. Since the SW deceleration due to increasing mass loading by heavy ions plays an important role in the induced magnetosphere formation, the ion composition is also expected to change around the induced magnetosphere boundary (IMB). Here we report on relations of the IMB, the ion composition boundary (ICB), and the <span class="hlt">pressure</span> balance boundary based on a statistical analysis of about 8 months of simultaneous ion, electron, and magnetic field <span class="hlt">observations</span> by Mars Atmosphere and Volatile EvolutioN (MAVEN) mission. We chose the period when MAVEN <span class="hlt">observed</span> the SW directly near its apoapsis to investigate their <span class="hlt">dependence</span> on SW parameters. Results show that IMBs almost coincide with ICBs on the dayside and locations of all three boundaries are affected by the SW dynamic <span class="hlt">pressure</span>. A remarkable feature is that all boundaries tend to locate at higher altitudes in the southern hemisphere than in the northern hemisphere on the nightside. This clear geographical asymmetry is permanently seen regardless of locations of the strong crustal B fields in the southern hemisphere, while the boundary locations become higher when the crustal B fields locate on the dayside. On the nightside, IMBs usually locate at higher altitude than ICBs. However, ICBs are likely to be located above IMBs in the nightside, southern, and downward ESW hemisphere when the strong crustal B fields locate on the dayside.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24274156','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24274156"><span>The influence of student characteristics on the <span class="hlt">dependability</span> of behavioral <span class="hlt">observation</span> data.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Briesch, Amy M; Volpe, Robert J; Ferguson, Tyler David</p> <p>2014-06-01</p> <p>Although generalizability theory has been used increasingly in recent years to investigate the <span class="hlt">dependability</span> of behavioral estimates, many of these studies have relied on use of general education populations as opposed to those students who are most likely to be referred for assessment due to problematic classroom behavior (e.g., inattention, disruption). The current study investigated the degree to which differences exist in terms of the magnitude of both variance component estimates and <span class="hlt">dependability</span> coefficients between students nominated by their teachers for Tier 2 interventions due to classroom behavior problems and a general classroom sample (i.e., including both nominated and non-nominated students). The academic engagement levels of 16 (8 nominated, 8 non-nominated) middle school students were measured by 4 trained <span class="hlt">observers</span> using momentary time-sampling procedures. A series of G and D studies were then conducted to determine whether the 2 groups were similar in terms of the (a) distribution of rating variance and (b) number of <span class="hlt">observations</span> needed to achieve an adequate level of <span class="hlt">dependability</span>. Results suggested that the behavior of students in the teacher-nominated group fluctuated more across time and that roughly twice as many <span class="hlt">observations</span> would therefore be required to yield similar levels of <span class="hlt">dependability</span> compared with the combined group. These findings highlight the importance of constructing samples of students that are comparable to those students with whom the measurement method is likely to be applied when conducting psychometric investigations of behavioral assessment tools. PsycINFO Database Record (c) 2014 APA, all rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12487321','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12487321"><span>Camphor-Crataegus berry extract combination dose-<span class="hlt">dependently</span> reduces tilt induced fall in blood <span class="hlt">pressure</span> in orthostatic hypotension.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Belz, G G; Butzer, R; Gaus, W; Loew, D</p> <p>2002-10-01</p> <p>In order to test the efficacy of a combination of natural D-camphor and an extract of fresh crataegus berries (Korodin Herz-Kreislauf-Tropfen) on orthostatic hypotension, two similar, controlled, randomized studies were carried out in a balanced crossover design in 24 patients each with orthostatic dysregulation. The camphor-crataegus berry combination (CCC) was orally administered as a single regimen in 3 different dosages of 5 drops, 20 drops and 80 drops; a placebo with 20 drops of a 60% alcoholic solution served as control. Orthostatic hypotension was assessed with the tilt table test before and after medication. Source data of both studies were pooled and meta-analytically evaluated for all 48 patients. CCC drops decreased the orthostatic fall in blood <span class="hlt">pressure</span> versus placebo, as almost uniformly established at all times by mean arterial <span class="hlt">pressure</span> and diastolic blood <span class="hlt">pressure</span>. Mean arterial <span class="hlt">pressure</span> demonstrated the very fast onset of action by a clearly dose-<span class="hlt">dependent</span> statistically significant effect even after 1-minute orthostasis. Increase of mean arterial <span class="hlt">pressure</span> as compared to the orthostasis test before medication was on average 4.5 mmHg. CCC affected diastolic blood <span class="hlt">pressure</span> after 1 minute of orthostasis in all dosages as compared to placebo. A statistically significant effect of the highest dose of 80 drops on diastolic blood <span class="hlt">pressure</span> could be demonstrated after 1-, 3-, and 5-minute orthostasis. The hemodynamic findings of a stabilizing effect on arterial <span class="hlt">pressure</span> in orthostasis corroborate the long-term medical experience with CCC and justify the indication orthostatic hypotension.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1185755-anomalous-pressure-dependence-thermal-conductivities-large-mass-ratio-compounds','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1185755-anomalous-pressure-dependence-thermal-conductivities-large-mass-ratio-compounds"><span>Anomalous <span class="hlt">pressure</span> <span class="hlt">dependence</span> of thermal conductivities of large mass ratio compounds</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Lindsay, Lucas R; Broido, David A.; Carrete, Jesus; ...</p> <p>2015-03-27</p> <p>The lattice thermal conductivities (k) of binary compound materials are examined as a function of hydrostatic <span class="hlt">pressure</span> P using a first-principles approach. Compound materials with relatively small mass ratios, such as MgO, show an increase in k with P, consistent with measurements. Conversely, compounds with large mass ratios (e.g., BSb, BAs, BeTe, BeSe) exhibit decreasing with increasing P, a behavior that cannot be understood using simple theories of k. This anomalous P <span class="hlt">dependence</span> of k arises from the fundamentally different nature of the intrinsic scattering processes for heat-carrying acoustic phonons in large mass ratio compounds compared to those with smallmore » mass ratios. We find this work demonstrates the power of first principles methods for thermal properties and advances the understanding of thermal transport in non-metals.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhyB..536..427M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhyB..536..427M"><span><span class="hlt">Pressure</span> and magnetic field effects on the valence transition of EuRh2Si2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mitsuda, Akihiro; Kishaba, Eigo; Fujimoto, Takumi; Oyama, Kohei; Wada, Hirofumi; Mizumaki, Masaichiro; Kawamura, Naomi; Ishimatsu, Naoki</p> <p>2018-05-01</p> <p>We have measured the X-ray absorption spectra (XAS), electrical resistivity and magnetic susceptibility of EuRh2Si2, which undergoes a valence transition under high <span class="hlt">pressures</span>. A sharp decrease in the Eu valence determined from the XAS was <span class="hlt">observed</span> at around 70 K in the temperature <span class="hlt">dependence</span> at P = 1.2-1.9 GPa. In the temperature <span class="hlt">dependence</span> of electrical resistivity and magnetic susceptibility, we <span class="hlt">observed</span> jumps associated with the temperature-induced valence transition under high <span class="hlt">pressures</span>. The magnetoresistance detected a field-induced valence transition. The results are discussed from the thermodynamic point of view.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16968995','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16968995"><span>The relationship between legal status, perceived <span class="hlt">pressure</span> and motivation in treatment for drug <span class="hlt">dependence</span>: results from a European study of Quasi-Compulsory Treatment.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Stevens, Alex; Berto, Daniele; Frick, Ulrich; Hunt, Neil; Kerschl, Viktoria; McSweeney, Tim; Oeuvray, Kerrie; Puppo, Irene; Santa Maria, Alberto; Schaaf, Susanne; Trinkl, Barbara; Uchtenhagen, Ambros; Werdenich, Wolfgang</p> <p>2006-01-01</p> <p>This paper reports on intake data from Quasi-Compulsory Treatment in Europe, a study of quasi-compulsory treatment (QCT) for drug <span class="hlt">dependent</span> offenders. It explores the link between formal legal coercion, perceived <span class="hlt">pressure</span> to be in treatment and motivation amongst a sample of 845 people who entered treatment for drug <span class="hlt">dependence</span> in five European countries, half of them in quasi-compulsory treatment and half 'voluntarily'. Using both quantitative and qualitative data, it suggests that those who enter treatment under QCT do perceive greater <span class="hlt">pressure</span> to be in treatment, but that this does not necessarily lead to higher or lower motivation than 'volunteers'. Many drug-<span class="hlt">dependent</span> offenders value QCT as an opportunity to get treatment. Motivation is mutable and can be developed or diminished by the quality of support and services offered to drug-<span class="hlt">dependent</span> offenders.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23061391','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23061391"><span>Impaired pulsation absorber mechanism in idiopathic normal <span class="hlt">pressure</span> hydrocephalus: laboratory investigation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Park, Eun-Hyoung; Eide, Per Kristian; Zurakowski, David; Madsen, Joseph R</p> <p>2012-12-01</p> <p>The pathophysiology of normal <span class="hlt">pressure</span> hydrocephalus (NPH), and the related problem of patient selection for treatment of this condition, have been of great interest since the description of this seemingly paradoxical condition nearly 50 years ago. Recently, Eide has reported that measurements of the amplitude of the intracranial <span class="hlt">pressure</span> (ICP) can both positively and negatively predict response to CSF shunting. Specifically, the fraction of time spent in a "high amplitude" (> 4 mm Hg) state predicted response to shunting, which may represent a marker for hydrocephalic pathophysiology. Increased ICP amplitude might suggest decreased brain compliance, meaning a static measure of a <span class="hlt">pressure</span>-volume ratio. Recent studies of canine data have shown that the brain compliance can be described as a frequency-<span class="hlt">dependent</span> function. The normal canine brain seems to show enhanced ability to absorb the pulsations around the heart rate, quantified as a cardiac pulsation absorbance (CPA), with properties like a notch filter in engineering. This frequency <span class="hlt">dependence</span> of the function is diminished with development of hydrocephalus in dogs. In this pilot study, the authors sought to determine whether frequency <span class="hlt">dependence</span> could be <span class="hlt">observed</span> in humans, and whether the frequency <span class="hlt">dependence</span> would be any different in epochs with high ICP amplitude compared with epochs of low ICP amplitude. Systems analysis was applied to arterial blood <span class="hlt">pressure</span> (ABP) and ICP waveforms recorded from 10 patients undergoing evaluations of idiopathic NPH to calculate a time-varying transfer function that reveals frequency <span class="hlt">dependence</span> and CPA, the measure of frequency-<span class="hlt">dependent</span> compliance previously used in animal experiments. The ICP amplitude was also calculated in the same samples, so that epochs with high (> 4 mm Hg) versus low (≤ 4 mm Hg) amplitude could be compared in CPA and transfer functions. Transfer function analysis for the more "normal" epochs with low amplitude exhibits a dip or notch in the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PhRvE..90d2725D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhRvE..90d2725D"><span>High-<span class="hlt">pressure</span> dynamics of hydrated protein in bioprotective trehalose environment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Diallo, S. O.; Zhang, Q.; O'Neill, H.; Mamontov, E.</p> <p>2014-10-01</p> <p>We present a <span class="hlt">pressure-dependence</span> study of the dynamics of lysozyme protein powder immersed in deuterated α ,α -trehalose environment via quasielastic neutron scattering (QENS). The goal is to assess the baroprotective benefits of trehalose on biomolecules by comparing the findings with those of a trehalose-free reference study. While the mean-square displacement of the trehalose-free protein (hydrated to dD2O≃ 40 w%) as a whole, is reduced by increasing <span class="hlt">pressure</span>, the actual <span class="hlt">observable</span> relaxation dynamics in the picoseconds to nanoseconds time range remains largely unaffected by pressure—up to the maximum investigated <span class="hlt">pressure</span> of 2.78(2) Kbar. Our <span class="hlt">observation</span> is independent of whether or not the protein is mixed with the deuterated sugar. This suggests that the hydrated protein's conformational states at atmospheric <span class="hlt">pressure</span> remain unaltered by hydrostatic <span class="hlt">pressures</span>, below 2.78 Kbar. We also found the QENS response to be totally recoverable after ambient <span class="hlt">pressure</span> conditions are restored. Small-angle neutron diffraction measurements confirm that the protein-protein correlation remains undisturbed. We <span class="hlt">observe</span>, however, a clear narrowing of the QENS response as the temperature is decreased from 290 to 230 K in both cases, which we parametrize using the Kohlrausch-Williams-Watts stretched exponential model. Only the fraction of protons that are immobile on the accessible time window of the instrument, referred to as the elastic incoherent structure factor, is <span class="hlt">observably</span> sensitive to <span class="hlt">pressure</span>, increasing only marginally but systematically with increasing <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28506960','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28506960"><span>Familial Analysis of Epistatic and Sex-<span class="hlt">Dependent</span> Association of Genes of the Renin-Angiotensin-Aldosterone System and Blood <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>Scurrah, Katrina J; Lamantia, Angela; Ellis, Justine A; Harrap, Stephen B</p> <p>2017-06-01</p> <p>Renin-angiotensin-aldosterone system genes have been inconsistently associated with blood <span class="hlt">pressure</span>, possibly because of unrecognized influences of sex-<span class="hlt">dependent</span> genetic effects or gene-gene interactions (epistasis). We tested association of systolic blood <span class="hlt">pressure</span> with single-nucleotide polymorphisms (SNPs) at renin ( REN ), angiotensinogen ( AGT ), angiotensin-converting enzyme ( ACE ), angiotensin II type 1 receptor ( AGTR1 ), and aldosterone synthase ( CYP11B2 ), including sex-SNP or SNP-SNP interactions. Eighty-eight tagSNPs were tested in 2872 white individuals in 809 pedigrees from the Victorian Family Heart Study using variance components models. Three SNPs (rs8075924 and rs4277404 at ACE and rs12721297 at AGTR1 ) were individually associated with lower systolic blood <span class="hlt">pressure</span> with significant ( P <0.00076) effect sizes ≈1.7 to 2.5 mm Hg. Sex-specific associations were seen for 3 SNPs in men (rs2468523 and rs2478544 at AGT and rs11658531 at ACE ) and 1 SNP in women (rs12451328 at ACE ). SNP-SNP interaction was suggested ( P <0.005) for 14 SNP pairs, none of which had shown individual association with systolic blood <span class="hlt">pressure</span>. Four SNP pairs were at the same gene (2 for REN , 1 for AGT , and 1 for AGTR1 ). The SNP rs3097 at CYP11B2 was represented in 5 separate pairs. SNPs at key renin-angiotensin-aldosterone system genes associate with systolic blood <span class="hlt">pressure</span> individually in both sexes, individually in one sex only and only when combined with another SNP. Analyses that incorporate sex-<span class="hlt">dependent</span> and epistatic effects could reconcile past inconsistencies and account for some of the missing heritability of blood <span class="hlt">pressure</span> and are generally relevant to SNP association studies for any phenotype. © 2017 American Heart Association, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..MAR.T1153Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..MAR.T1153Y"><span>High <span class="hlt">Pressure</span> Raman Spectroscopic Studies on CuInTe2 Quantum Dots</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yanxon, Howard; Kumar, Ravhi; HiPSEC-University of Nevada Las Vegas Team</p> <p></p> <p>High <span class="hlt">pressure</span> Raman spectroscopy studies were performed on CuInTe2 Quantum Dots (QD) up to 7.7 GPa. At ambient conditions, the Raman modes of the QD loaded into a high-<span class="hlt">pressure</span> diamond anvil cell (DAC) were <span class="hlt">observed</span> at 125.1 cm-1 (A1 mode) and 142.8 cm-1 (B2 or E mode). As the <span class="hlt">pressure</span> increases, the A1 mode starts to split above 2 GPa and shifts to the left as indication of a structural change. A <span class="hlt">pressure</span>-induced phase transition was <span class="hlt">observed</span> around 2.9 GPa due to the collapse of the modes with the appearance of a new Raman peaks. The phase transition <span class="hlt">observed</span> in our experiments compare well with the characteristics of bulk and larger nanoparticles. Further, it could be concluded that the phase transition <span class="hlt">pressure</span> <span class="hlt">observed</span> mainly <span class="hlt">depends</span> on the particle size. H.Y. thanks McNair foundation for fellowship award. He also acknowledges Melanie White, Jason Baker and Phuc Tran for help in the experiments. He thanks Michael Pravica for using the Raman facility.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28181445','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28181445"><span><span class="hlt">Pressure-Dependent</span> Detection of Carbon Monoxide Employing Wavelength Modulation Spectroscopy Using a Herriott-Type Cell.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Chuanliang; Wu, Yingfa; Qiu, Xuanbing; Wei, Jilin; Deng, Lunhua</p> <p>2017-05-01</p> <p>Wavelength modulation spectroscopy (WMS) combined with a multipass absorption cell has been used to measure a weak absorption line of carbon monoxide (CO) at 1.578 µm. A 0.95m Herriott-type cell provides an effective absorption path length of 55.1 m. The WMS signals from the first and second harmonic output of a lock-in amplifier (WMS-1 f and 2 f, respectively) agree with the Beer-Lambert law, especially at low concentrations. After boxcar averaging, the minimum detection limit achieved is 4.3 ppm for a measurement time of 0.125 s. The corresponding normalized detection limit is 84 ppm m Hz -1/2 . If the integrated time is increased to 88 s, the minimum detectable limit of CO can reach to 0.29 ppm based on an Allan variation analysis. The <span class="hlt">pressure-dependent</span> relationship is validated after accounting for the <span class="hlt">pressure</span> factor in data processing. Finally, a linear correlation between the WMS-2 f amplitudes and gas concentrations is obtained at concentration ratios less than 15.5%, and the accuracy is better than 92% at total <span class="hlt">pressure</span> less than 62.7 Torr.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150010972','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150010972"><span>Temperature and <span class="hlt">Pressure</span> <span class="hlt">Dependence</span> of Signal Amplitudes for Electrostriction Laser-Induced Thermal Acoustics</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Herring, Gregory C.</p> <p>2015-01-01</p> <p>The relative signal strength of electrostriction-only (no thermal grating) laser-induced thermal acoustics (LITA) in gas-phase air is reported as a function of temperature T and <span class="hlt">pressure</span> P. Measurements were made in the free stream of a variable Mach number supersonic wind tunnel, where T and P are varied simultaneously as Mach number is varied. Using optical heterodyning, the measured signal amplitude (related to the optical reflectivity of the acoustic grating) was averaged for each of 11 flow conditions and compared to the expected theoretical <span class="hlt">dependence</span> of a pure-electrostriction LITA process, where the signal is proportional to the square root of [P*P /( T*T*T)].</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27282319','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27282319"><span>The Chemical Shift Baseline for High-<span class="hlt">Pressure</span> NMR Spectra of Proteins.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Frach, Roland; Kibies, Patrick; Böttcher, Saraphina; Pongratz, Tim; Strohfeldt, Steven; Kurrmann, Simon; Koehler, Joerg; Hofmann, Martin; Kremer, Werner; Kalbitzer, Hans Robert; Reiser, Oliver; Horinek, Dominik; Kast, Stefan M</p> <p>2016-07-18</p> <p>High-<span class="hlt">pressure</span> (HP) NMR spectroscopy is an important method for detecting rare functional states of proteins by analyzing the <span class="hlt">pressure</span> response of chemical shifts. However, for the analysis of the shifts it is mandatory to understand the origin of the <span class="hlt">observed</span> <span class="hlt">pressure</span> <span class="hlt">dependence</span>. Here we present experimental HP NMR data on the (15) N-enriched peptide bond model, N-methylacetamide (NMA), in water, combined with quantum-chemical computations of the magnetic parameters using a <span class="hlt">pressure</span>-sensitive solvation model. Theoretical analysis of NMA and the experimentally used internal reference standard 4,4-dimethyl-4-silapentane-1-sulfonic (DSS) reveal that a substantial part of <span class="hlt">observed</span> shifts can be attributed to purely solvent-induced electronic polarization of the backbone. DSS is only marginally responsive to <span class="hlt">pressure</span> changes and is therefore a reliable sensor for variations in the local magnetic field caused by <span class="hlt">pressure</span>-induced changes of the magnetic susceptibility of the solvent. © 2016 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20120013537&hterms=High+Pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DHigh%2BPressure','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20120013537&hterms=High+Pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DHigh%2BPressure"><span>A Record-High Ocean Bottom <span class="hlt">Pressure</span> in the South Pacific <span class="hlt">Observed</span> by GRACE</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Boening, Carmen; Lee, Tong; Zlotnicki, Victor</p> <p>2011-01-01</p> <p>In late 2009 to early 2010, the Gravity Recovery and Climate Experiment (GRACE) satellite pair <span class="hlt">observed</span> a record increase in ocean bottom <span class="hlt">pressure</span> (OBP) over a large mid-latitude region of the South East Pacific. Its magnitude is substantially larger than other oceanic events in the Southern Hemisphere found in the entire GRACE data records (2003-2010) on multi-month time scales. The OBP data help to understand the nature of a similar signal in sea surface height (SSH) anomaly <span class="hlt">observed</span> by altimetry: the SSH increase is mainly due to mass convergence. Analysis of the barotropic vorticity equation using scatterometer data, atmospheric reanalysis product, and GRACE and altimeter an atmospheric reanalysis product <span class="hlt">observations</span> suggests that the <span class="hlt">observed</span> OBP/SSH signal was primarily caused by wind stress curl associated with a strong and persistent anticyclone in late 2009 in combination with effects of planetary vorticity gradient, bottom topography, and friction</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMMR33A2642N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMMR33A2642N"><span><span class="hlt">Dependencies</span> of pore <span class="hlt">pressure</span> on elastic wave velocities and Vp/Vs ratio for thermally cracked gabbro</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nishimura, K.; Uehara, S. I.; Mizoguchi, K.</p> <p>2015-12-01</p> <p>Marine seismic refraction have found that there are high Vp/Vs ratio regions in oceanic crusts at subducting oceanic plates (e.g, Cascadia subduction zone (2.0-2.8) (Audet et al., 2009)). Previous studies based on laboratory measurements indicated that Vp/Vs ratio is high when porosity and/or pore <span class="hlt">pressure</span> is high (Christensen, 1984; Peacock et al., 2011). Although several studies have investigated the relationships between fracture distributions and Vp, Vs (e.g., Wang et al., 2012; Blake et al., 2013), the relationships for rocks (e.g., gabbro and basalt) composing oceanic crust are still unclear. This study reports the results of laboratory measurements of Vp, Vs (transmission method) at controlled confining and pore <span class="hlt">pressure</span> and estimation of Vp/Vs ratio for thermally cracked gabbro which mimic highly fractured rocks in the high Vp/Vs ratio zone, in order to declare the <span class="hlt">dependence</span> of fracture distributions on Vp/Vs. For the measurements, we prepared three type specimens; a non-heated intact specimen, specimens heated up to 500 °C and 700 °C for 24 hours. Porosities of intact, 500 °C and 700 °C specimens measured under the atmospheric <span class="hlt">pressure</span> are 0.5, 3.4 and 3.5%, respectively. Measurements were conducted at a constant confining <span class="hlt">pressure</span> of 50 MPa, with decreasing pore <span class="hlt">pressure</span> from 49 to 0.1 MPa and then increasing to 49 MPa. While Vp/Vs for the intact specimen is almost constant at elevated pore <span class="hlt">pressure</span>, the Vp/Vs values for the thermally cracked ones were 2.0~2.2 when pore <span class="hlt">pressure</span> was larger than 30 MPa. In future, we will reveal the relationship between the measured elastic wave velocities and the characteristics of the microfracture distribution. This work was supported by JSPS Grant-in-Aid for Scientific Research (Grant Number 26400492).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4230124','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4230124"><span>CXCR6 deficiency attenuates <span class="hlt">pressure</span> overload-induced monocytes migration and cardiac fibrosis through downregulating TNF-α-<span class="hlt">dependent</span> MMP9 pathway</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Wang, Jia-Hong; Su, Feng; Wang, Shijun; Lu, Xian-Cheng; Zhang, Shao-Heng; Chen, De; Chen, Nan-Nan; Zhong, Jing-Quan</p> <p>2014-01-01</p> <p>An immerging role of TNF-α in collagen synthesis and cardiac fibrosis implies the significance of TNF-α production in the development of myocardial remodeling. Our previous study showed a reduction of TNF-α and attenuated cardiac remodeling in CXCR6 knockout (KO) mice after ischemia/reperfusion injury. However, the potential mechanism of TNF-α-mediated cardiac fibrosis with <span class="hlt">pressure</span> overload has not been well elucidated. In the present study, we aim to investigate the role of CXCR6 in TNF-α release and myocardial remodeling in response to <span class="hlt">pressure</span> overload. <span class="hlt">Pressure</span> overload was performed by constriction of transverse aorta (TAC) surgery on CXCR6 KO mice and C57 wild-type (WT) counterparts. At 6 weeks after TAC, cardiac remodeling was assessed by echocardiography, cardiac TNF-α release and its type I receptor (TNFRI), were detected by ELISA and western blot, collagen genes Col1a1 (type I) and Col3a1 (type III) were examined by real-time PCR. Compared with CXCR6 WT mice, CXCR6 KO mice exhibited less cardiac dysfunction, reduced expression of TNFRI, Col1a1 and Col3a. In vitro, we confirmed that CXCR6 deficiency led to reduced homing and infiltration of CD11b+ monocytes, which contributed to attenuated TNF-α release in myocardium. Furthermore, TNFRI antagonist pretreatment blocked AT1 receptor signaling and NOX4 expression, reduced collagen synthesis, and blunted the activity of MMP9 in CXCR6 WT mice after TAC, but these were not <span class="hlt">observed</span> in CXCR6 KO mice. In the present work, we propose a mechanism that CXCR6 is essential for <span class="hlt">pressure</span> overload-mediated myocardial recruitment of monocytes, which contributes to cardiac fibrosis through TNF-α-<span class="hlt">dependent</span> MMP9 activation and collagen synthesis. PMID:25400729</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25400729','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25400729"><span>CXCR6 deficiency attenuates <span class="hlt">pressure</span> overload-induced monocytes migration and cardiac fibrosis through downregulating TNF-α-<span class="hlt">dependent</span> MMP9 pathway.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Jia-Hong; Su, Feng; Wang, Shijun; Lu, Xian-Cheng; Zhang, Shao-Heng; Chen, De; Chen, Nan-Nan; Zhong, Jing-Quan</p> <p>2014-01-01</p> <p>An immerging role of TNF-α in collagen synthesis and cardiac fibrosis implies the significance of TNF-α production in the development of myocardial remodeling. Our previous study showed a reduction of TNF-α and attenuated cardiac remodeling in CXCR6 knockout (KO) mice after ischemia/reperfusion injury. However, the potential mechanism of TNF-α-mediated cardiac fibrosis with <span class="hlt">pressure</span> overload has not been well elucidated. In the present study, we aim to investigate the role of CXCR6 in TNF-α release and myocardial remodeling in response to <span class="hlt">pressure</span> overload. <span class="hlt">Pressure</span> overload was performed by constriction of transverse aorta (TAC) surgery on CXCR6 KO mice and C57 wild-type (WT) counterparts. At 6 weeks after TAC, cardiac remodeling was assessed by echocardiography, cardiac TNF-α release and its type I receptor (TNFRI), were detected by ELISA and western blot, collagen genes Col1a1 (type I) and Col3a1 (type III) were examined by real-time PCR. Compared with CXCR6 WT mice, CXCR6 KO mice exhibited less cardiac dysfunction, reduced expression of TNFRI, Col1a1 and Col3a. In vitro, we confirmed that CXCR6 deficiency led to reduced homing and infiltration of CD11b(+) monocytes, which contributed to attenuated TNF-α release in myocardium. Furthermore, TNFRI antagonist pretreatment blocked AT1 receptor signaling and NOX4 expression, reduced collagen synthesis, and blunted the activity of MMP9 in CXCR6 WT mice after TAC, but these were not <span class="hlt">observed</span> in CXCR6 KO mice. In the present work, we propose a mechanism that CXCR6 is essential for <span class="hlt">pressure</span> overload-mediated myocardial recruitment of monocytes, which contributes to cardiac fibrosis through TNF-α-<span class="hlt">dependent</span> MMP9 activation and collagen synthesis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70023277','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70023277"><span>Diamond-anvil cell <span class="hlt">observations</span> of a new methane hydrate phase in the 100-MPa <span class="hlt">pressure</span> range</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Chou, I.-Ming; Sharma, A.; Burruss, R.C.; Hemley, R.J.; Goncharov, A.F.; Stern, L.A.; Kirby, S.H.</p> <p>2001-01-01</p> <p>A new high-<span class="hlt">pressure</span> phase of methane hydrate has been identified based on its high optical relief, distinct <span class="hlt">pressure</span>-temperature phase relations, and Raman spectra. In-situ optical <span class="hlt">observations</span> were made in a hydrothermal diamond-anvil cell at temperatures between -40?? and 60 ??C and at <span class="hlt">pressures</span> up to 900 MPa. Two new invariant points were located at -8.7 ??C and 99 MPa for the assemblage consisting of the new phase, structure I methane hydrate, ice Ih, and water, and at 35.3 ??C and 137 MPa for the new phase-structure I methane hydrate-water-methane vapor. Existence of the new phase is critical for understanding the phase relations among the hydrates at low to moderate <span class="hlt">pressures</span>, and may also have important implications for understanding the hydrogen bonding in H2O and the behavior of water in the planetary bodies, such as Europa, of the outer solar system.</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('http://adsabs.harvard.edu/abs/2017AGUFMMR44A..06C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR44A..06C"><span>Breakdown <span class="hlt">pressures</span> and characteristic flaw sizes during fluid injection experiments in shale at elevated confining <span class="hlt">pressures</span>.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chandler, M.; Mecklenburgh, J.; Rutter, E. H.; Taylor, R.; Fauchille, A. L.; Ma, L.; Lee, P. D.</p> <p>2017-12-01</p> <p>Fracture propagation trajectories in gas-bearing shales <span class="hlt">depend</span> on the interaction between the anisotropic mechanical properties of the shale and the anisotropic in-situ stress field. However, there is a general paucity of available experimental data on their anisotropic mechanical, physical and fluid-flow properties, especially at elevated confining <span class="hlt">pressures</span>. A suite of mechanical, flow and elastic measurements have been made on two shale materials, the Whitby mudrock and the Mancos shale (an interbedded silt and mudstone), as well as Pennant sandstone, an isotropic baseline and tight-gas sandstone analogue. Mechanical characterization includes standard triaxial experiments, <span class="hlt">pressure-dependent</span> permeability, brazilian disk tensile strength, and fracture toughness determined using double-torsion experiments. Elastic characterisation was performed through ultrasonic velocities determined using a cross-correlation method. Additionally, we report the results of laboratory-scale fluid injection experiments for the same materials. Injection experiments involved the pressurisation of a blind-ending central hole in a dry cylindrical sample. Pressurisation is conducted under constant volume-rate control, using silicon oils of varying viscosities. Breakdown <span class="hlt">pressure</span> is not seen to exhibit a strong <span class="hlt">dependence</span> on rock type or orientation, and increases linearly with confining <span class="hlt">pressure</span>. In most experiments, a small drop in the injection <span class="hlt">pressure</span> record is <span class="hlt">observed</span> at what is taken to be fracture initiation, and in the Pennant sandstone this is accompanied by a small burst of acoustic energy. The shale materials were acoustically quiet. Breakdown is found to be rapid and uncontrollable after initiation if injection is continued. A simplified 2-dimensional model for explaining this is presented in terms of the stress intensities at the tip of a pressurised crack, and is used alongside the triaxial data to derive a characteristic flaw size from which the fractures have initiated</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4261180','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4261180"><span>Synthesis of Ordered Mesoporous Phenanthrenequinone-Carbon via π-π Interaction-<span class="hlt">Dependent</span> Vapor <span class="hlt">Pressure</span> for Rechargeable Batteries</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kwon, Mi-Sook; Choi, Aram; Park, Yuwon; Cheon, Jae Yeong; Kang, Hyojin; Jo, Yong Nam; Kim, Young-Jun; Hong, Sung You; Joo, Sang Hoon; Yang, Changduk; Lee, Kyu Tae</p> <p>2014-01-01</p> <p>The π-π interaction-<span class="hlt">dependent</span> vapour <span class="hlt">pressure</span> of phenanthrenequinone can be used to synthesize a phenanthrenequinone-confined ordered mesoporous carbon. Intimate contact between the insulating phenanthrenequinone and the conductive carbon framework improves the electrical conductivity. This enables a more complete redox reaction take place. The confinement of the phenanthrenequinone in the mesoporous carbon mitigates the diffusion of the dissolved phenanthrenequinone out of the mesoporous carbon, and improves cycling performance. PMID:25490893</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ITSP...64.1854H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ITSP...64.1854H"><span>A Coalitional Game for Distributed Inference in Sensor Networks With <span class="hlt">Dependent</span> <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>He, Hao; Varshney, Pramod K.</p> <p>2016-04-01</p> <p>We consider the problem of collaborative inference in a sensor network with heterogeneous and statistically <span class="hlt">dependent</span> sensor <span class="hlt">observations</span>. Each sensor aims to maximize its inference performance by forming a coalition with other sensors and sharing information within the coalition. It is proved that the inference performance is a nondecreasing function of the coalition size. However, in an energy constrained network, the energy consumption of inter-sensor communication also increases with increasing coalition size, which discourages the formation of the grand coalition (the set of all sensors). In this paper, the formation of non-overlapping coalitions with statistically <span class="hlt">dependent</span> sensors is investigated under a specific communication constraint. We apply a game theoretical approach to fully explore and utilize the information contained in the spatial <span class="hlt">dependence</span> among sensors to maximize individual sensor performance. Before formulating the distributed inference problem as a coalition formation game, we first quantify the gain and loss in forming a coalition by introducing the concepts of diversity gain and redundancy loss for both estimation and detection problems. These definitions, enabled by the statistical theory of copulas, allow us to characterize the influence of statistical <span class="hlt">dependence</span> among sensor <span class="hlt">observations</span> on inference performance. An iterative algorithm based on merge-and-split operations is proposed for the solution and the stability of the proposed algorithm is analyzed. Numerical results are provided to demonstrate the superiority of our proposed game theoretical approach.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28828436','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28828436"><span>Analyzing the <span class="hlt">dependence</span> of oxygen incorporation current density on overpotential and oxygen partial <span class="hlt">pressure</span> in mixed conducting oxide electrodes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Guan, Zixuan; Chen, Di; Chueh, William C</p> <p>2017-08-30</p> <p>The oxygen incorporation reaction, which involves the transformation of an oxygen gas molecule to two lattice oxygen ions in a mixed ionic and electronic conducting solid, is a ubiquitous and fundamental reaction in solid-state electrochemistry. To understand the reaction pathway and to identify the rate-determining step, near-equilibrium measurements have been employed to quantify the exchange coefficients as a function of oxygen partial <span class="hlt">pressure</span> and temperature. However, because the exchange coefficient contains contributions from both forward and reverse reaction rate constants and <span class="hlt">depends</span> on both oxygen partial <span class="hlt">pressure</span> and oxygen fugacity in the solid, unique and definitive mechanistic assessment has been challenging. In this work, we derive a current density equation as a function of both oxygen partial <span class="hlt">pressure</span> and overpotential, and consider both near and far from equilibrium limits. Rather than considering specific reaction pathways, we generalize the multi-step oxygen incorporation reaction into the rate-determining step, preceding and following quasi-equilibrium steps, and consider the number of oxygen ions and electrons involved in each. By evaluating the <span class="hlt">dependence</span> of current density on oxygen partial <span class="hlt">pressure</span> and overpotential separately, one obtains the reaction orders for oxygen gas molecules and for solid-state species in the electrode. We simulated the oxygen incorporation current density-overpotential curves for praseodymium-doped ceria for various candidate rate-determining steps. This work highlights a promising method for studying the exchange kinetics far away from equilibrium.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.T43D2684N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.T43D2684N"><span>Strengthening of synthetic quartz-rich sediments during time-<span class="hlt">dependent</span> compaction due to <span class="hlt">pressure</span> solution-precipitation compaction creep</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Noda, H.; Okazaki, K.; Katayama, I.</p> <p>2013-12-01</p> <p>During diagenesis, incohesive sediments are compacted and gain strength against shear deformation for a geologically long time scale. The evolution of shear strength as well as the change in the mechanical and hydraulic characteristics under shear deformation is of significant importance in considering deformation at shallow part of the subduction zones and in accretionary prisms. Sediments after induration due to time-<span class="hlt">dependent</span> diagenesis process probably deform with increases in porosity and permeability much more significantly than normally compacted incohesive sediments. An active fault in a shallow incohesive medium may favor thermal <span class="hlt">pressurization</span> of pore fluid when slid rapidly, while the lack of time-<span class="hlt">dependent</span> healing effect may cause stable (e.g., rate-strengthening) frictional property there. On the other hand, indurated sediments may deform with significant post-failure weakening, and thus exhibit localization of deformation or unstable behavior. In order to investigate how the time-<span class="hlt">dependent</span> compaction and induration affect the mechanical and hydraulic characteristics of sediments under deformation, we have conducted a series of compaction experiments under hydrothermal conditions (at temperatures from R.T. to 500 °C, 200 MPa confining <span class="hlt">pressure</span>, 100 MPa pore water <span class="hlt">pressure</span>, and for various time), and following triaxial deformation experiments for the compacted samples, with monitoring permeability and storage capacity with pore <span class="hlt">pressure</span> oscillation method [Fischer and Paterson, 1992]. Previous work [e.g., Niemeijer et at., 2003] reported that under the adopted conditions, quartz aggregate deforms by <span class="hlt">pressure</span> solution-precipitation creep. The initial synthetic sediments have been prepared by depositing commercially available crushed quartzite the grain size of which is about 6 μm on average. 4 cm long samples have been extracted from the middle of 10 cm long deposited columns. The experiments have been performed with a gas-medium apparatus in Hiroshima</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=rate+AND+reaction+AND+decomposition&id=EJ717074','ERIC'); return false;" href="https://eric.ed.gov/?q=rate+AND+reaction+AND+decomposition&id=EJ717074"><span><span class="hlt">Pressure</span> <span class="hlt">Dependence</span> of Gas-Phase Reaction Rates</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 Persis, Stephanie; Dollet, Alain; Teyssandier, Francis</p> <p>2004-01-01</p> <p>It is presented that only simple concepts, mainly taken from activated-complex or transition-state theory, are required to explain and analytically describe the influence of <span class="hlt">pressure</span> on gas-phase reaction kinetics. The simplest kind of elementary gas-phase reaction is a unimolecular decomposition reaction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ApPhL.109q1903R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ApPhL.109q1903R"><span><span class="hlt">Pressure</span> induced structural, electronic topological, and semiconductor to metal transition in AgBiSe2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rajaji, V.; Malavi, Pallavi S.; Yamijala, Sharma S. R. K. C.; Sorb, Y. A.; Dutta, Utpal; Guin, Satya N.; Joseph, B.; Pati, Swapan K.; Karmakar, S.; Biswas, Kanishka; Narayana, Chandrabhas</p> <p>2016-10-01</p> <p>We report the effect of strong spin orbit coupling inducing electronic topological and semiconductor to metal transitions on the thermoelectric material AgBiSe2 at high <span class="hlt">pressures</span>. The synchrotron X-ray diffraction and the Raman scattering measurement provide evidence for a <span class="hlt">pressure</span> induced structural transition from hexagonal (α-AgBiSe2) to rhombohedral (β-AgBiSe2) at a relatively very low <span class="hlt">pressure</span> of around 0.7 GPa. The sudden drop in the electrical resistivity and clear anomalous changes in the Raman line width of the A1g and Eg(1) modes around 2.8 GPa was <span class="hlt">observed</span> suggesting a <span class="hlt">pressure</span> induced electronic topological transition. On further increasing the <span class="hlt">pressure</span>, anomalous <span class="hlt">pressure</span> <span class="hlt">dependence</span> of phonon (A1g and Eg(1)) frequencies and line widths along with the <span class="hlt">observed</span> temperature <span class="hlt">dependent</span> electrical resistivity show a <span class="hlt">pressure</span> induced semiconductor to metal transition above 7.0 GPa in β-AgBiSe2. First principles theoretical calculations reveal that the metallic character of β-AgBiSe2 is induced mainly due to redistributions of the density of states (p orbitals of Bi and Se) near to the Fermi level. Based on its <span class="hlt">pressure</span> induced multiple electronic transitions, we propose that AgBiSe2 is a potential candidate for the good thermoelectric performance and <span class="hlt">pressure</span> switches at high <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhSS...60..769P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhSS...60..769P"><span><span class="hlt">Pressure</span> <span class="hlt">Dependences</span> of Elastic Constants of AMg6 Aluminum-Magnesium Alloy and n-AMg6/C60 Nanocomposite Alloy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Prokhorov, V. M.; Gromnitskaya, E. L.</p> <p>2018-04-01</p> <p>The ultrasonic study results for <span class="hlt">dependence</span> of the elastic wave velocities and second-order elasticity coefficients of the polycrystalline aluminum alloy AMg6 and its nanocomposite n-AMg6/C60 on hydrostatic <span class="hlt">pressure</span> up to 1.6 GPa have been described. The ultrasonic research has been carried out using a highpressure ultrasonic piezometer based on the piston-cylinder device. The <span class="hlt">pressure</span> derivatives of the secondorder elastic constants of these materials established in the present study have been compared with the results of the third-order elastic constants measurements of the test alloys using the Thurston-Brugger method. Involving available literature data, we determined the relationships between the <span class="hlt">pressure</span> derivatives of the second-order elastic constants of the AMg6 alloy and the Mg-content and nanostructuring.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19770023513','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19770023513"><span>Temperature and <span class="hlt">pressure</span> <span class="hlt">dependence</span> of dichloro-difluoromethane (CF2C12) absorption coefficients for CO2 waveguide laser radiation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Harward, C. N.</p> <p>1977-01-01</p> <p>Measurements were performed to determine the <span class="hlt">pressure</span> and temperature <span class="hlt">dependence</span> of CFM-12 absorption coefficients for CO2 waveguide laser radiation. The absorption coefficients of CFM-12 for CO2 waveguide laser radiation were found to have no spectral structure within small spectral bandwidths around the CO2 waveguide laser lines in the CO2 spectral band for <span class="hlt">pressures</span> above 20 torr. All of the absorption coefficients for the CO2 laser lines studied are independent of <span class="hlt">pressure</span> above 100 torr, except for the P(36) laser CO2 spectral band. The absorption coefficients associated with the P(42) line in the same band showed the greatest change with temperature, and it also has the largest value of all the lines studied.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/ED175929.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/ED175929.pdf"><span>The <span class="hlt">Dependability</span> of Classroom <span class="hlt">Observations</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>Hiatt, Diana Buell; Keesling, J. Ward</p> <p></p> <p>A generalizability study of timed <span class="hlt">observations</span> was conducted in 25 primary grade classes to <span class="hlt">observe</span> teachers' use of time--for instruction, evaluation of instruction, and classroom management--according to the hour and day <span class="hlt">observed</span>. <span class="hlt">Observational</span> methods used by on-site researchers included videotape, checklists, running documentaries, frequency…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvM...1d3605P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvM...1d3605P"><span>High-<span class="hlt">pressure</span> behavior of CaMo O4</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Panchal, V.; Garg, N.; Poswal, H. K.; Errandonea, D.; Rodríguez-Hernández, P.; Muñoz, A.; Cavalli, E.</p> <p>2017-09-01</p> <p>We report a high-<span class="hlt">pressure</span> study of tetragonal scheelite-type CaMo O4 up to 29 GPa. In order to characterize its high-<span class="hlt">pressure</span> behavior, we have combined Raman and optical-absorption measurements with density functional theory calculations. We have found evidence of a <span class="hlt">pressure</span>-induced phase transition near 15 GPa. Experiments and calculations agree in assigning the high-<span class="hlt">pressure</span> phase to a monoclinic fergusonite-type structure. The reported results are consistent with previous powder x-ray-diffraction experiments, but are in contradiction with the conclusions obtained from earlier Raman measurements, which support the existence of more than one phase transition in the <span class="hlt">pressure</span> range covered by our studies. The <span class="hlt">observed</span> scheelite-fergusonite transition induces significant changes in the electronic band gap and phonon spectrum of CaMo O4 . We have determined the <span class="hlt">pressure</span> evolution of the band gap for the low- and high-<span class="hlt">pressure</span> phases as well as the frequencies and <span class="hlt">pressure</span> <span class="hlt">dependencies</span> of the Raman-active and infrared-active modes. In addition, based on calculations of the phonon dispersion of the scheelite phase, carried out at a <span class="hlt">pressure</span> higher than the transition <span class="hlt">pressure</span>, we propose a possible mechanism for the reported phase transition. Furthermore, from the calculations we determined the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the unit-cell parameters and atomic positions of the different phases and their room-temperature equations of state. These results are compared with previous experiments showing a very good agreement. Finally, information on bond compressibility is reported and correlated with the macroscopic compressibility of CaMo O4 . The reported results are of interest for the many technological applications of this oxide.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15529759','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15529759"><span><span class="hlt">Pressure</span> and temperature interactions on cellular respiration: a review.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sebert, P; Theron, M; Vettier, A</p> <p>2004-06-01</p> <p>Thermodynamic equations show that <span class="hlt">pressure</span> and temperature can, theoretically, act in synergy or in opposite directions <span class="hlt">depending</span> on their respective variations. Hence, they interact to establish rates of biological processes (<span class="hlt">pressure</span>/temperature interactions, PTI). For such studies, it is interesting to use aquatic ectotherms, in particular fish, because it is easy to submit them to temperature and/or <span class="hlt">pressure</span> changes. This review focuses on the effects of temperature and <span class="hlt">pressure</span> changes on the energy metabolism of fish, mitochondrial oxygen consumption and functioning, showing that the <span class="hlt">observed</span> effects do not always match the predictions made by equations or models. Unpublished results concerning the mitochondrial function of eels acclimatised at two temperatures and two <span class="hlt">pressures</span> show that the mitochondrial targets of <span class="hlt">pressure</span> and temperature are probably not the same. The possible mechanisms and consequences of PTI are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120003167','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120003167"><span><span class="hlt">Pressure</span> <span class="hlt">Dependence</span> of Insulator-Insulator Contact Charging</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hogue, Michael D.</p> <p>2005-01-01</p> <p>The mechanism of insulator-insulator triboelectric (contact) charging is being studied by the Electrostatics and Surface Physics Laboratory at KSC. The hypothesis that surface ion exchange is the primary mechanism is being tested experimentally. A two-phase model based on a small partial <span class="hlt">pressure</span> of singly charged ions in an ambient ideal gas in equilibrium with a submonolayer adsorbed film will provide predictions about charging as a function Of ion mass, <span class="hlt">pressure</span>, temperature, and surface adsorption energy. Interactions between ions will be considered in terms of coulombic and screened potential energies. This work is yielding better understanding of the triboelectrification of insulators, which is an important problem in. space exploration technology. The work is also relevant to important industrial processes such as xerography and the application of paints and coatings. Determining a better understanding of the fundamental mechanism of insulator-insulator triboelectrification will hopefully lead to better means of eliminating or at least mitigating its hazards and enhancing its useful applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27284648','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27284648"><span><span class="hlt">Observation</span> of Energy and Baseline <span class="hlt">Dependent</span> Reactor Antineutrino Disappearance in the RENO Experiment.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Choi, J H; Choi, W Q; Choi, Y; Jang, H I; Jang, J S; Jeon, E J; Joo, K K; Kim, B R; Kim, H S; Kim, J Y; Kim, S B; Kim, S Y; Kim, W; Kim, Y D; Ko, Y; Lee, D H; Lim, I T; Pac, M Y; Park, I G; Park, J S; Park, R G; Seo, H; Seo, S H; Seon, Y G; Shin, C D; Siyeon, K; Yang, J H; Yeo, I S; Yu, I</p> <p>2016-05-27</p> <p>The RENO experiment has analyzed about 500 live days of data to <span class="hlt">observe</span> an energy <span class="hlt">dependent</span> disappearance of reactor ν[over ¯]_{e} by comparing their prompt signal spectra measured in two identical near and far detectors. In the period between August of 2011 and January of 2013, the far (near) detector <span class="hlt">observed</span> 31 541 (290 775) electron antineutrino candidate events with a background fraction of 4.9% (2.8%). The measured prompt spectra show an excess of reactor ν[over ¯]_{e} around 5 MeV relative to the prediction from a most commonly used model. A clear energy and baseline <span class="hlt">dependent</span> disappearance of reactor ν[over ¯]_{e} is <span class="hlt">observed</span> in the deficit of the <span class="hlt">observed</span> number of ν[over ¯]_{e}. Based on the measured far-to-near ratio of prompt spectra, we obtain sin^{2}2θ_{13}=0.082±0.009(stat)±0.006(syst) and |Δm_{ee}^{2}|=[2.62_{-0.23}^{+0.21}(stat)_{-0.13}^{+0.12}(syst)]×10^{-3}  eV^{2}.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2576329','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2576329"><span>Aerophagia and Gastroesophageal Reflux Disease in Patients using Continuous Positive Airway <span class="hlt">Pressure</span>: A Preliminary <span class="hlt">Observation</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>Watson, Nathaniel F.; Mystkowski, Sue K.</p> <p>2008-01-01</p> <p>Study Objectives: Aerophagia is a complication of continuous positive airway <span class="hlt">pressure</span> (CPAP) therapy for sleep disordered breathing (SDB), whereupon air is forced into the stomach and bowel. Associated discomfort can result in CPAP discontinuation. We hypothesize that aerophagia is associated with gastroesophageal reflux disease (GERD) via mechanisms involving GERD related lower esophageal sphincter (LES) compromise. Methods: Twenty-two subjects with aerophagia and 22 controls, matched for age, gender, and body mass index, who were being treated with CPAP for SDB were compared in regard to clinical aspects of GERD, GERD associated habits, SDB severity as measured by polysomnography, and mean CPAP <span class="hlt">pressure</span>. Results: More subjects with aerophagia had symptoms of GERD (77.3% vs. 36.4%; p < 0.01) and were on GERD related medications (45.5% vs. 18.2%, p < 0.05) than controls. Regarding polysomnography, mean oxygen saturation percentages were lower in the aerophagia group than controls (95.0% vs. 96.5%, p < 0.05). No other differences were <span class="hlt">observed</span>, including mean CPAP <span class="hlt">pressures</span>. No one in the aerophagia group (vs. 27.3% of the control group) was a current tobacco user (p < 0.01). There was no difference in caffeine or alcohol use between the 2 groups. Conclusions: These results imply aerophagia is associated with GERD symptoms and GERD related medication use. This finding suggests a relationship between GERD related LES pathophysiology and the development of aerophagia in patients with SDB treated with CPAP. Citation: Watson NF; Mystkowski SK. Aerophagia and gastroesophageal reflux disease in patients using continuous positive airway <span class="hlt">pressure</span>: a preliminary <span class="hlt">observation</span>. J Clin Sleep Med 2008;4(5):434–438. PMID:18853700</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.V32A..05M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.V32A..05M"><span>Transmission of magmatic <span class="hlt">pressure</span> changes at Kilauea volcano</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Montagna, C. P.; Gonnermann, H. M.</p> <p>2012-12-01</p> <p>Volcanic eruptions are often accompanied by spatiotemporal migration of ground deformation, a consequence of <span class="hlt">pressure</span> changes within magma reservoirs and pathways. We have modeled the propagation of such <span class="hlt">pressure</span> variations, caused by eruptive magma withdrawal during the early eruptive episodes of the ongoing Pu`u `O`o-Kupaianaha eruption of Kilauea volcano. Tilt measurements show that the onset of eruptive episodes at Pu`u `O`o was typically accompanied by abrupt deflation and followed by a sudden onset of gradual re-inflation, once the eruptive episode ended. Tilt of Kilauea's summit underwent similar patterns of deflation and inflation, albeit with a time delay of several hours during most episodes. The <span class="hlt">observed</span> delay times can be reproduced by a numerical model of <span class="hlt">pressure</span> variations within an elastic-walled dike that connects Kilauea's summit to its east rift zone. As <span class="hlt">pressure</span> changes travel through the dike, the interplay between elastic response of the dike wall and viscous resistance of the fluid determines the delay time. An example of the ability of the model to reproduce <span class="hlt">observed</span> tilt data is presented in Figure 1, which shows measured tilt at Pu`u `O`o during episode 18, together with measured and modeled tilt at Kilauea's summit. Magma withdrawal beneath Pu`u `O`o causes a decrease in <span class="hlt">pressure</span> and deflation. This <span class="hlt">pressure</span> change is estimated from <span class="hlt">observed</span> ground deformation, and it constitutes the time-<span class="hlt">dependent</span> model boundary condition at Pu`u `O`o, which propagates to Kilauea's summit. The resultant increase in magma flux causes deflation of Kilauea's Halema`uma`u magma reservoir and the change and time delay of tilt are reproduced by the model. The time delay <span class="hlt">depends</span> on elasticity of the wall rock, dike dimensions, magma viscosity, as well as magnitude and duration of the <span class="hlt">pressure</span> variations themselves. In addition, these parameters also affect the attenuation of the amplitude of the <span class="hlt">pressure</span> variation, as it travels between Puu Oo and summit</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4217124','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4217124"><span>Imaging Intratumoral Convection: <span class="hlt">Pressure</span> <span class="hlt">Dependent</span> Enhancement in Chemotherapeutic Delivery to Solid Tumors</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Gade, Terence P.F.; Buchanan, Ian M.; Motley, Matthew W.; Mazaheri, Yousef; Spees, William M.; Koutcher, Jason A.</p> <p>2014-01-01</p> <p>Purpose Low molecular weight (LMW) chemotherapeutics are believed to reach tumors through diffusion across capillary beds as well as membrane transporters. Unexpectedly, the delivery of these agents appears to be augmented by reductions in tumor interstitial fluid <span class="hlt">pressure</span> (TIFP), an effect typically associated with high molecular weight molecules which reach tumors principally through convection. We investigated the hypothesis that improved intratumoral convection can alter tumor metabolism and enhance the delivery of a LMW chemotherapeutic agent to solid tumors. Experimental Design For this purpose we applied 31P/19F MR spectroscopy and spectroscopic imaging to examine the influence of type I collagenase on tumor bioenergetics and the delivery of 5-fluorouracil (5FU) to HT29 human colorectal tumors grown subcutaneously in mice. Results Collagenase effected a 34% reduction in TIFP with an attendant disintegration of intratumoral collagen. Neither mice administered collagenase nor controls receiving PBS demonstrated changes in 31PMRS-measured tumor bioenergetics; however, a time-<span class="hlt">dependent</span> increase in the content of extracellular inorganic phosphate (Pie) was <span class="hlt">observed</span> in tumors of collagenase-treated animals. 31PMRSI demonstrated that this increase underscored a more homogeneous distribution of Pie in tumors of experimental mice. 19FMRS showed that these changes were associated with a 50% increase in 5FU uptake in tumors of experimental versus control animals; however, this increase resulted in an increase in 5FU catabolites rather than fluoronucleotide intermediates that are required for subsequent cytotoxicity. Conclusions These data indicate that the modulation of convective flow within tumors can improve the delivery of (LMW) chemotherapeutics and demonstrate the potential role for non-invasive imaging of this process in vivo. PMID:19118052</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhRvL.109u7402Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhRvL.109u7402Y"><span>Inelastic Light Scattering Measurements of a <span class="hlt">Pressure</span>-Induced Quantum Liquid in KCuF3</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yuan, S.; Kim, M.; Seeley, J. T.; Lee, J. C. T.; Lal, S.; Abbamonte, P.; Cooper, S. L.</p> <p>2012-11-01</p> <p><span class="hlt">Pressure-dependent</span>, low-temperature inelastic light (Raman) scattering measurements of KCuF3 show that applied <span class="hlt">pressure</span> above P*˜7kbar suppresses a previously <span class="hlt">observed</span> structural phase transition temperature to zero temperature in KCuF3, resulting in the development of a fluctuational (quasielastic) response near T˜0K. This <span class="hlt">pressure</span>-induced fluctuational response—which we associate with slow fluctuations of the CuF6 octahedral orientation—is temperature independent and exhibits a characteristic fluctuation rate that is much larger than the temperature, consistent with quantum fluctuations of the CuF6 octahedra. A model of pseudospin-phonon coupling provides a qualitative description of both the temperature- and <span class="hlt">pressure-dependent</span> evolution of the Raman spectra of KCuF3.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17046147','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17046147"><span>pH <span class="hlt">dependence</span> of the dissociation of multimeric hemoglobin probed by high hydrostatic <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>Bispo, Jose A C; Santos, Jose L R; Landini, Gustavo F; Goncalves, Juliana M; Bonafe, Carlos F S</p> <p>2007-02-01</p> <p>We investigated the thermodynamic features of the classic alkaline dissociation of multimeric hemoglobin (3.1 MDa) from Glossoscolex paulistus (Annelidea) using high hydrostatic <span class="hlt">pressure</span>. Light scattering measurements up to microscopic thermodynamic equilibrium indicated a high pH <span class="hlt">dependency</span> of dissociation and association. Electron microscopy and gel filtration corroborated these findings. The volume change of dissociation decreased in absolute values from -48.0 mL/mol of subunit at pH 6.0 to -19.2 mL/mol at pH 9.0, suggesting a lack of protein interactions under alkaline conditions. Concomitantly, an increase in pH reduced the Gibbs free energy of dissociation from 37.7 to 27.5 kJ/mol of subunit. The stoichiometry of proton release calculated from the <span class="hlt">pressure</span>-induced dissociation curves was +0.602 mol of H(+)/mol of subunit. These results provide a direct quantification of proton participation in stabilizing the aggregated state of the hemoglobin, and contribute to our understanding of protein-protein interactions and of the surrounding conditions that modulate the process of aggregation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22086257-spatially-dependent-heating-ionization-icme-observed-both-ace-ulysses','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22086257-spatially-dependent-heating-ionization-icme-observed-both-ace-ulysses"><span>SPATIALLY <span class="hlt">DEPENDENT</span> HEATING AND IONIZATION IN AN ICME <span class="hlt">OBSERVED</span> BY BOTH ACE AND ULYSSES</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>Lepri, Susan T.; Laming, J. Martin; Rakowski, Cara E.</p> <p>2012-12-01</p> <p>The 2005 January 21 interplanetary coronal mass ejection (ICME) <span class="hlt">observed</span> by multiple spacecraft at L1 was also <span class="hlt">observed</span> from January 21-February 4 at Ulysses (5.3 AU). Previous studies of this ICME have found evidence suggesting that the flanks of a magnetic cloud like structure associated with this ICME were <span class="hlt">observed</span> at L1 while a more central cut through the associated magnetic cloud was <span class="hlt">observed</span> at Ulysses. This event allows us to study spatial variation across the ICME and relate it to the eruption at the Sun. In order to examine the spatial <span class="hlt">dependence</span> of the heating in this ICME, wemore » present an analysis and comparison of the heavy ion composition <span class="hlt">observed</span> during the passage of the ICME at L1 and at Ulysses. Using SWICS, we compare the heavy ion composition across the two different <span class="hlt">observation</span> cuts through the ICME and compare it with predictions for heating during the eruption based on models of the time-<span class="hlt">dependent</span> ionization balance throughout the event.« less</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('http://adsabs.harvard.edu/abs/2018PhRvM...2d0401N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvM...2d0401N"><span>In situ ESEM imaging of the vapor-<span class="hlt">pressure-dependent</span> sublimation-induced morphology of ice</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nair, Malavika; Husmann, Anke; Cameron, Ruth E.; Best, Serena M.</p> <p>2018-04-01</p> <p>Sublimation is a fundamental phase transition that has a profound impact on both natural phenomena and advanced manufacturing technologies. Although great strides have been made in the study of ice growth from melt and vapor, little consideration has been given to the effect of sublimation on the morphological features that develop in the ice microstructure. In this experimental study, we demonstrate the effect of vapor <span class="hlt">pressure</span> on the mesoscopic faceting <span class="hlt">observed</span> and show that a vapor-<span class="hlt">pressure</span>-specific wavelength characterizes the periodic features that arise during sublimation. The ability to control the length scale of these features not only provides us with new insights into the mesoscopic roughness of ice crystals, but also presents the potential to exploit this effect in a plethora of applications from comet dating to ice-templated tissue engineering scaffolds.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3345817','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3345817"><span><span class="hlt">Observing</span> and Studying Extreme Low <span class="hlt">Pressure</span> Events with Altimetry</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Carrère, Loren; Mertz, Françoise; Dorandeu, Joel; Quilfen, Yves; Patoux, Jerome</p> <p>2009-01-01</p> <p>The ability of altimetry to detect extreme low <span class="hlt">pressure</span> events and the relationship between sea level <span class="hlt">pressure</span> and sea level anomalies during extra-tropical depressions have been investigated. Specific altimeter treatments have been developed for tropical cyclones and applied to obtain a relevant along-track sea surface height (SSH) signal: the case of tropical cyclone Isabel is presented here. The S- and C-band measurements are used because they are less impacted by rain than the Ku-band, and new sea state bias (SSB) and wet troposphere corrections are proposed. More accurate strong altimeter wind speeds are computed thanks to the Young algorithm. Ocean signals not related to atmospheric <span class="hlt">pressure</span> can be removed with accuracy, even within a Near Real Time context, by removing the maps of sea level anomaly (SLA) provided by SSALTO/Duacs. In the case of Extra-Tropical Depressions, the classical altimeter processing can be used. Ocean signal not related to atmospheric <span class="hlt">pressure</span> is along-track filtered. The sea level <span class="hlt">pressure</span> (SLP)-SLA relationship is investigated for the North Atlantic, North Pacific and Indian oceans; three regression models are proposed allowing restoring an altimeter SLP with a mean error of 5 hPa if compared to ECMWF or buoys SLP. The analysis of barotropic simulation outputs points out the regional variability of the SLP/Model Sea Level relationship and the wind effects. PMID:22573955</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22306310-pressure-induced-amorphization-la-sub-tao-sub','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22306310-pressure-induced-amorphization-la-sub-tao-sub"><span><span class="hlt">Pressure</span>-induced amorphization of La{sub 1/3}TaO{sub 3}</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>Noked, O., E-mail: noked@bgu.ac.il; Physics Department, Ben-Gurion University, Beer Sheva 84105; Melchior, A.</p> <p>2013-06-15</p> <p>La{sub 1/3}TaO{sub 3}, an A-site cation deficient perovskite, has been studied under <span class="hlt">pressure</span> by synchrotron X-ray powder diffraction and Raman spectroscopy. It undergoes irreversible <span class="hlt">pressure</span> induced amorphization at P=18.5 GPa. An almost linear unit cell volume decrease vs. <span class="hlt">pressure</span> is <span class="hlt">observed</span> from ambient <span class="hlt">pressure</span> up to the phase transition. The Raman spectroscopy also shows amorphization at the same <span class="hlt">pressure</span>, with positive shifts of all modes as a function of <span class="hlt">pressure</span>. The <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the E{sub g} and A{sub 1g} Raman modes arising from the octahedral oxygen network is discussed. - Graphical abstract: La{sub 1/3}Tao{sub 3} exhibits linear pressure–volume relationmore » until irreversible <span class="hlt">pressure</span> induced amorphization at 18.5 Gpa. - Highlights: • La{sub 1/3}TaO{sub 3} has been studied under <span class="hlt">pressure</span> by synchrotron XRD and Raman spectroscopy. • La{sub 1/3}TaO{sub 3} undergoes irreversible <span class="hlt">pressure</span> induced amorphization around 18.5 GPa. • The transition is manifested in both XRD and Raman measurements. • A linear P–V relation is <span class="hlt">observed</span> from ambient <span class="hlt">pressure</span> up to the phase transition.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080012610','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080012610"><span>Oxidation of C/SiC Composites at Reduced Oxygen Partial <span class="hlt">Pressures</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Opila, E. J.; Serra, J. L.</p> <p>2007-01-01</p> <p>T-300 carbon fibers and T-300 carbon fiber reinforced silicon carbide composites (C/SiC) were oxidized in flowing reduced oxygen partial <span class="hlt">pressure</span> environments at a total <span class="hlt">pressure</span> of one atmosphere (0.5 atm O2, 0.05 atm O2 and 0.005 atm O2, balance argon). Experiments were conducted at four temperatures (816deg, 1149deg, 1343deg, and 1538 C). The oxidation kinetics were monitored using thermogravimetric analysis. T-300 fibers were oxidized to completion for times between 0.6 and 90 h. Results indicated that fiber oxidation kinetics were gas phase diffusion controlled. Oxidation rates had an oxygen partial <span class="hlt">pressure</span> <span class="hlt">dependence</span> with a power law exponent close to one. In addition, oxidation rates were only weakly <span class="hlt">dependent</span> on temperature. The C/SiC coupon oxidation kinetics showed some variability, attributed to differences in the number and width of cracks in the SiC seal coat. In general, weight losses were <span class="hlt">observed</span> indicating oxidation of the carbon fibers dominated the oxidation behavior. Low temperatures and high oxygen <span class="hlt">pressures</span> resulted in the most rapid consumption of the carbon fibers. At higher temperatures, the lower oxidation rates were primarily attributed to crack closure due to SiC thermal expansion, rather than oxidation of SiC since these reduced rates were <span class="hlt">observed</span> even at the lowest oxygen partial <span class="hlt">pressures</span> where SiC oxidation is minimal.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4272451','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4272451"><span>Evidence of a Structural Defect in Ice VII and the Side Chain <span class="hlt">Dependent</span> Response of Small Model Peptides to Increased <span class="hlt">Pressure</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>Scott, J. Nathan; Vanderkooi, Jane M.</p> <p>2014-01-01</p> <p>The effect of high <span class="hlt">pressure</span> on the OH stretch of dilute HOD in D2O was examined using high <span class="hlt">pressure</span> FTIR. It was found that at <span class="hlt">pressures</span> directly above the ice VI to ice VII transition, ice VII displays a splitting in the OH absorption indicative of differing hydrogen bonding environments. This result is contrary to published structures of ice VII in which each OH oscillator should experience an identical electronic environment. The anomalous band was found to decrease in absorbance and finally disappear at ~43.0 kbar. In addition, the <span class="hlt">pressure</span> response of the amide I′ and II′ bands of three small model peptides was examined. Analysis of these bands’ response to increased <span class="hlt">pressure</span> indicates significant side chain <span class="hlt">dependence</span> of their structural rearrangement, which may play a role in the composition of full length proteins of barophilic organisms. PMID:21740637</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21694378','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21694378"><span>High <span class="hlt">pressure</span> study of Pu(0.92)Am(0.08) binary alloy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Klosek, V; Griveau, J C; Faure, P; Genestier, C; Baclet, N; Wastin, F</p> <p>2008-07-09</p> <p>The phase transitions (by means of x-ray diffraction) and electrical resistivity of a Pu(0.92)Am(0.08) binary alloy were determined under <span class="hlt">pressure</span> (up to 2 GPa). The evolution of atomic volume with <span class="hlt">pressure</span> gives detailed information concerning the degree of localization of 5f electronic states and their delocalization process. A quasi-linear V = f(P) <span class="hlt">dependence</span> reflects subtle modifications of the electronic structure when P increases. The electrical resistivity measurements reveal the very high stability of the δ phase for <span class="hlt">pressures</span> less than 0.7 GPa, since no martensitic-like transformation occurs at low temperature. Remarkable electronic behaviours have also been <span class="hlt">observed</span>. Finally, resistivity curves have shown the temperature <span class="hlt">dependence</span> of the phase transformations together with unexpected kinetic effects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/10516739','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/10516739"><span>Blood <span class="hlt">pressure</span> and social support <span class="hlt">observations</span> from Mamre, South Africa, during social and political transition.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Daniels, A; Hoffman, M; Lombard, C; Steyn, K; Levitt, N; Katzenellenbogen, J</p> <p>1999-10-01</p> <p>Social support, by moderating cardiovascular reactivity, has been demonstrated to attenuate the effects of stress on blood <span class="hlt">pressure</span> in American communities. This is the first report to examine the relationship between social support and blood <span class="hlt">pressure</span> in a South African context, during a period of infrastructure modernisation and political change. A total of 1240 residents (542 men, 698 women) of mixed ethnic origin, older than 14 years and stratified by age and sex, participated in a survey to determine risk factors for hypertension and cardiovascular diseases. Social support was assessed by a questionnaire developed in consultation with the community. It was defined by interactions that may threaten family harmony (score 1) and by networking between relatives, friends, colleagues and neighbours (score 2). Mean blood <span class="hlt">pressure</span> of the sample was 130/79 mm Hg (s.d. 25/14 mm Hg). Hypertension prevalence was 26.9%. Only 36% of women compared to 57.3% of men (P < 0.0001) were employed. More women (29%) than men (22%) reported threats to family harmony, but social support networks were similarly perceived by both sexes. Systolic and diastolic blood <span class="hlt">pressure</span> correlated weakly with score 1 (r = 0.096, P < 0.0007) but no association was <span class="hlt">observed</span> with score 2. Score 1 was not associated with blood <span class="hlt">pressure</span> by multiple regression analysis, that included confounding by age, sex, BMI, alcohol consumption and smoking status. Neither threats to family harmony nor networking between relatives, friends or neighbours, significantly influences blood <span class="hlt">pressure</span> in this community. Measures of social support thought to moderate blood <span class="hlt">pressure</span> may have limited cross-cultural application. Attitudinal changes during socio-political transition may impact on the generalisability of instruments for measurement.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5223461-flux-transfer-events-dayside-magnetopause-transient-reconnection-magnetosheath-dynamic-pressure-pulses','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/5223461-flux-transfer-events-dayside-magnetopause-transient-reconnection-magnetosheath-dynamic-pressure-pulses"><span>Flux transfer events at the dayside magnetopause: Transient reconnection or magnetosheath dynamic <span class="hlt">pressure</span> pulses</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>Lockwood, M.</p> <p>1991-04-01</p> <p>The suggestion is discussed that characteristic particle and field signatures at the dayside magnetopause, termed flux transfer events, are, in at least some cases, due to transient solar wind and/or magnetosheath dynamic <span class="hlt">pressure</span> increases, rather than time-<span class="hlt">dependent</span> magnetic reconnection. It is found that most individual cases of FTEs <span class="hlt">observed</span> by a single spacecraft can, at least qualitatively, be explained by the <span class="hlt">pressure</span> pulse model, provided a few rather unsatisfactory features of the predictions are explained in terms of measurement uncertainties. The most notable exceptions to this are some two-regime <span class="hlt">observations</span> made by two satellites simultaneously, one on either side ofmore » the magnetopause. However, this configuration has not been frequently achieved for sufficient time, such <span class="hlt">observations</span> are rare, and the relevant tests are still not conclusive. The strongest evidence that FTEs are produced by magnetic reconnection is the <span class="hlt">dependence</span> of their occurence on the north-south component of the interplanetary magnetic field (IMF) or of the magnetosheath field. The <span class="hlt">pressure</span> pulse model provides an explanation for this <span class="hlt">dependence</span> in the case of magnetosheath FTEs, but does not apply to magnetosphere FTEs. The only surveys of magnetosphere FTEs have not employed the simultaneous IMF, but have shown that their occurence is strongly <span class="hlt">dependent</span> on the north-south component of the magnetosheath field, as <span class="hlt">observed</span> earlier/later on the same magnetopause crossing. This paper employs statistics on the variability of the IMF orientation to investigate the effects of IMF changes between the times of the magnetosheath and FTE <span class="hlt">observations</span>. It is shown that the previously published results are consistent with magnetospheric FTEs being entirely absent when the magentosheath field is northward.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21576777','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21576777"><span>Temperature and <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the optical properties of Cr3+-doped Gd3Ga5O12 nanoparticles.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Martín-Rodríguez, R; Valiente, R; Rodríguez, F; Bettinelli, M</p> <p>2011-07-01</p> <p>Since the crystal-field strength at the Cr(3+) site is very close to the excited-state crossover (ESCO), this work investigates the optical properties of Cr(3+)-doped Gd(3)Ga(5)O(12) (GGG) nanoparticles as a function of temperature and <span class="hlt">pressure</span> in order to establish the effect of the ESCO on the optical behaviour of nanocrystalline GGG. Luminescence, time-resolved emission and lifetime measurements have been performed on GGG:0.5% Cr(3+) nanoparticles in the 25-300 K temperature range, as well as under hydrostatic <span class="hlt">pressure</span> up to 20 GPa. We show how low temperature and high <span class="hlt">pressure</span> progressively transforms Cr(3+)(4)T(2) --> (4)A(2) broadband emission into a ruby-like (2)E --> (4)A(2) luminescence. This behaviour together with the lifetime <span class="hlt">dependence</span> on <span class="hlt">pressure</span> and temperature are explained on the basis of the spin-orbit interaction between the (4)T(2) and (2)E states of Cr(3+).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15811750','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15811750"><span>Experimental <span class="hlt">observation</span> of intraocular <span class="hlt">pressure</span> changes during microkeratome suctioning in laser in situ keratomileusis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bissen-Miyajima, Hiroko; Suzuki, Shintaro; Ohashi, Yoshie; Minami, Keiichiro</p> <p>2005-03-01</p> <p>To <span class="hlt">observe</span> changes in intraocular <span class="hlt">pressure</span> (IOP), the manner in which the eye is suctioned, and the effect of the number of suction ports. Department of Ophthalmology, Tokyo Dental College, Suidobashi Hospital, Tokyo, Japan. Suction rings with single or dual ports were made of transparent acrylic acid resin to facilitate <span class="hlt">observation</span> with a digital video camera. The IOP and the duration of the IOP increase (time to reach 90% of the maximum IOP) were measured in 6 porcine eyes with an intra-vein <span class="hlt">pressure</span>-sensor catheter in the vitreous cavity. The IOP changes were recorded using a personal computer. Suctioning with single- and dual-port suction rings was similar. The IOP increases with single- and dual-port suction rings were similar (99.1 mm Hg +/- 6.1 [SD] and 99.0 +/- 6.5 mm Hg, respectively) (P=.987). The duration of the IOP increase was also similar (4.21 +/- 0.24 seconds and 4.12 +/- 0.33 seconds, respectively) (P=.190). The number of ports did not affect suctioning and changes in IOP. This technique is useful in developing the ideal shape and setting of the suction ring.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1918713Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1918713Z"><span>Cracked rocks with positive and negative Poisson's ratio: real-crack properties extracted from <span class="hlt">pressure</span> <span class="hlt">dependence</span> of elastic-wave velocities</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zaitsev, Vladimir Y.; Radostin, Andrey V.; Dyskin, Arcady V.; Pasternak, Elena</p> <p>2017-04-01</p> <p>We report results of analysis of literature data on P- and S-wave velocities of rocks subjected to variable hydrostatic <span class="hlt">pressure</span>. Out of about 90 examined samples, in more than 40% of the samples the reconstructed Poisson's ratios are negative for lowest confining <span class="hlt">pressure</span> with gradual transition to the conventional positive values at higher <span class="hlt">pressure</span>. The portion of rocks exhibiting negative Poisson's ratio appeared to be unexpectedly high. To understand the mechanism of negative Poisson's ratio, <span class="hlt">pressure</span> <span class="hlt">dependences</span> of P- and S-wave velocities were analyzed using the effective medium model in which the reduction in the elastic moduli due to cracks is described in terms of compliances with respect to shear and normal loading that are imparted to the rock by the presence of cracks. This is in contrast to widely used descriptions of effective cracked medium based on a specific crack model (e.g., penny-shape crack) in which the ratio between normal and shear compliances of such a crack is strictly predetermined. The analysis of <span class="hlt">pressure-dependences</span> of the elastic wave velocities makes it possible to reveal the ratio between pure normal and shear compliances (called q-ratio below) for real defects and quantify their integral content in the rock. The examination performed demonstrates that a significant portion (over 50%) of cracks exhibit q-ratio several times higher than that assumed for the conventional penny-shape cracks. This leads to faster reduction of the Poisson's ratio with increasing the crack concentration. Samples with negative Poisson's ratio are characterized by elevated q-ratio and simultaneously crack concentration. Our results clearly indicate that the traditional crack model is not adequate for a significant portion of rocks and that the interaction between the opposite crack faces leading to domination of the normal compliance and reduced shear displacement discontinuity can play an important role in the mechanical behavior of rocks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMDI41C2638K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMDI41C2638K"><span>Melting temperatures of MgO under high <span class="hlt">pressure</span> determined by micro-texture <span class="hlt">observation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kimura, T.; Ohfuji, H.; Nishi, M.; Irifune, T.</p> <p>2016-12-01</p> <p>Periclase (MgO) is the second abundant mineral after bridgmanite in the Earth's lower mantle, and its melting temperature (Tm) under <span class="hlt">pressure</span> is important to constrain the chemical composition of ultra-deep magma formed near the mantle-core boundary. However, the melting behavior is highly controversial among previous studies: a laser-heated diamond anvil cell (LHDAC) study reported a melting curve with a dTm/dP of 30 K/GPa at zero <span class="hlt">pressure</span> [1], while several theoretical computations gave substantially higher dTm/dP of 90 100 K/GPa [2,3]. We performed a series of LHDAC experiments for measurements of Tm of MgO under high <span class="hlt">pressure</span>, using single crystal MgO as the starting material. The melting was detected by using micro-texture <span class="hlt">observations</span> of the quenched samples. We found that the laser-heated area of the sample quenched from the Tm in previous LHDAC experiments [1] showed randomly aggregated granular crystals, which was not caused by melting, but by plastic deformation of the sample. This suggests that the Tms of their study were substantially underestimated. On the other hand, the sample recovered from the temperature higher by 1500-1700 K than the Tms in previous LHDAC experiments showed a characteristic internal texture comparable to the solidification texture typically shown in metal casting. We determined the Tms based on the <span class="hlt">observation</span> of this texture up to 32 GPa. Fitting our Tms to the Simon equation yields dTm/dP of 82 K/GPa at zero <span class="hlt">pressure</span>, which is consistent with those of the theoretical predictions (90 100 K/GPa) [2,3]. Extrapolation of the present melting curve of MgO to the <span class="hlt">pressure</span> of the CMB (135 GPa) gives a melting temperature of 8900 K. The present steep melting slope offers the eutectic composition close to peridotite (in terms of Mg/Si ratio) throughout the lower mantle conditions. According to the model for sink/float relationship between the solid mantle and the magma [4], a considerable amount of iron (Fe/(Mg+Fe) > 0.24) is expected</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930050380&hterms=fundamentals+characteristics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dfundamentals%2Bcharacteristics','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930050380&hterms=fundamentals+characteristics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dfundamentals%2Bcharacteristics"><span>Characteristics of a high <span class="hlt">pressure</span> gas proportional counter filled with xenon</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sakurai, H.; Ramsey, B. D.</p> <p>1991-01-01</p> <p>The characteristics of a conventional cylindrical geometry proportional counter filled with high <span class="hlt">pressure</span> xenon gas up to 10 atm. were fundamentally investigated for use as a detector in hard X-ray astronomy. With a 2 percent methane gas mixture the energy resolutions at 10 atm. were 9.8 percent and 7.3 percent for 22 keV and 60 keV X-rays, respectively. From calculations of the Townsend ionization coefficient, it is shown that proportional counters at high <span class="hlt">pressure</span> operate at weaker reduced electric field than low <span class="hlt">pressure</span> counters. The characteristics of a parallel grid proportional counter at low <span class="hlt">pressure</span> showed similar <span class="hlt">pressure</span> <span class="hlt">dependence</span>. It is suggested that this is the fundamental reason for the degradation of resolution <span class="hlt">observed</span> with increasing <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27878400','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27878400"><span>Multiphoton microscopy <span class="hlt">observations</span> of 3D elastin and collagen fiber microstructure changes during <span class="hlt">pressurization</span> in aortic media.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sugita, Shukei; Matsumoto, Takeo</p> <p>2017-06-01</p> <p>Elastin and collagen fibers play important roles in the mechanical properties of aortic media. Because knowledge of local fiber structures is required for detailed analysis of blood vessel wall mechanics, we investigated 3D microstructures of elastin and collagen fibers in thoracic aortas and monitored changes during <span class="hlt">pressurization</span>. Using multiphoton microscopy, autofluorescence images from elastin and second harmonic generation signals from collagen were acquired in media from rabbit thoracic aortas that were stretched biaxially to restore physiological dimensions. Both elastin and collagen fibers were <span class="hlt">observed</span> in all longitudinal-circumferential plane images, whereas alternate bright and dark layers were <span class="hlt">observed</span> along the radial direction and were recognized as elastic laminas (ELs) and smooth muscle-rich layers (SMLs), respectively. Elastin and collagen fibers are mainly oriented in the circumferential direction, and waviness of collagen fibers was significantly higher than that of elastin fibers. Collagen fibers were more undulated in longitudinal than in radial direction, whereas undulation of elastin fibers was equibiaxial. Changes in waviness of collagen fibers during <span class="hlt">pressurization</span> were then evaluated using 2-dimensional fast Fourier transform in mouse aortas, and indices of waviness of collagen fibers decreased with increases in intraluminal <span class="hlt">pressure</span>. These indices also showed that collagen fibers in SMLs became straight at lower intraluminal <span class="hlt">pressures</span> than those in EL, indicating that SMLs stretched more than ELs. These results indicate that deformation of the aorta due to <span class="hlt">pressurization</span> is complicated because of the heterogeneity of tissue layers and differences in elastic properties of ELs, SMLs, and surrounding collagen and elastin.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPCS..113....1O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPCS..113....1O"><span>Phase transformation of GaAs at high <span class="hlt">pressures</span> and temperatures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ono, Shigeaki; Kikegawa, Takumi</p> <p>2018-02-01</p> <p>The high-<span class="hlt">pressure</span> behavior of gallium arsenide, GaAs, has been investigated using an in-situ X-ray powder diffraction technique in a diamond anvil cell combined with a resistance heating method, at <span class="hlt">pressures</span> and temperatures up to 25 GPa and 1000 K respectively. The <span class="hlt">pressure</span>-induced phase transition from a zincblende to an orthorhombic (Cmcm) structure was <span class="hlt">observed</span>. This transition occurred at 17.3 GPa and at room temperature, where a negative temperature <span class="hlt">dependence</span> for this transition was confirmed. The transition boundary was determined to be P (GPa) = 18.0 - 0.0025 × T (K).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28581758','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28581758"><span>Molecular Gibbs Surface Excess and CO2-Hydrate Density Determine the Strong Temperature- and <span class="hlt">Pressure-Dependent</span> Supercritical CO2-Brine Interfacial Tension.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ji, Jiayuan; Zhao, Lingling; Tao, Lu; Lin, Shangchao</p> <p>2017-06-29</p> <p>In CO 2 geological storage, the interfacial tension (IFT) between supercritical CO 2 and brine is critical for the storage capacitance design to prevent CO 2 leakage. IFT relies not only on the interfacial molecule properties but also on the environmental conditions at different storage sites. In this paper, supercritical CO 2 -NaCl solution systems are modeled at 343-373 K and 6-35 MPa under the salinity of 1.89 mol/L using molecular dynamics simulations. After computing and comparing the molecular density profile across the interface, the atomic radial distribution function, the molecular orientation distribution, the molecular Gibbs surface excess (derived from the molecular density profile), and the CO 2 -hydrate number density under the above environmental conditions, we confirm that only the molecular Gibbs surface excess of CO 2 molecules and the CO 2 -hydrate number density correlate strongly with the temperature- and <span class="hlt">pressure-dependent</span> IFTs. We also compute the populations of two distinct CO 2 -hydrate structures (T-type and H-type) and attribute the <span class="hlt">observed</span> <span class="hlt">dependence</span> of IFTs to the dominance of the more stable, surfactant-like T-type CO 2 -hydrates at the interface. On the basis of these new molecular mechanisms behind IFT variations, this study could guide the rational design of suitable injecting environmental <span class="hlt">pressure</span> and temperature conditions. We believe that the above two molecular-level metrics (Gibbs surface excess and hydrate number density) are of great fundamental importance for understanding the supercritical CO 2 -water interface and engineering applications in geological CO 2 storage.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhCS.899b2003D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhCS.899b2003D"><span>An experimental study of <span class="hlt">dependence</span> of hydro turbine vibration parameters on <span class="hlt">pressure</span> pulsations in the flow path</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dekterev, D.; Maslennikova, A.; Abramov, A.</p> <p>2017-09-01</p> <p>The operation modes of the hydraulic power plant water turbine with the formation of a precessing vortex core were studied on the hydrodynamic set-up with the model of hydraulic unit. The <span class="hlt">dependence</span> of low-frequency vibrations on flow <span class="hlt">pressure</span> pulsations in the hydraulic unit was established. The results of the air injection effect on the vibrational parameters of the hydrodynamic set-up were presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19980015260&hterms=wine&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dwine','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19980015260&hterms=wine&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dwine"><span>Kinetics of the BrO + NO2 Association Reaction. Temperature and <span class="hlt">Pressure</span> <span class="hlt">Dependence</span> in the Falloff Regime</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Thron, R. P.; Daykin, E. P.; Wine, P.H.</p> <p>1997-01-01</p> <p>A laser flash photolysis-long path absorption technique has been employed to study the kinetics of the reaction BrO + NO2 + M yields (k1) products as a function of temperature (248-346 K), <span class="hlt">pressure</span> (16-800 torr), and buffer gas identity (N2,CF4) The reaction is found to be in the falloff regime between third and second-order over the entire range of conditions investigated This is the first study where temperature-<span class="hlt">dependent</span> measurements of k1(P,T) have been reported at <span class="hlt">pressures</span> greater than 12 torr; hence, our results help constrain choices of k1(P,T) for use in models of lower stratospheric BrO(x) chemistry. Approximate falloff parameters in a convenient form for atmospheric modeling are derived.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29020268','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29020268"><span>Office blood <span class="hlt">pressure</span> or ambulatory blood <span class="hlt">pressure</span> for the prediction of cardiovascular events.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mortensen, Rikke Nørmark; Gerds, Thomas Alexander; Jeppesen, Jørgen Lykke; Torp-Pedersen, Christian</p> <p>2017-11-21</p> <p>To determine the added value of (i) 24-h ambulatory blood <span class="hlt">pressure</span> relative to office blood <span class="hlt">pressure</span> and (ii) night-time ambulatory blood <span class="hlt">pressure</span> relative to daytime ambulatory blood <span class="hlt">pressure</span> for 10-year person-specific absolute risks of fatal and non-fatal cardiovascular events. A total of 7927 participants were included from the International Database on Ambulatory blood <span class="hlt">pressure</span> monitoring in relation to Cardiovascular Outcomes. We used cause-specific Cox regression to predict 10-year person-specific absolute risks of fatal and non-fatal cardiovascular events. Discrimination of 10-year outcomes was assessed by time-<span class="hlt">dependent</span> area under the receiver operating characteristic curve (AUC). No differences in predicted risks were <span class="hlt">observed</span> when comparing office blood <span class="hlt">pressure</span> and ambulatory blood <span class="hlt">pressure</span>. The median difference in 10-year risks (1st; 3rd quartile) was -0.01% (-0.3%; 0.1%) for cardiovascular mortality and -0.1% (-1.1%; 0.5%) for cardiovascular events. The difference in AUC (95% confidence interval) was 0.65% (0.22-1.08%) for cardiovascular mortality and 1.33% (0.83-1.84%) for cardiovascular events. Comparing daytime and night-time blood <span class="hlt">pressure</span>, the median difference in 10-year risks was 0.002% (-0.1%; 0.1%) for cardiovascular mortality and -0.01% (-0.5%; 0.2%) for cardiovascular events. The difference in AUC was 0.10% (-0.08 to 0.29%) for cardiovascular mortality and 0.15% (-0.06 to 0.35%) for cardiovascular events. Ten-year predictions obtained from ambulatory blood <span class="hlt">pressure</span> are similar to predictions from office blood <span class="hlt">pressure</span>. Night-time blood <span class="hlt">pressure</span> does not improve 10-year predictions obtained from daytime measurements. For an otherwise healthy population sufficient prognostic accuracy of cardiovascular risks can be achieved with office blood <span class="hlt">pressure</span>. Published on behalf of the European Society of Cardiology. All rights reserved. © The Author 2017. For permissions, please email: journals.permissions@oup.com.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930027453&hterms=platinum&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dplatinum','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930027453&hterms=platinum&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dplatinum"><span><span class="hlt">Pressure</span> <span class="hlt">dependence</span> of the oxygen reduction reaction at the platinum microelectrode/nafion interface - Electrode kinetics and mass transport</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Parthasarathy, Arvind; Srinivasan, Supramaniam; Appleby, A. J.; Martin, Charles R.</p> <p>1992-01-01</p> <p>The investigation of oxygen reduction kinetics at the platinum/Nafion interface is of great importance in the advancement of proton-exchange-membrane (PEM) fuel-cell technology. This study focuses on the <span class="hlt">dependence</span> of the oxygen reduction kinetics on oxygen <span class="hlt">pressure</span>. Conventional Tafel analysis of the data shows that the reaction order with respect to oxygen is unity at both high and low current densities. Chronoamperometric measurements of the transport parameters for oxygen in Nafion show that oxygen dissolution follows Henry's isotherm. The diffusion coefficient of oxygen is invariant with <span class="hlt">pressure</span>; however, the diffusion coefficient for oxygen is lower when air is used as the equilibrating gas as compared to when oxygen is used for equilibration. These results are of value in understanding the influence of O2 partial <span class="hlt">pressure</span> on the performance of PEM fuel cells and also in elucidating the mechanism of oxygen reduction at the platinum/Nafion interface.</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('http://adsabs.harvard.edu/abs/2018JChPh.148i4201M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JChPh.148i4201M"><span>Nano-viscosity of supercooled liquid measured by fluorescence correlation spectroscopy: <span class="hlt">Pressure</span> and temperature <span class="hlt">dependence</span> and the density scaling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Meier, G.; Gapinski, J.; Ratajczyk, M.; Lettinga, M. P.; Hirtz, K.; Banachowicz, E.; Patkowski, A.</p> <p>2018-03-01</p> <p>The Stokes-Einstein relation allows us to calculate apparent viscosity experienced by tracers in complex media on the basis of measured self-diffusion coefficients. Such defined nano-viscosity values can be obtained through single particle techniques, like fluorescence correlation spectroscopy (FCS) and particle tracking (PT). In order to perform such measurements, as functions of <span class="hlt">pressure</span> and temperature, a new sample cell was designed and is described in this work. We show that this cell in combination with a long working distance objective of the confocal microscope can be used for successful FCS, PT, and confocal imaging experiments in broad <span class="hlt">pressure</span> (0.1-100 MPa) and temperature ranges. The temperature and <span class="hlt">pressure</span> <span class="hlt">dependent</span> nano-viscosity of a van der Waals liquid obtained from the translational diffusion coefficient measured in this cell by means of FCS obeys the same scaling as the rotational relaxation and macro-viscosity of the system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMMR41B0410S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR41B0410S"><span>Micro X-ray CT imaging of pore-scale changes in unconsolidated sediment under confining <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>Schindler, M.; Prasad, M.</p> <p>2017-12-01</p> <p>Micro X-ray computed tomography was used to image confining-<span class="hlt">pressure</span> induced changes in a dry, unconsolidated quartz sand pack while simultaneously recording ultrasonic P-wave velocities. The experiments were performed under in-situ <span class="hlt">pressure</span> of up to 4000 psi. The majority of digital rock physics studies rely on micro CT images obtained under ambient <span class="hlt">pressure</span> and temperature conditions although effective rock properties strongly <span class="hlt">depend</span> on in situ conditions. Goal of this work is to be able to obtain micro CT images of rock samples while pore and confining <span class="hlt">pressure</span> is applied. Simultaneously we recorded ultrasonic P-wave velocities. The combination of imaging and velocity measurements provides insight in pore-scale changes in the rock and their influence on elastic properties. We visually <span class="hlt">observed</span> a reduction in porosity by more than a third of the initial value as well as extensive grain damage, changes in pore and grain size distribution and an increase in contact number and contact radius with increasing confining <span class="hlt">pressure</span>. An increase in measured ultrasonic P-wave velocities with increasing <span class="hlt">pressure</span> was <span class="hlt">observed</span>. We used porosity, contact number and contact radius obtained from micro CT images to model P-wave velocity with the contact-radius model by Bachrach et al. (1998). Our <span class="hlt">observations</span> showed that the frame of unconsolidated sediments is significantly altered starting at <span class="hlt">pressures</span> of only 1000 psi. This finding indicates that common assumptions in rock physics models (the solid frame remains unchanged) are violated for unconsolidated sediments. The effects on the solid frame should be taken into account when modeling the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of elastic rock properties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.T13H..03K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.T13H..03K"><span>Simultaneous <span class="hlt">observations</span> of reaction kinetics, creep behavior, and AE activities during syndeformational antigorite dehydration at high <span class="hlt">pressures</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kubo, T.; Iwasato, T.; Higo, Y.; Kato, T.; Kaneshima, S.; Uehara, S.; Koizumi, S.; Imamura, M.; Tange, Y.</p> <p>2015-12-01</p> <p>Intermediate-depth earthquakes are seismic activities in Wadati-Benioff zone at depths from 60 km to 300 km, where subducting plates deform plastically rather than brittle failure. Although it has been reported that unstable faulting occurred during antigorite dehydration even at higher <span class="hlt">pressures</span> than ~2 GPa (e.g., Jung et al., 2009), the recent study by Chernak and Hirth (2011) revealed that the syndefromational antigorite dehydration does not produces stick-slip instabilities but stable fault slip. In the present study, we newly developed an AE monitoring system for high-<span class="hlt">pressure</span> reaction-deformation processes combined with D-DIA and synchrotron monochromatic X-ray to <span class="hlt">observe</span> reaction kinetics, creep behaviors, and AE activities simultaneously. We applied this technique to investigate shear instability during syndeformational antigorite dehydration. High-<span class="hlt">pressure</span> deformation experiments were conducted up to ~8 GPa, ~1050 K, and strain rates of 3.4-9.2 x 10-5 s-1 in compression using a D-DIA type apparatus installed at BL-04B1, SPring-8. 50 keV mono X-ray were used to measure reaction kinetics and stress-strain data. To monitor shear instabilities by detecting AEs, six piezoelectric devices were positioned between first and second stage anvils of MA 6-6 type system. We used three kinds of starting materials of polycrystalline antigorite, fine-grained forsterite polycrystal, and two-phase mixtures of antigorite and San Carlos olivine (10%, 30%, and 50%atg). Clear contrasts were <span class="hlt">observed</span> in AE activities between forsterite and antigorite samples. AE activities detected within the forsterite polycrystal suggested (semi) brittle behaviors at low <span class="hlt">pressures</span> during the cold compression stage.
Almost no AEs were detected within the antigorite samples during any stages of cold compression, ramping, deformation, and syndeformational dehydration although localized deformation textures were <span class="hlt">observed</span> in recovered samples. Instead, we detected some AEs outside the sample</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008ApPhL..93w1503L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008ApPhL..93w1503L"><span><span class="hlt">Observation</span> of collisionless heating of low energy electrons in low <span class="hlt">pressure</span> inductively coupled argon plasmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, Min-Hyong; Lee, Hyo-Chang; Chung, Chin-Wook</p> <p>2008-12-01</p> <p>Collisionless heating of low energy electrons was <span class="hlt">observed</span> in low <span class="hlt">pressure</span> argon rf-biased inductively coupled plasmas (ICPs) by measurement of the electron energy distribution function (EEDF). When only capacitive power (bias) was supplied, the EEDF in the discharge was a bi-Maxwellian distribution with two electron groups. It was found that the low energy electrons were heated up significantly even with a little inductive power (<20 W) even when the discharge was in E mode. Due to the low gas <span class="hlt">pressure</span> and low temperature of low energy electrons (close to the energy of the Ramsauer minimum), the collisional heating of low energy electrons appears to be negligible. Therefore, this effective heating of the low energy electrons showed a direct experimental evidence of the collisionless heating by inductive field. The significant heating of low energy electrons in E mode indicates that collisionless heating in the skin layer is an important electron heating mechanism of low <span class="hlt">pressure</span> ICP even when the discharge is in E mode.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1055687','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1055687"><span>Oxygen isotope fractionation in the vacuum ultraviolet photodissociation of carbon monoxide: Wavelength, <span class="hlt">pressure</span> and temperature <span class="hlt">dependency</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>Chakraborty, Subrata; Davis, Ryan; Ahmed, Musahid</p> <p></p> <p>Several absorption bands exist in the VUV region of Carbon monoxide (CO). Emission spectra indicate that these bands are all predissociative. An experimental investigation of CO photodissociation by vacuum ultraviolet photons (90 to 108 nm; ~13 to 11 eV) from the Advanced Light Source Synchrotron and direct measurement of the associated oxygen isotopic composition of the products are presented here. A wavelength <span class="hlt">dependency</span> of the oxygen isotopic composition in the photodissociation product was <span class="hlt">observed</span>. Slope values (δ'{sup 18}O/ δ'{sup 17}O) ranging from 0.76 to 1.32 were <span class="hlt">observed</span> in oxygen three-isotope space (δ'{sup 18}O vs. δ'{sup 17}O) which correlated with increasingmore » synchrotron photon energy, and indicate a <span class="hlt">dependency</span> of the upper electronic state specific dissociation dynamics (e.g., perturbation and coupling associated with a particular state). An unprecedented magnitude in isotope separation was <span class="hlt">observed</span> for photodissociation at the 105 and 107 nm synchrotron bands and are found to be associated with accidental predissociation of the vibrational states ({nu} = 0 and 1) of the upper electronic state E{sup 1}Π. For each synchrotron band, a large (few hundred per mil) extent of isotopic fractionation was <span class="hlt">observed</span> and the range of fractionation is a combination of column density and exposure time. A significant temperature <span class="hlt">dependency</span> in oxygen isotopic fractionation was <span class="hlt">observed</span>, indicating a rotational level <span class="hlt">dependency</span> in the predissociation process.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19970000409','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19970000409"><span><span class="hlt">Observations</span> of Time-<span class="hlt">Dependent</span> Behavior in the Two-Layer Rayleigh-Benard System</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Andereck, C. David; Colovas, Peter W.; Degen, Michael M.</p> <p>1996-01-01</p> <p>In this paper we present results from experiments with a system consisting of two immiscible fluid layers in rectangular and annular geometries, driven by a vertical temperature gradient. Time-<span class="hlt">dependent</span> variations in the type of coupling <span class="hlt">observed</span> between the two layers are described and characterized.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930091965','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930091965"><span>Knocking Combustion <span class="hlt">Observed</span> in a Spark-Ignition Engine with Simultaneous Direct and Schlieren High-Speed Motion Pictures and <span class="hlt">Pressure</span> Records</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Osterstrom, Gordon E</p> <p>1948-01-01</p> <p>Simultaneous direct and Schlieren photographs at 40,000 frames per second and correlated <span class="hlt">pressure</span> records were taken of knocking combustion in a special spark-ignition engine to ascertain the intensity of certain end-zone reactions previously noted from Schlieren photography alone. A violent propagated homogeneous autoignition, or a similar phenomenon, previously <span class="hlt">observed</span>, was again <span class="hlt">observed</span>. The <span class="hlt">pressure</span> records show autoignition of varying violence before the passage of a probable detonation wave. Extensive autoignition without occurrence of gas vibrations was seen in one explosion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/869670','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/869670"><span>Apparatus and method for non-contact, acoustic resonance determination of intraocular <span class="hlt">pressure</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Sinha, Dipen N.; Wray, William O.</p> <p>1994-01-01</p> <p>Apparatus and method for measuring intraocular <span class="hlt">pressure</span> changes in an eye under investigation by detection of vibrational resonances therein. An ultrasonic transducer operating at its resonant frequency is amplitude modulated and swept over a range of audio frequencies in which human eyes will resonate. The output therefrom is focused onto the eye under investigation, and the resonant vibrations of the eye <span class="hlt">observed</span> using a fiber-optic reflection vibration sensor. Since the resonant frequency of the eye is <span class="hlt">dependent</span> on the <span class="hlt">pressure</span> therein, changes in intraocular <span class="hlt">pressure</span> may readily be determined after a baseline <span class="hlt">pressure</span> is established.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6609230','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/6609230"><span>Apparatus and method for non-contact, acoustic resonance determination of intraocular <span class="hlt">pressure</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Sinha, D.N.; Wray, W.O.</p> <p>1994-12-27</p> <p>The apparatus and method for measuring intraocular <span class="hlt">pressure</span> changes in an eye under investigation by detection of vibrational resonances therein. An ultrasonic transducer operating at its resonant frequency is amplitude modulated and swept over a range of audio frequencies in which human eyes will resonate. The output therefrom is focused onto the eye under investigation, and the resonant vibrations of the eye <span class="hlt">observed</span> using a fiber-optic reflection vibration sensor. Since the resonant frequency of the eye is <span class="hlt">dependent</span> on the <span class="hlt">pressure</span> therein, changes in intraocular <span class="hlt">pressure</span> may readily be determined after a baseline <span class="hlt">pressure</span> is established. 3 figures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004MeScT..15.1185M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004MeScT..15.1185M"><span>Exhaust <span class="hlt">pressure</span> pulsation <span class="hlt">observation</span> from turbocharger instantaneous speed measurement</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Macián, V.; Luján, J. M.; Bermúdez, V.; Guardiola, C.</p> <p>2004-06-01</p> <p>In internal combustion engines, instantaneous exhaust <span class="hlt">pressure</span> measurements are difficult to perform in a production environment. The high temperature of the exhaust manifold and its pulsating character make its application to exhaust gas recirculation control algorithms impossible. In this paper an alternative method for estimating the exhaust <span class="hlt">pressure</span> pulsation is presented. A numerical model is built which enables the exhaust <span class="hlt">pressure</span> pulses to be predicted from instantaneous turbocharger speed measurements. Although the model is data based, a theoretical description of the process is also provided. This combined approach makes it possible to export the model for different engine operating points. Also, compressor contribution in the turbocharger speed pulsation is discussed extensively. The compressor contribution is initially neglected, and effects of this simplified approach are analysed.</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 <span class="hlt">Dependent</span> 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> gradient 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> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JChPh.147r4107Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JChPh.147r4107Y"><span>Development of isothermal-isobaric replica-permutation method for molecular dynamics and Monte Carlo simulations and its application to reveal temperature and <span class="hlt">pressure</span> <span class="hlt">dependence</span> of folded, misfolded, and unfolded states of chignolin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yamauchi, Masataka; Okumura, Hisashi</p> <p>2017-11-01</p> <p>We developed a two-dimensional replica-permutation molecular dynamics method in the isothermal-isobaric ensemble. The replica-permutation method is a better alternative to the replica-exchange method. It was originally developed in the canonical ensemble. This method employs the Suwa-Todo algorithm, instead of the Metropolis algorithm, to perform permutations of temperatures and <span class="hlt">pressures</span> among more than two replicas so that the rejection ratio can be minimized. We showed that the isothermal-isobaric replica-permutation method performs better sampling efficiency than the isothermal-isobaric replica-exchange method and infinite swapping method. We applied this method to a β-hairpin mini protein, chignolin. In this simulation, we <span class="hlt">observed</span> not only the folded state but also the misfolded state. We calculated the temperature and <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the fractions on the folded, misfolded, and unfolded states. Differences in partial molar enthalpy, internal energy, entropy, partial molar volume, and heat capacity were also determined and agreed well with experimental data. We <span class="hlt">observed</span> a new phenomenon that misfolded chignolin becomes more stable under high-<span class="hlt">pressure</span> conditions. We also revealed this mechanism of the stability as follows: TYR2 and TRP9 side chains cover the hydrogen bonds that form a β-hairpin structure. The hydrogen bonds are protected from the water molecules that approach the protein as the <span class="hlt">pressure</span> increases.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25904000','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25904000"><span>A prospective <span class="hlt">observational</span> study comparing a non-operator <span class="hlt">dependent</span> automatic PWV analyser to pulse <span class="hlt">pressure</span>, in assessing arterial stiffness in hemodialysis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Salvadé, Igor; Schätti-Stählin, Sibylle; Violetti, Eleonora; Schönholzer, Carlo; Cereghetti, Claudio; Zwahlen, Hugo; Berwert, Lorenzo; Burnier, Michel; Gabutti, Luca</p> <p>2015-04-23</p> <p>Chronic kidney disease (CKD) accelerates vascular stiffening related to age. Arterial stiffness may be evaluated measuring the carotid-femoral pulse wave velocity (PWV) or more simply, as recommended by KDOQI, monitoring pulse <span class="hlt">pressure</span> (PP). Both correlate to survival and incidence of cardiovascular disease. PWV can also be estimated on the brachial artery using a Mobil-O-Graph; a non-operator <span class="hlt">dependent</span> automatic device. The aim was to analyse whether, in a dialysis population, PWV obtained by Mobil-O-Graph (MogPWV) is more sensitive for vascular aging than PP. A cohort of 143 patients from 4 dialysis units has been followed measuring MogPWV and PP every 3 to 6 months and compared to a control group with the same risk factors but an eGFR > 30 ml/min. MogPWV contrarily to PP did discriminate the dialysis population from the control group. The mean difference translated in age between the two populations was 8.4 years. The increase in MogPWV, as a function of age, was more rapid in the dialysis group. 13.3% of the dialysis patients but only 3.0% of the control group were outliers for MogPWV. The mortality rate (16 out of 143) was similar in outliers and inliers (7.4 and 8.0%/year). Stratifying patients according to MogPWV, a significant difference in survival was seen. A high parathormone (PTH) and to be dialysed for a hypertensive nephropathy were associated to a higher baseline MogPWV. Assessing PWV on the brachial artery using a Mobil-O-Graph is a valid and simple alternative, which, in the dialysis population, is more sensitive for vascular aging than PP. As demonstrated in previous studies PWV correlates to mortality. Among specific CKD risk factors only PTH is associated with a higher baseline PWV. ClinicalTrials.gov Identifier: NCT02327962.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1242673-pressure-dependence-magnetic-ground-states-mnp','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1242673-pressure-dependence-magnetic-ground-states-mnp"><span><span class="hlt">Pressure</span> <span class="hlt">dependence</span> of the magnetic ground states in MnP</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Matsuda, Masaaki; Ye, Feng; Dissanayake, Sachith E.; ...</p> <p>2016-03-17</p> <p>MnP, a superconductor under <span class="hlt">pressure</span>, exhibits a ferromagnetic order below TC~290 K followed by a helical order with the spins lying in the ab plane and the helical rotation propagating along the c axis below Ts~50 K at ambient <span class="hlt">pressure</span>. We performed single-crystal neutron diffraction experiments to determine the magnetic ground states under <span class="hlt">pressure</span>. Both TC and Ts are gradually suppressed with increasing <span class="hlt">pressure</span> and the helical order disappears at ~1.2 GPa. At intermediate <span class="hlt">pressures</span> of 1.8 and 2.0 GPa, the ferromagnetic order first develops and changes to a conical or two-phase (ferromagnetic and helical) structure with the propagation alongmore » the b axis below a characteristic temperature. At 3.8 GPa, a helical magnetic order appears below 208 K, which hosts the spins in the ac plane and the propagation along the b axis. The period of this b axis modulation is shorter than that at 1.8 GPa. Here, our results indicate that the magnetic phase in the vicinity of the superconducting phase may have a helical magnetic correlation along the b axis.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22399900','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22399900"><span>Diode laser detection of greenhouse gases in the near-infrared region by wavelength modulation spectroscopy: <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the detection sensitivity.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Asakawa, Takashi; Kanno, Nozomu; Tonokura, Kenichi</p> <p>2010-01-01</p> <p>We have investigated the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the detection sensitivity of CO(2), N(2)O and CH(4) using wavelength modulation spectroscopy (WMS) with distributed feed-back diode lasers in the near infrared region. The spectral line shapes and the background noise of the second harmonics (2f) detection of the WMS were analyzed theoretically. We determined the optimum <span class="hlt">pressure</span> conditions in the detection of CO(2), N(2)O and CH(4), by taking into consideration the background noise in the WMS. At the optimum total <span class="hlt">pressure</span> for the detection of CO(2), N(2)O and CH(4), the limits of detection in the present system were determined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1225544-anisotropic-hc2-thermodynamic-transport-measurements-pressure-dependence-tc-k2cr3as3-single-crystals','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1225544-anisotropic-hc2-thermodynamic-transport-measurements-pressure-dependence-tc-k2cr3as3-single-crystals"><span>Anisotropic H c 2 , thermodynamic and transport measurements, and <span class="hlt">pressure</span> <span class="hlt">dependence</span> of T c in K 2 Cr 3 As 3 single crystals</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Kong, Tai; Bud'ko, Sergey L.; Canfield, Paul C.</p> <p>2015-01-30</p> <p>We present a detailed study of single crystalline K 2Cr 3As 3 and analyze its thermodynamic and transport properties, anisotropic H c2(T), and initial <span class="hlt">pressure</span> <span class="hlt">dependence</span> of T c. In zero field, the temperature-<span class="hlt">dependent</span> resistivity is metallic. Deviation from a linear temperature <span class="hlt">dependence</span> is evident below 100 K and a T 3 <span class="hlt">dependence</span> is roughly followed from just above T c (~10K) to ~40K. Anisotropic H c2(T) data were measured up to 140 kOe with field applied along and perpendicular to the rodlike crystals. For the applied field perpendicular to the rod, H c2(T) is linear with a slope ~–70more » kOe/K. For field applied along the rod, the slope is about –120 kOe/K below 70 kOe. Above 70 kOe, the magnitude of the slope decreases to ~–70 kOe/K. The electronic specific heat coefficient γ, just above T c, is 73 mJ/mol K 2; the Debye temperature Θ D is 220 K. As a result, the specific heat jump at the superconducting transition ΔC~2.2γT c. Finally, for hydrostatic <span class="hlt">pressures</span> up to ~7 kbar, T c decreases under <span class="hlt">pressure</span> linearly at a rate of –0.034K/kbar.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006APS..MARY39012K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006APS..MARY39012K"><span><span class="hlt">Pressure</span> <span class="hlt">Dependence</span> Transport Studies of the Possible Charge Kondo Effect in Tl-doped PbTe</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kurosaki, Yosuke; Shinagawa, Jun; Matsushita, Yana; Geballe, Ted; Fisher, Ian; Brown, Stuart</p> <p>2006-03-01</p> <p>Pb1-xTlxTe is noteworthy for a high superconducting transition temperature relative to carrier concentration, as well as normal state properties consistent with a charge-Kondo effect. Recent experiments also demonstrate that the onset of an <span class="hlt">observable</span> superconducting Tc with Tl concentration at x˜0.3% coincides with features characteristic of charge Kondo [1], including dρ/dT<0 at low temperatures and an unusual linear variation of the resistivity ρ(T)=ρ0+AT at higher temperatures. Together, these <span class="hlt">observations</span> are consistent with an association between the two phenomena [2]. We report the effect of applied <span class="hlt">pressures</span> up to P˜1.5GPa on ρ(T), Tc, and the Hall number pH≡RH-1 for x= 0.3%, 0.8%, and 1.3%. Tc is reduced sharply with <span class="hlt">pressure</span>, dTc/dP=400-500mK/GPa as the low temperature Kondo- like upturn in ρ(T) is weakened. Also, dA/dP<0 and dpH/dP>0. These <span class="hlt">observations</span> are discussed in the context of the proposed charge-Kondo model for Pb1-xTlxTe. [1] Y. Matsushita, H. Bluhm, T.H. Geballe and I.R. Fisher, Phys.Rev.Lett. 94, 157002(2005).[2] M. Dzero and J. Schmalian, Phys.Rev.Lett. 94, 157003 (2005). This work is supported by NSF frant DMR-0520552.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMMR31C..03F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR31C..03F"><span>Pore fluid <span class="hlt">pressure</span> and the seismic cycle</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>French, M. E.; Zhu, W.; Hirth, G.; Belzer, B.</p> <p>2017-12-01</p> <p>In the brittle crust, the critical shear stress required for fault slip decreases with increasing pore fluid <span class="hlt">pressures</span> according to the effective stress criterion. As a result, higher pore fluid <span class="hlt">pressures</span> are thought to promote fault slip and seismogenesis, consistent with <span class="hlt">observations</span> that increasing fluid <span class="hlt">pressure</span> as a result of wastewater injection is correlated with increased seismicity. On the other hand, elevated pore fluid <span class="hlt">pressure</span> is also proposed to promote slow stable failure rather than seismicity along some fault zones, including during slow slip in subduction zones. Here we review recent experimental evidence for the roles that pore fluid <span class="hlt">pressure</span> and the effective stress play in controlling fault slip behavior. Using two sets of experiments on serpentine fault gouge, we show that increasing fluid <span class="hlt">pressure</span> does decrease the shear stress for reactivation under brittle conditions. However, under semi-brittle conditions as expected near the base of the seismogenic zone, high pore fluid <span class="hlt">pressures</span> are much less effective at reducing the shear stress of reactivation even though deformation is localized and frictional. We use an additional study on serpentinite to show that cohesive fault rocks, potentially the product of healing and cementation, experience an increase in fracture energy during faulting as fluid <span class="hlt">pressures</span> approach lithostatic, which can lead to more stable failure. Structural <span class="hlt">observations</span> show that the increased fracture energy is associated with a greater intensity of transgranular fracturing and delocalization of deformation. Experiments on several lithologies indicate that the stabilizing effect of fluid <span class="hlt">pressure</span> occurs independent of rock composition and hydraulic properties. Thus, high pore fluid <span class="hlt">pressures</span> have the potential to either enhance seismicity or promote stable faulting <span class="hlt">depending</span> on <span class="hlt">pressure</span>, temperature, and fluid <span class="hlt">pressure</span> conditions. Together, the results of these studies indicate that pore fluid <span class="hlt">pressure</span> promotes</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1064919-pressure-dependence-oxygen-isotope-exchange-rates-between-solution-apical-oxygens-uo2-oh-ion','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1064919-pressure-dependence-oxygen-isotope-exchange-rates-between-solution-apical-oxygens-uo2-oh-ion"><span>The <span class="hlt">pressure</span> <span class="hlt">dependence</span> of oxygen-isotope-exchange rates between solution and apical oxygens on the UO 2(OH) 4 2- ion</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>Harley, Steven J.; Ohlin, C. Andre; Johnson, Rene L.</p> <p>2011-04-06</p> <p>The <span class="hlt">pressure</span> <span class="hlt">dependence</span> of isotope exchange rate was determined for apical oxygen atoms in the UO 2(OH) 4 2-(aq) ion. The results can be interpreted to indicate an associative character of the reaction.</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 gradient-<span class="hlt">dependent</span> 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 gradients 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 <span class="hlt">observed</span> 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> </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('http://adsabs.harvard.edu/abs/2009PhDT.......105W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009PhDT.......105W"><span><span class="hlt">Pressure</span> broadening and <span class="hlt">pressure</span> shift of diatomic iodine at 675 nm</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wolf, Erich N.</p> <p></p> <p>Doppler-limited, steady-state, linear absorption spectra of 127 I2 (diatomic iodine) near 675 nm were recorded with an internally-referenced wavelength modulation spectrometer, built around a free-running diode laser using phase-sensitive detection, and capable of exceeding the signal-to-noise limit imposed by the 12-bit data acquisition system. <span class="hlt">Observed</span> I2 lines were accounted for by published spectroscopic constants. <span class="hlt">Pressure</span> broadening and <span class="hlt">pressure</span> shift coefficients were determined respectively from the line-widths and line-center shifts as a function of buffer gas <span class="hlt">pressure</span>, which were determined from nonlinear regression analysis of <span class="hlt">observed</span> line shapes against a Gaussian-Lorentzian convolution line shape model. This model included a linear superposition of the I2 hyperfine structure based on changes in the nuclear electric quadrupole coupling constant. Room temperature (292 K) values of these coefficients were determined for six unblended I 2 lines in the region 14,817.95 to 14,819.45 cm-1 for each of the following buffer gases: the atoms He, Ne, Ar, Kr, and Xe; and the molecules H2, D2, N2, CO2, N2O, air, and H2O. These coefficients were also determined at one additional temperature (388 K) for He and CO2, and at two additional temperatures (348 and 388 K) for Ar. Elastic collision cross-sections were determined for all <span class="hlt">pressure</span> broadening coefficients in this region. Room temperature values of these coefficients were also determined for several low-J I2 lines in the region 14,946.17 to 14,850.29 cm-1 for Ar. A line shape model, obtained from a first-order perturbation solution of the time-<span class="hlt">dependent</span> Schrodinger equation for randomly occurring interactions between a two-level system and a buffer gas treated as step-function potentials, reveals a relationship between the ratio of <span class="hlt">pressure</span> broadening to <span class="hlt">pressure</span> shift coefficients and a change in the wave function phase-factor, interpreted as reflecting the "cause and effect" of state-changing events in the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19582884','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19582884"><span>Investigating the potential of Bacillus subtilis alpha-amylase as a <span class="hlt">pressure</span>-temperature-time indicator for high hydrostatic <span class="hlt">pressure</span> pasteurization processes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Grauwet, Tara; Van der Plancken, Iesel; Vervoort, Liesbeth; Hendrickx, Marc E; Van Loey, Ann</p> <p>2009-01-01</p> <p>The potential of Bacillus subtilis alpha-amylase (BSA) as a <span class="hlt">pressure</span>-temperature-time indicator (pTTI) for high <span class="hlt">pressure</span> pasteurization processing (400-600 MPa; T(i) 10-40 degrees C; 1-15 min) was investigated. A stepwise approach was followed for the development of an enzyme-based, extrinsic, isolated pTTI. First, based on literature data on the <span class="hlt">pressure</span> stability, BSA was selected as a candidate indicator. Next to the accuracy and ease of the measurement of the indicator's response (residual activity) to the <span class="hlt">pressure</span> treatment, the storage and handling stability of BSA at atmospheric <span class="hlt">pressure</span> was verified. Second, the stability of BSA at a constant temperature (T) and time in function of <span class="hlt">pressure</span> (p) was investigated. Solvent engineering was used to shift the inactivation window of BSA in the processing range of interest. Third, the enzyme (1 g/L BSA-MES 0.05 M pH 5.0) was kinetically calibrated under isobaric-isothermal conditions. Time <span class="hlt">dependent</span> changes in activity could be modeled best by a first-order model. Except for low <span class="hlt">pressures</span> and high temperatures, a synergistic effect between <span class="hlt">pressure</span> and temperature could be <span class="hlt">observed</span>. Based on the model selected to describe the combined p,T-<span class="hlt">dependency</span> of the inactivation rate constant, an elliptically shaped isorate contour plot could be constructed, illustrating the processing range where BSA can be used to demonstrate temperature gradients. Fourth, the validity of the kinetic model was tested successfully under dynamic conditions similar to those used in food industry. Finally, the indicator was found suitable to demonstrate nonuniformity in two-sectional planes of a vertical, single vessel system. (c) 2009 American Institute of Chemical Engineers. Biotechnol. Prog., 2009.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70024035','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70024035"><span>Experimental <span class="hlt">observations</span> of <span class="hlt">pressure</span> oscillations and flow regimes in an analogue volcanic 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>Lane, S.J.; Chouet, B.A.; Phillips, J.C.; Dawson, P.; Ryan, G.A.; Hurst, E.</p> <p>2001-01-01</p> <p>Gas-liquid flows, designed to be analogous to those in volcanic conduits, are generated in the laboratory using organic gas-gum rosin mixtures expanding in a vertically mounted tube. The expanding fluid shows a range of both flow and <span class="hlt">pressure</span> oscillation behaviors. Weakly supersaturated source liquids produce a low Reynolds number flow with foam expanding from the top surface of a liquid that exhibits zero fluid velocity at the tube wall; i.e., the conventional "no-slip" boundary condition. <span class="hlt">Pressure</span> oscillations, often with strong long-period characteristics and consistent with longitudinal and radial resonant oscillation modes, are detected in these fluids. Strongly supersaturated source liquids generate more energetic flows that display a number of flow regimes. These regimes include a static liquid source, viscous flow, detached flow (comprising gas-pockets-at-wall and foam-in-gas annular flow, therefore demonstrating strong radial heterogeneity), and a fully turbulent transonic fragmented or mist flow. Each of these flow regimes displays characteristic <span class="hlt">pressure</span> oscillations that can be related to resonance of flow features or wall impact phenomena. The <span class="hlt">pressure</span> oscillations are produced by the degassing processes without the need of elastic coupling to the confining medium or flow restrictors and valvelike features. The oscillatory behavior of the experimental flows is compared to seismoacoustic data from a range of volcanoes where resonant oscillation of the fluid within the conduit is also often invoked as controlling the <span class="hlt">observed</span> oscillation frequencies. On the basis of the experimental data we postulate on the nature of seismic signals that may be measured during large-scale explosive activity. Copyright 2001 by the American Geophysical Union.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/20713948-pressure-temperature-dependence-shear-modulus-yield-strength-aluminum-copper-tungsten-under-shock-compression','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/20713948-pressure-temperature-dependence-shear-modulus-yield-strength-aluminum-copper-tungsten-under-shock-compression"><span><span class="hlt">Pressure</span> and temperature <span class="hlt">dependence</span> of shear modulus and yield strength for aluminum, copper, and tungsten under shock compression</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>Peng Jianxiang; Jing Fuqian; Li Dahong</p> <p>2005-07-01</p> <p>Experimental data for the shear modulus and yield strength of shocked aluminum, copper, and tungsten were systematically analyzed. Comparisons between these data and calculations using the Steinberg-Cochran-Guinan (SCG) constitutive model [D. J. Steinberg, S. G. Cochran, and M. W. Guinan, J. Appl. Phys. 51, 1498 (1980)] indicate that the yield strength has the same <span class="hlt">dependence</span> on <span class="hlt">pressure</span> and temperature as the shear modulus for aluminum for shock <span class="hlt">pressures</span> up to 50 GPa, for copper to 100 GPa, and for tungsten to 200 GPa. Therefore, the assumption of Y{sub p}{sup '}/Y{sub 0}=G{sub p}{sup '}/G{sub 0},Y{sub T}{sup '}/Y{sub 0}=G{sub T}{sup '}/G{sub 0}more » is basically acceptable for these materials, and the SCG model can be used to describe the shear modulus and yield strength of the shocked material at high <span class="hlt">pressure</span> and temperature.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2269608','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2269608"><span>Subatmospheric <span class="hlt">pressure</span> in the rabbit pleural lymphatic network</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Negrini, Daniela; Del Fabbro, Massimo</p> <p>1999-01-01</p> <p>Hydraulic <span class="hlt">pressure</span> in intercostal and diaphragmatic lymphatic vessels was measured through the micropuncture technique in 23 anaesthetised paralysed rabbits. Pleural lymphatic vessels with diameters ranging from 55 to 950 μm were <span class="hlt">observed</span> under stereomicroscope view about 3–4 h after intrapleural injection of 20 % fluorescent dextrans. Lymphatic <span class="hlt">pressure</span> oscillated from a minimum (Pmin) to a maximum (Pmax) value, reflecting oscillations in phase with cardiac activity (cardiogenic oscillations) and lymphatic myogenic activity. With intact pleural space, Pmin in submesothelial diaphragmatic lymphatic vessels of the lateral apposition zone was −9.1 ± 4.2 mmHg, more subatmospheric than the simultaneously recorded pleural liquid <span class="hlt">pressure</span> amounting to −3.9 ± 1.2 mmHg. In extrapleural intercostal lymphatic vessels Pmin averaged −1.3 ± 2.7 mmHg. Cardiogenic <span class="hlt">pressure</span> oscillations (Pmax−Pmin), were <span class="hlt">observed</span> in all recordings; their mean amplitude was about 5 mmHg and was not <span class="hlt">dependent</span> upon frequency of cardiac contraction, nor lymphatic vessel diameter, nor the Pmin value. Intrinsic contractions of lymphatic vessel walls caused spontaneous <span class="hlt">pressure</span> waves of about 7 mmHg in amplitude at a rate of 8 cycles min−1. These results demonstrated the ability of pleural lymphatic vessels to generate <span class="hlt">pressure</span> oscillations driving fluid from the subatmospheric pleural space into the lymphatic network. PMID:10545142</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhyC..548...61A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhyC..548...61A"><span><span class="hlt">Pressure</span> <span class="hlt">dependence</span> of effective Coulomb interaction parameters in BaFe2As2 by first-principle calculation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aghajani, M.; Hadipour, H.; Akhavan, M.</p> <p>2018-05-01</p> <p><span class="hlt">Pressure</span> <span class="hlt">dependence</span> of the onsite Coulomb interactions of the BaFe2As2 has been studied by employing the constrained random phase approximation within first-principle calculations. Analyzing total and projected density of states, a pseudogap is found for dxy band at the energy roughly 0.25 eV higher than the Fermi level. Also, by applying <span class="hlt">pressure</span> the spectral weight of the dxy orbital vanishes while other orbitals remain metallic. The different screening channels, as discussed in four different models, affect significantly on the Hubbard U while the Hund J remains almost unchanged. The average onsite bare and partially and fully screened Coulomb interactions increase with different rates upon compression. These different rates can be explained by competition between the electronic screening and reduction of bond lengths.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015IAUGA..2258213C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015IAUGA..2258213C"><span>Jellyfish: <span class="hlt">Observational</span> Properties of Extreme Ram-<span class="hlt">Pressure</span> Stripping Events in Massive Galaxy Clusters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Conor, McPartland; Ebeling, Harald; Roediger, Elke</p> <p>2015-08-01</p> <p>We investigate the physical origin and <span class="hlt">observational</span> signatures of extreme ram-<span class="hlt">pressure</span> stripping (RPS) in 63 massive galaxy clusters at z=0.3-0.7, based on data in the F606W passband obtained with the Advanced Camera for Surveys aboard the Hubble Space Telescope. Using a training set of a dozen ``jellyfish" galaxies identified earlier in the same imaging data, we define quantitative morphological criteria to select candidate galaxies which are similar to known cases of RPS. Considering a sample of 16 ``jellyfish" galaxies (10 of which we present for the first time), we visually derive estimates of the projected direction of motion based on dynamical features such as apparent compression shocks and debris trails. Our findings suggest that the <span class="hlt">observed</span> events occur primarily at large distances from the cluster core and involve infall trajectories featuring high impact parameters. Simple models of cluster growth show that such trajectories are consistent with two scenarios: 1) galaxy infall along filaments; and 2) infall at high velocities (≥1000 km/s) characteristic of cluster mergers. The <span class="hlt">observed</span> distribution of events is best described by timescales of ˜few Myr in agreement with recent numerical simulations of RPS. The broader areal coverage of the Hubble Frontier Fields should provide an even larger sample of RPS events to determine the relative contributions of infall and cluster mergers. Prompted by the discovery of several jellyfish galaxies whose brightness in the F606W passband rivals or exceeds that of the respective brightest cluster galaxy, we attempt to constrain the luminosity function of galaxies undergoing RPS. The <span class="hlt">observed</span> significant excess at the bright end compared to the luminosity functions of blue cluster members strongly suggests enhanced star formation, thus challenging theoretical and numerical studies according to which RPS merely displaces existing star-forming regions. In-depth studies of individual objects will help test our</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22502549','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22502549"><span>High-<span class="hlt">pressure</span> effect on the dynamics of solvated peptides.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nellas, Ricky B; Glover, Mary M; Hamelberg, Donald; Shen, Tongye</p> <p>2012-04-14</p> <p>The dynamics of peptides has a direct connection to how quickly proteins can alter their conformations. The speed of exploring the free energy landscape <span class="hlt">depend</span> on many factors, including the physical parameters of the environment, such as <span class="hlt">pressure</span> and temperature. We performed a series of molecular dynamics simulations to investigate the <span class="hlt">pressure</span>-temperature effects on peptide dynamics, especially on the torsional angle and peptide-water hydrogen bonding (H-bonding) dynamics. Here, we show that the dynamics of the omega angle and the H-bonding dynamics between water and the peptide are affected by <span class="hlt">pressure</span>. At high temperature (500 K), both the dynamics of the torsional angle ω and H-bonding slow down significantly with increasing <span class="hlt">pressure</span>, interestingly, at approximately the same rate. However, at a lower temperature of 300 K, the <span class="hlt">observed</span> trend on H-bonding dynamics as a function of <span class="hlt">pressure</span> reverses, i.e., higher <span class="hlt">pressure</span> speeds up H-bonding dynamics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12481804','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12481804"><span>Water cycles in closed ecological systems: effects of atmospheric <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>Rygalov, Vadim Y; Fowler, Philip A; Metz, Joannah M; Wheeler, Raymond M; Bucklin, Ray A</p> <p>2002-01-01</p> <p>In bioregenerative life support systems that use plants to generate food and oxygen, the largest mass flux between the plants and their surrounding environment will be water. This water cycle is a consequence of the continuous change of state (evaporation-condensation) from liquid to gas through the process of transpiration and the need to transfer heat (cool) and dehumidify the plant growth chamber. Evapotranspiration rates for full plant canopies can range from ~1 to 10 L m-2 d-1 (~1 to 10 mm m-2 d-1), with the rates <span class="hlt">depending</span> primarily on the vapor <span class="hlt">pressure</span> deficit (VPD) between the leaves and the air inside the plant growth chamber. VPD in turn is <span class="hlt">dependent</span> on the air temperature, leaf temperature, and current value of relative humidity (RH). Concepts for developing closed plant growth systems, such as greenhouses for Mars, have been discussed for many years and the feasibility of such systems will <span class="hlt">depend</span> on the overall system costs and reliability. One approach for reducing system costs would be to reduce the operating <span class="hlt">pressure</span> within the greenhouse to reduce structural mass and gas leakage. But managing plant growth environments at low <span class="hlt">pressures</span> (e.g., controlling humidity and heat exchange) may be difficult, and the effects of low-<span class="hlt">pressure</span> environments on plant growth and system water cycling need further study. We present experimental evidence to show that water saturation <span class="hlt">pressures</span> in air under isothermal conditions are only slightly affected by total <span class="hlt">pressure</span>, but the overall water flux from evaporating surfaces can increase as <span class="hlt">pressure</span> decreases. Mathematical models describing these <span class="hlt">observations</span> are presented, along with discussion of the importance for considering "water cycles" in closed bioregenerative life support systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040087943&hterms=water+gas+exchange&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dwater%2Bgas%2Bexchange','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040087943&hterms=water+gas+exchange&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dwater%2Bgas%2Bexchange"><span>Water cycles in closed ecological systems: effects of atmospheric <span class="hlt">pressure</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rygalov, Vadim Y.; Fowler, Philip A.; Metz, Joannah M.; Wheeler, Raymond M.; Bucklin, Ray A.; Sager, J. C. (Principal Investigator)</p> <p>2002-01-01</p> <p>In bioregenerative life support systems that use plants to generate food and oxygen, the largest mass flux between the plants and their surrounding environment will be water. This water cycle is a consequence of the continuous change of state (evaporation-condensation) from liquid to gas through the process of transpiration and the need to transfer heat (cool) and dehumidify the plant growth chamber. Evapotranspiration rates for full plant canopies can range from 1 to 10 L m-2 d-1 (1 to 10 mm m-2 d-1), with the rates <span class="hlt">depending</span> primarily on the vapor <span class="hlt">pressure</span> deficit (VPD) between the leaves and the air inside the plant growth chamber. VPD in turn is <span class="hlt">dependent</span> on the air temperature, leaf temperature, and current value of relative humidity (RH). Concepts for developing closed plant growth systems, such as greenhouses for Mars, have been discussed for many years and the feasibility of such systems will <span class="hlt">depend</span> on the overall system costs and reliability. One approach for reducing system costs would be to reduce the operating <span class="hlt">pressure</span> within the greenhouse to reduce structural mass and gas leakage. But managing plant growth environments at low <span class="hlt">pressures</span> (e.g., controlling humidity and heat exchange) may be difficult, and the effects of low-<span class="hlt">pressure</span> environments on plant growth and system water cycling need further study. We present experimental evidence to show that water saturation <span class="hlt">pressures</span> in air under isothermal conditions are only slightly affected by total <span class="hlt">pressure</span>, but the overall water flux from evaporating surfaces can increase as <span class="hlt">pressure</span> decreases. Mathematical models describing these <span class="hlt">observations</span> are presented, along with discussion of the importance for considering "water cycles" in closed bioregenerative life support systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28699802','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28699802"><span>Positive correlation between blood <span class="hlt">pressure</span> or heart rate and chymase-<span class="hlt">dependent</span> angiotensin II-forming activity in circulating mononuclear leukocytes measured by new ELISA.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Okamura, Keisuke; Okuda, Tetsu; Shirai, Kazuyuki; Urata, Hidenori</p> <p>2018-01-01</p> <p>The aim of the present study was to establish a convenient clinically applicable assay method for chymase-<span class="hlt">dependent</span> angiotensin II forming activity of circulating mononuclear leukocytes (CML), which was potentially a marker of tissue chymase activity. Using this method, association between CML chymase activity and clinical parameters was determined. Cardiovascular outpatients (n = 170) without taking antihypertensive medication were recruited. An ELISA for chymase-<span class="hlt">dependent</span> angiotensin II-forming activity in CML was established using Nma /Dnp-modified angiotensin I. Logistic regression analysis revealed that age and male gender were significant independent determinants of the increased CML chymase activity. After adjustment by age and gender, the CML chymase activity was positively correlated with systolic blood <span class="hlt">pressure</span>, pulse rate, and the brain natriuretic peptide level. The relation between blood <span class="hlt">pressure</span> and CML chymase activity suggests that it might reflect that increased tissue chymase activity contributes to systemic high blood <span class="hlt">pressure</span> and heart rate because plasma chymase is inactive due to inhibitory plasma inhibitors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20059898','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20059898"><span>Casein micelle dissociation in skim milk during high-<span class="hlt">pressure</span> treatment: effects of <span class="hlt">pressure</span>, pH, and temperature.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Orlien, V; Boserup, L; Olsen, K</p> <p>2010-01-01</p> <p>The effect of pH (from 5.5 to 7.5) and temperature (from 5 to 40 degrees C) on the turbidity of reconstituted skim milk powder was investigated at ambient <span class="hlt">pressure</span> and in situ under <span class="hlt">pressure</span> (up to 500MPa) by measurement of light scattering. High-<span class="hlt">pressure</span> treatment reduced the turbidity of milk for all combinations of pH and temperature due to micelle dissociation. The turbidity profiles had a characteristic sigmoidal shape in which almost no effect on turbidity was <span class="hlt">observed</span> at low <span class="hlt">pressures</span> (100MPa), followed by a stronger <span class="hlt">pressure</span> <span class="hlt">dependency</span> over a <span class="hlt">pressure</span> range of 150MPa during which turbidity decreased extremely. From the turbidity profiles, the threshold <span class="hlt">pressure</span> for disruption of micelle integrity was determined and ranged from 150MPa at low pH to 350-400MPa at high pH. The threshold <span class="hlt">pressure</span> diagram clearly showed a relationship between the barostability of casein micelles and pH, whereas almost no effect of temperature was shown. This remarkable pH effect was a consequence of <span class="hlt">pressure</span>-induced changes in the electrostatic interactions between colloidal calcium phosphate and the caseins responsible for maintaining micellar structure and was explained by a shift in the calcium phosphate balance in the micelle-serum system. Accordingly, a mechanism for high <span class="hlt">pressure</span>-induced disruption of micelle integrity is suggested in which the state of calcium plays a crucial role in the micelle dissociation process. Copyright 2010 American Dairy Science Association. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19830016164','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19830016164"><span><span class="hlt">Observations</span> of magnetic fields on solar-type stars</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Marcy, G. W.</p> <p>1982-01-01</p> <p>Magnetic-field <span class="hlt">observations</span> were carried out for 29 G and K main-sequence stars. The area covering-factors of magnetic regions tends to be greater in the K dwarfs than in the G dwarfs. However, no spectral-type <span class="hlt">dependence</span> is found for the field strengths, contrary to predictions that <span class="hlt">pressure</span> equilibrium with the ambient photospheric gas <span class="hlt">pressure</span> would determine the surface field strengths. Coronal soft X-ray fluxes from the G and K dwarfs correlate well with the fraction of the stellar surface covered by magnetic regions. The <span class="hlt">dependence</span> of coronal soft X-ray fluxes on photospheric field strengths is consistent with Stein's predicted generation-rates for Alfven waves. These <span class="hlt">dependences</span> are inconsistent with the one dynamo model for which a specific prediction is offered. Finally, time variability of magnetic fields is seen on the two active stars that have been extensively monitored. Significant changes in magnetic fields are seen to occur on timescales as short as one day.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3985862','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3985862"><span><span class="hlt">Observation</span> of Complete <span class="hlt">Pressure</span>-Jump Protein Refolding in Molecular Dynamics Simulation and Experiment</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>2015-01-01</p> <p>Density is an easily adjusted variable in molecular dynamics (MD) simulations. Thus, <span class="hlt">pressure</span>-jump (P-jump)-induced protein refolding, if it could be made fast enough, would be ideally suited for comparison with MD. Although <span class="hlt">pressure</span> denaturation perturbs secondary structure less than temperature denaturation, protein refolding after a fast P-jump is not necessarily faster than that after a temperature jump. Recent P-jump refolding experiments on the helix bundle λ-repressor have shown evidence of a <3 μs burst phase, but also of a ∼1.5 ms “slow” phase of refolding, attributed to non-native helical structure frustrating microsecond refolding. Here we show that a λ-repressor mutant is nonetheless capable of refolding in a single explicit solvent MD trajectory in about 19 μs, indicating that the burst phase <span class="hlt">observed</span> in experiments on the same mutant could produce native protein. The simulation reveals that after about 18.5 μs of conformational sampling, the productive structural rearrangement to the native state does not occur in a single swift step but is spread out over a brief series of helix and loop rearrangements that take about 0.9 μs. Our results support the molecular time scale inferred for λ-repressor from near-downhill folding experiments, where transition-state population can be seen experimentally, and also agrees with the transition-state transit time <span class="hlt">observed</span> in slower folding proteins by single-molecule spectroscopy. PMID:24437525</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29671421','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29671421"><span>Voltage and partial <span class="hlt">pressure</span> <span class="hlt">dependent</span> defect chemistry in (La,Sr)FeO3-δ thin films investigated by chemical capacitance measurements.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Schmid, Alexander; Rupp, Ghislain M; Fleig, Jürgen</p> <p>2018-05-03</p> <p>La0.6Sr0.4FeO3-δ (LSF) thin films of different thickness were prepared by pulsed laser deposition on yttria stabilized zirconia (YSZ) and characterized by using three electrode impedance spectroscopy. Electrochemical film capacitance was analyzed in relation to oxygen partial <span class="hlt">pressure</span> (0.25 mbar to 1 bar), DC polarization (0 m to -600 m) and temperature (500 to 650 °C). For most measurement parameters, the chemical bulk capacitance dominates the overall capacitive properties and the corresponding defect chemical state <span class="hlt">depends</span> solely on the oxygen chemical potential inside the film, independent of atmospheric oxygen <span class="hlt">pressure</span> and DC polarization. Thus, defect chemical properties (defect concentrations and defect formation enthalpies) could be deduced from such measurements. Comparison with LSF defect chemical bulk data from the literature showed good agreement for vacancy formation energies but suggested larger electronic defect concentrations in the films. From thickness-<span class="hlt">dependent</span> measurements at lower oxygen chemical potentials, an additional capacitive contribution could be identified and attributed to the LSF|YSZ interface. Deviations from simple chemical capacitance models at high <span class="hlt">pressures</span> are most probably due to defect interactions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.S44B..07G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.S44B..07G"><span>Slow slip pulses driven by thermal <span class="hlt">pressurization</span> of pore fluid: theory and <span class="hlt">observational</span> constraints</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Garagash, D.</p> <p>2012-12-01</p> <p>We discuss recently developed solutions for steadily propagating self-healing slip pulses driven by thermal <span class="hlt">pressurization</span> (TP) of pore fluid [Garagash, 2012] on a fault with a constant sliding friction. These pulses are characterized by initial stage of undrained weakening of the fault (when fluid/heat can not yet escape the frictionally heated shear zone), which gives way to partial restrengthening due to increasing hydrothermal diffusion under conditions of diminished rate of heating, leading to eventual locking of the slip. The rupture speed of these pulses is decreasing function of the thickness (h) of the principal shear zone. We find that "thick" shear zones, h >> hdyna, where hdyna = (μ/τ0) (ρc/fΛ)(4α/cs), can support aseismic TP pulses propagating at a fraction hdyna/h of the shear wave speed cs, while "thin" shear zones, h˜hdyna or thinner, can only harbor seismic slip. (Here μ - shear modulus, τ0 - the nominal fault strength, f - sliding friction, ρc - the heat capacity of the fault gouge, Λ - the fluid thermal <span class="hlt">pressurization</span> factor, α - hydrothermal diffusivity parameter of the gouge). For plausible range of fault parameters, hdyna is between 10s to 100s of micrometers, suggesting that slow slip transients propagating at 1 to 10 km/day may occur in the form of a TP slip pulse accommodated by a meter-thick shear zone. We verify that this is, indeed, a possibility by contrasting the predictions for aseismic, small-slip TP pulses operating at seismologically-constrained, near-lithostatic pore <span class="hlt">pressure</span> (effective normal stress ≈ 3 to 10 MPa) with the <span class="hlt">observations</span> (slip duration at a given fault location ≈ week, propagation speed ≈ 15 km/day, and the inferred total slip ≈ 2 to 3 cm) for along-strike propagation of the North Cascadia slow slip events of '98-99 [Dragert et al., 2001, 2004]. Furthermore, we show that the effect of thermal <span class="hlt">pressurization</span> on the strength of the subduction interface is comparable to or exceeds that of the rate-<span class="hlt">dependence</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009EGUGA..1112325S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009EGUGA..1112325S"><span>Elasticity of MgSiO3 glass to <span class="hlt">pressures</span> of the transition zone</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Speziale, S.; Reichmann, H. J.; Marquardt, H.; Shim, S.-H.</p> <p>2009-04-01</p> <p>Geophysical <span class="hlt">observations</span> suggest the presence of liquid silicates in regions at the top of the transition zone and at the core-mantle boundary. In addition, a mainly silicate magma ocean probably played a crucial role in the evolution of the early Earth. For these reasons understanding the physical behavior of silicates melts at high <span class="hlt">pressures</span> is important. In situ experimental investigation of the physical properties of silicate melts at high <span class="hlt">pressures</span> poses substantial technical difficulties, and computer simulations are nowadays the most effective method to explore the elasticity and the density of such material at relevant conditions of the deep Earth. Due to these difficulties, glasses are often used as "frozen" proxies of melts for experimental studies of their physical properties. Here we present the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of sound velocity of MgSiO3 glass measured by Brillouin spectroscopy in the diamond-anvil cell across the whole <span class="hlt">pressure</span> range of the upper mantle and transition zone. We measured both compressional and shear velocity at 36 different <span class="hlt">pressures</span> both on compression and decompression. Fixing the starting density to 2.742 ± 0.003 g/cm3, we determined both bulk modulus KS0 and shear modulus G0, and their <span class="hlt">pressure</span> derivatives at ambient conditions to be KS0 = 76.2 ± 1.0 GPa, G0 = 40.11 ± 0.32 GPa, (‚KS/‚P)0 = 3.04 ± 0.23, and (‚G/‚P )0 = 0.46 ± 0.06. We <span class="hlt">observe</span> two discontinuities of the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of both compressional and shear velocity at 7 ± 2 GPa and at 21 ± 1 GPa. These two discontinuities take place at <span class="hlt">pressures</span> at which: (a) changes in the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of both Si-O-Si bending and Si-O stretching vibrations of the polymerized SiO4 network were <span class="hlt">observed</span> in the same glass by laser Raman scattering [1], and (b) new spectral features were <span class="hlt">observed</span> by X-ray Raman scattering [2].The velocities measured upon decompression are significantly different from those measured during compression. The whole of our velocity</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16375539','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16375539"><span><span class="hlt">Pressure</span> broadening and fine-structure-<span class="hlt">dependent</span> predissociation in oxygen B 3sigma(u)-, v = 0.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hannemann, Sandro; Wu, GuoRong; van Duijn, Eric-Jan; Ubachs, Wim; Cosby, Philip C</p> <p>2005-11-01</p> <p>Both laser-induced fluorescence and cavity ring-down spectral <span class="hlt">observations</span> were made in the Schumann-Runge band system of oxygen, using a novel-type ultranarrow deep-UV pulsed laser source. From measurements on the very weak (0,0) band <span class="hlt">pressure</span> broadening, <span class="hlt">pressure</span> shift, and predissociation line-broadening parameters were determined for the B 3sigma(u)-, v = 0,F(i) fine-structure components for various rotational levels in O2. The information content from these studies was combined with that of entirely independent measurements probing the much stronger (0,10), (0,19), and (0,20) Schumann-Runge bands involving preparation of vibrationally excited O2 molecules via photolysis of ozone. The investigations result in a consistent set of predissociation widths for the B 3sigma(u)-, v = 0 state of oxygen.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22606430-pressure-dependence-band-gap-phase-transitions-bulk-cux-cl-br','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22606430-pressure-dependence-band-gap-phase-transitions-bulk-cux-cl-br"><span><span class="hlt">Pressure</span> <span class="hlt">dependence</span> of band-gap and phase transitions in bulk CuX (X = Cl, Br, I)</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>Azhikodan, Dilna; Nautiyal, Tashi; Sharma, S.</p> <p>2016-05-06</p> <p>Usually a phase transition, in theoretical studies, is explored or verified by studying the total energy as a function of the volume considering various plausible phases. The intersection point, if any, of the free energy vs. volume curves for the different phases is then the indicator of the phase transition(s). The question is, can the theoretical study of a single phase alone indicate a phase transition? i.e. can we look beyond the phase under consideration through such a study? Using density-functional theory, we report a novel approach to suggest phase transition(s) through theoretical study of a single phase. Copper halidesmore » have been engaged for this study. These are direct band-gap semiconductors, with zinc blende structure at ambient conditions, and are reported to exhibit many phase transitions. We show that the study of volume <span class="hlt">dependence</span> of energy band-gap in a single phase facilitates looking beyond the phase under consideration. This, when translated to <span class="hlt">pressures</span>, reflects the phase transition <span class="hlt">pressures</span> for CuX (X = Cl, Br, I) with an encouraging accuracy. This work thus offers a simple, yet reliable, approach based on electronic structure calculations to investigate new semiconducting materials for phase changes under <span class="hlt">pressure</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28904452','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28904452"><span>Long-term Response of Cerebrospinal Fluid <span class="hlt">Pressure</span> in Patients with Idiopathic Intracranial Hypertension - A Prospective <span class="hlt">Observational</span> Study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gafoor, V Abdul; Smita, B; Jose, James</p> <p>2017-01-01</p> <p>Idiopathic intracranial hypertension (IIH) is increased intracranial <span class="hlt">pressure</span> (ICP) with normal cerebrospinal fluid (CSF) contents, in the absence of an intracranial mass, hydrocephalus, or other identifiable causes. The current knowledge of the treatment outcome of IIH is limited, and the data on the natural history of this entity are scant. The objective of the study is to study the treatment response of IIH by serially measuring the CSF opening <span class="hlt">pressure</span> and to delineate the factors influencing the same. A prospective <span class="hlt">observational</span> study in a cohort of fifty patients with IIH in whom CSF opening <span class="hlt">pressure</span> was serially measured at pre-specified intervals. The mean CSF opening <span class="hlt">pressure</span> at baseline was 302.4 ± 51.69 mm of H 2 O (range: 220-410). Even though a higher body mass index (BMI) showed a trend toward a higher CSF opening <span class="hlt">pressure</span>, the association was not significant ( P = 0.168). However, the age of the patient had a significant negative correlation with the CSF <span class="hlt">pressure</span> ( P = 0.006). The maximum reduction in CSF <span class="hlt">pressure</span> occurred in the first 3 months of treatment, and thereafter it plateaued. Remission was attained in 12 (24%) patients. BMI had the strongest association with remission ( P = 0.001). In patients with IIH, treatment response is strongly related to BMI. However, patients with normal BMI are also shown to relapse and hence should have continuous, long-term follow-up. The reduction in CSF <span class="hlt">pressure</span> attained in the first 3 months could reflect the long-term response to treatment.</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('https://www.osti.gov/biblio/614998-dx-center-transformation-te-donors-gasb-under-hydrostatic-pressure','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/614998-dx-center-transformation-te-donors-gasb-under-hydrostatic-pressure"><span>DX-center transformation of Te donors in GaSb under hydrostatic <span class="hlt">pressure</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>Navarro-Contreras, H.; de Anda-Salazar, F.; Hsu, L.</p> <p>1998-05-01</p> <p>We have <span class="hlt">observed</span> the transformation of Te shallow donors in GaSb into DX centers at hydrostatic <span class="hlt">pressures</span> of 27.8{plus_minus}2.6kbar. The position of the Te DX energy level at zero <span class="hlt">pressure</span> is calculated to lie 300{plus_minus}70meV above the conduction band at atmospheric <span class="hlt">pressure</span>, consistent with the theory that in the III-V compounds the DX centers line up in energy with respect to the vacuum level within experimental error. This binding energy at zero <span class="hlt">pressure</span> of the Te DX compares well with the value of 210 meV calculated from the cation-cation bonded DX-center model recently proposed by Park and Chadi. At pressuresmore » where the Te shallow donor into DX-center transformation has taken place we <span class="hlt">observe</span> evidence of the existence of a bound phonon associated with the Te DX center. From its <span class="hlt">observed</span> <span class="hlt">pressure</span> <span class="hlt">dependence</span> the LO optical phonon Gr{umlt u}neisen parameter is calculated to be {gamma}{sub LO}=0.93{plus_minus}0.09. {copyright} {ital 1998} {ital The American Physical Society}« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1415561-pressure-dependence-ce-valence-cerhin5','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1415561-pressure-dependence-ce-valence-cerhin5"><span><span class="hlt">Pressure</span> <span class="hlt">dependence</span> of Ce valence in CeRhIn 5</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Brubaker, Z. E.; Stillwell, R. L.; Chow, P.; ...</p> <p>2017-12-14</p> <p>We have studied the Ce valence as a function of <span class="hlt">pressure</span> in CeRhIn5 at 300 K and at 22 K using x-ray absorption spectroscopy in partial fluorescent yield mode. At room temperature, we found no detectable change in Ce valence greater than 0.01 up to a <span class="hlt">pressure</span> of 5.5 GPa. At 22 K, the valence remains robust against <span class="hlt">pressure</span> below 6 GPa, in contrast to the predicted valence crossover at P = 2.35 GPa. In conclusion, this work yields an upper limit for the change in Ce-valence and suggests that the critical valence fluctuation scenario, in its current form, ismore » unlikely.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21443013-observability-radiation-pressure-shot-noise-optomechanical-systems','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21443013-observability-radiation-pressure-shot-noise-optomechanical-systems"><span><span class="hlt">Observability</span> of radiation-<span class="hlt">pressure</span> shot noise in optomechanical systems</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>Boerkje, K.; Nunnenkamp, A.; Zwickl, B. M.</p> <p>2010-07-15</p> <p>We present a theoretical study of an experiment designed to detect radiation-<span class="hlt">pressure</span> shot noise in an optomechanical system. Our model consists of a coherently driven optical cavity mode that is coupled to a mechanical oscillator. We examine the cross-correlation between two quadratures of the output field from the cavity. We determine under which circumstances radiation-<span class="hlt">pressure</span> shot noise can be detected by a measurement of this cross-correlation. This is done in the general case of nonzero detuning between the frequency of the drive and the cavity resonance frequency. We study the qualitative features of the different contributions to the cross-correlator andmore » provide quantitative figures of merit for the relative importance of the radiation-<span class="hlt">pressure</span> shot noise contribution to other contributions. We also propose a modified setup of this experiment relevant to the 'membrane-in-the-middle' geometry, which potentially can avoid the problems of static bistability and classical noise in the drive.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2143451','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2143451"><span>Experimentally <span class="hlt">observed</span> conformation-<span class="hlt">dependent</span> geometry and hidden strain in proteins.</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Karplus, P. A.</p> <p>1996-01-01</p> <p>A database has been compiled documenting the peptide conformations and geometries from 70 diverse proteins refined at 1.75 A or better. Analysis of the well-ordered residues within the database shows phi, psi-distributions that have more fine structure than is generally <span class="hlt">observed</span>. Also, clear evidence is presented that the peptide covalent geometry <span class="hlt">depends</span> on conformation, with the interpeptide N-C alpha-C bond angle varying by nearly +/-5 degrees from its standard value. The <span class="hlt">observed</span> deviations from standard peptide geometry are greatest near the edges of well-populated regions, consistent with strain occurring in these conformations. Minimization of such hidden strain could be an important factor in thermostability of proteins. These empirical data describing how equilibrium peptide geometry varies as a function of conformation confirm and extend quantum mechanics calculations, and have predictive value that will aid both theoretical and experimental analyses of protein structure. PMID:8819173</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JThSc..24...67Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JThSc..24...67Y"><span>Temperature and <span class="hlt">pressure</span> measurements at cold exit of counter-flow vortex tube with flow visualization of reversed flow</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yusof, Mohd Hazwan bin; Katanoda, Hiroshi; Morita, Hiromitsu</p> <p>2015-02-01</p> <p>In order to clarify the structure of the cold flow discharged from the counter-flow vortex tube (VT), the temperature and <span class="hlt">pressure</span> of the cold flow were measured, and the existence and behavior of the reversed flow at the cold exit was studied using a simple flow visualization technique consisting of a 0.75mm-diameter needle, and an oil paint droplet. It is <span class="hlt">observed</span> through this experiment that the Pitot <span class="hlt">pressure</span> at the cold exit center can either be lower or higher than atmospheric <span class="hlt">pressure</span>, <span class="hlt">depending</span> on the inlet <span class="hlt">pressure</span> and the cold fraction, and that a reversed flow is <span class="hlt">observed</span> when the Pitot <span class="hlt">pressure</span> at the cold exit center is lower than atmospheric <span class="hlt">pressure</span>. In addition, it is <span class="hlt">observed</span> that when reducing the cold fraction from unity at any arbitrary inlet <span class="hlt">pressure</span>, the region of reversed and colder flow in the central part of cold exit extends in the downstream direction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1209272','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1209272"><span>Development of Extended Period <span class="hlt">Pressure-Dependent</span> Demand Water Distribution Models</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>Judi, David R.; Mcpherson, Timothy N.</p> <p>2015-03-20</p> <p>Los Alamos National Laboratory (LANL) has used modeling and simulation of water distribution systems for N-1 contingency analyses to assess criticality of water system assets. Critical components considered in these analyses include pumps, tanks, and supply sources, in addition to critical pipes or aqueducts. A contingency represents the complete removal of the asset from system operation. For each contingency, an extended period simulation (EPS) is run using EPANET. An EPS simulates water system behavior over a time period, typically at least 24 hours. It assesses the ability of a system to respond and recover from asset disruption through distributed storagemore » in tanks throughout the system. Contingencies of concern are identified as those in which some portion of the water system has unmet delivery requirements. A delivery requirement is defined as an aggregation of water demands within a service area, similar to an electric power demand. The metric used to identify areas of unmet delivery requirement in these studies is a <span class="hlt">pressure</span> threshold of 15 pounds per square inch (psi). This <span class="hlt">pressure</span> threshold is used because it is below the required <span class="hlt">pressure</span> for fire protection. Any location in the model with <span class="hlt">pressure</span> that drops below this threshold at any time during an EPS is considered to have unmet service requirements and is used to determine cascading consequences. The outage area for a contingency is the aggregation of all service areas with a <span class="hlt">pressure</span> below the threshold at any time during the EPS.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013Nanos...5.3400L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013Nanos...5.3400L"><span>Photoluminescence and time-resolved carrier dynamics in thiol-capped CdTe nanocrystals under high <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>Lin, Yan-Cheng; Chou, Wu-Ching; Susha, Andrei S.; Kershaw, Stephen V.; Rogach, Andrey L.</p> <p>2013-03-01</p> <p>The application of static high <span class="hlt">pressure</span> provides a method for precisely controlling and investigating many fundamental and unique properties of semiconductor nanocrystals (NCs). This study systematically investigates the high-<span class="hlt">pressure</span> photoluminescence (PL) and time-resolved carrier dynamics of thiol-capped CdTe NCs of different sizes, at different concentrations, and in various stress environments. The zincblende-to-rocksalt phase transition in thiol-capped CdTe NCs is <span class="hlt">observed</span> at a <span class="hlt">pressure</span> far in excess of the bulk phase transition <span class="hlt">pressure</span>. Additionally, the process of transformation <span class="hlt">depends</span> strongly on NC size, and the phase transition <span class="hlt">pressure</span> increases with NC size. These peculiar phenomena are attributed to the distinctive bonding of thiols to the NC surface. In a nonhydrostatic environment, considerable flattening of the PL energy of CdTe NC powder is <span class="hlt">observed</span> above 3.0 GPa. Furthermore, asymmetric and double-peak PL emissions are obtained from a concentrated solution of CdTe NCs under hydrostatic <span class="hlt">pressure</span>, implying the feasibility of <span class="hlt">pressure</span>-induced interparticle coupling.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=gas+AND+liquid&pg=2&id=EJ935038','ERIC'); return false;" href="https://eric.ed.gov/?q=gas+AND+liquid&pg=2&id=EJ935038"><span>Gas <span class="hlt">Pressure</span>-Drop Experiment</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>Luyben, William L.; Tuzla, Kemal</p> <p>2010-01-01</p> <p>Most chemical engineering undergraduate laboratories have fluid mechanics experiments in which <span class="hlt">pressure</span> drops through pipes are measured over a range of Reynolds numbers. The standard fluid is liquid water, which is essentially incompressible. Since density is constant, <span class="hlt">pressure</span> drop does not <span class="hlt">depend</span> on the <span class="hlt">pressure</span> in the pipe. In addition, flow…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..1410770V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..1410770V"><span>Integration of Infrasound, Atmospheric <span class="hlt">Pressure</span>, and Seismic <span class="hlt">Observations</span> with the NSF EarthScope USArray Transportable Array</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vernon, F.; Tytell, J.; Hedlin, M. A. H.; Walker, K.; Busby, R.; Woodward, R.</p> <p>2012-04-01</p> <p>Earthscope's USArray Transportable Array (TA) network serves as a real-time monitoring and recording platform for both seismic and weather phenomena. To date, most of the approximately 500 TA stations have been retrofitted with VTI SCP1000 MEMS barometric <span class="hlt">pressure</span> gauges capable of recording data at 1 sample per second (sps). Additionally, over 300 of the TA stations have also been retrofitted with Setra 278 barometric gauges and NCPA infrasound sensors capable of recording data at 1 and 40 sps. While individual seismic events have been successfully researched via the TA network, <span class="hlt">observations</span> of powerful weather events by the TA network have yet to be embraced by the scientific community. This presentation will focus on case studies involving severe weather passage across portions of the TA network throughout 2011 in order to highlight its viability as a platform for real-time weather monitoring and research. It will also highlight the coupling of atmospheric signals into the seismic <span class="hlt">observations</span>. Examples of gust front passages and <span class="hlt">pressure</span> couplets from severe thunderstorms will be presented, as will <span class="hlt">observations</span> of multiple tornados occurred in the Spring of 2011. These data will demonstrate the overall viability of the TA network for monitoring severe weather events in real-time.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ChPhB..24e8901L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ChPhB..24e8901L"><span>Transportation-cyber-physical-systems-oriented engine cylinder <span class="hlt">pressure</span> estimation using high gain <span class="hlt">observer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Yong-Fu; Xiao-Pei, Kou; Zheng, Tai-Xiong; Li, Yin-Guo</p> <p>2015-05-01</p> <p>In transportation cyber-physical-systems (T-CPS), vehicle-to-vehicle (V2V) communications play an important role in the coordination between individual vehicles as well as between vehicles and the roadside infrastructures, and engine cylinder <span class="hlt">pressure</span> is significant for engine diagnosis on-line and torque control within the information exchange process under V2V communications. However, the parametric uncertainties caused from measurement noise in T-CPS lead to the dynamic performance deterioration of the engine cylinder <span class="hlt">pressure</span> estimation. Considering the high accuracy requirement under V2V communications, a high gain <span class="hlt">observer</span> based on the engine dynamic model is designed to improve the accuracy of <span class="hlt">pressure</span> estimation. Then, the analyses about convergence, converge speed and stability of the corresponding error model are conducted using the Laplace and Lyapunov method. Finally, results from combination of Simulink with GT-Power based numerical experiments and comparisons demonstrate the effectiveness of the proposed approach with respect to robustness and accuracy. Project supported by the National Natural Science Foundation of China (Grant No. 61304197), the Scientific and Technological Talents of Chongqing, China (Grant No. cstc2014kjrc-qnrc30002), the Key Project of Application and Development of Chongqing, China (Grant No. cstc2014yykfB40001), the Natural Science Funds of Chongqing, China (Grant No. cstc2014jcyjA60003), and the Doctoral Start-up Funds of Chongqing University of Posts and Telecommunications, China (Grant No. A2012-26).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22402774-pressure-magnetic-field-induced-phase-transformation-ni-sub-mn-sub-sub-heusler-alloy','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22402774-pressure-magnetic-field-induced-phase-transformation-ni-sub-mn-sub-sub-heusler-alloy"><span><span class="hlt">Pressure</span>-magnetic field induced phase transformation in Ni{sub 46}Mn{sub 41}In{sub 13} Heusler alloy</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>Rama Rao, N. V., E-mail: nvrrao@dmrl.drdo.in; Manivel Raja, M.; Pandian, S.</p> <p>2014-12-14</p> <p>The effect of hydrostatic <span class="hlt">pressure</span> and magnetic field on the magnetic properties and phase transformation in Ni{sub 46}Mn{sub 41}In{sub 13} Heusler alloy was investigated. <span class="hlt">Pressure</span> (P)-magnetic field (H)-temperature (T) phase diagram has been constructed from experimental results. In the P–T contour of the phase diagram, the slope of the austenite-martensite phase boundary line appears positive (dT/dP > 0), while it appears negative (dT/dH < 0) in the H–T contour. The results revealed that <span class="hlt">pressure</span> and magnetic field have opposite effect on phase stabilization. The combined effect of <span class="hlt">pressure</span> and magnetic field on martensitic transition has led to two important findings: (i) <span class="hlt">pressure</span> <span class="hlt">dependent</span> shiftmore » of austenite start temperature (A{sub s}) is higher when larger field is applied, and (ii) field <span class="hlt">dependent</span> shift of A{sub s} is lowered when a higher <span class="hlt">pressure</span> is applied. The <span class="hlt">pressure</span> and magnetic field <span class="hlt">dependent</span> shift <span class="hlt">observed</span> in the martensitic transformation has been explained on the basis of thermodynamic calculations. Curie temperature of the phases was found to increase with <span class="hlt">pressure</span> at a rate of 0.6 K/kbar.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1990JGR....95..341D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1990JGR....95..341D"><span>Micromechanics of <span class="hlt">pressure</span>-induced grain crushing in porous rocks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Davis, Daniel M.</p> <p>1990-01-01</p> <p>The hydrostatic compaction behavior of a suite of porous sandstones was investigated at confining <span class="hlt">pressures</span> up to 600 MPa and constant pore <span class="hlt">pressures</span> ranging up to 50 MPa. These five sandstones (Boise, Kayenta, St. Peter, Berea, and Weber) were selected because of their wide range of porosity (5-35%) and grain size (60-460 μm). We tested the law of effective stress for the porosity change as a function of <span class="hlt">pressure</span>. Except for Weber sandstone (which has the lowest porosity and smallest grain size), the hydrostat of each sandstone shows an inflection point corresponding to a critical effective <span class="hlt">pressure</span> beyond which an accelerated, irrecoverable compaction occurs. Our microstructural <span class="hlt">observations</span> show that brittle grain crushing initiates at this critical <span class="hlt">pressure</span>. We also <span class="hlt">observed</span> distributed cleavage cracking in calcite and intensive kinking in mica. The critical <span class="hlt">pressures</span> for grain crushing in our sandstones range from 75 to 380 MPa. In general, a sandstone with higher porosity and larger grain size has a critical <span class="hlt">pressure</span> which is lower than that of a sandstone with lower porosity and smaller grain size. We formulate a Hertzian fracture model to analyze the micromechanics of grain crushing. Assuming that the solid grains have preexisting microcracks with dimensions which scale with grain size, we derive an expression for the critical <span class="hlt">pressure</span> which <span class="hlt">depends</span> on the porosity, grain size, and fracture toughness of the solid matrix. The theoretical prediction is in reasonable agreement with our experimental data as well as other data from soil and rock mechanics studies for which the critical <span class="hlt">pressures</span> range over 3 orders of magnitude.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21104014-effect-solvent-absorption-spectra-all-trans-beta-carotene-under-high-pressure','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21104014-effect-solvent-absorption-spectra-all-trans-beta-carotene-under-high-pressure"><span>Effect of solvent on absorption spectra of all-trans-{beta}-carotene under high <span class="hlt">pressure</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>Liu, W. L.; Zheng, Z. R.; Liu, Z. G.</p> <p></p> <p>The absorption spectra of all-trans-{beta}-carotene in n-hexane and carbon disulfide (CS{sub 2}) solutions are measured under high <span class="hlt">pressure</span> at ambient temperature. The common redshift and broadening in the spectra are <span class="hlt">observed</span>. Simulation of the absorption spectra was performed by using the time-domain formula of the stochastic model. The <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the 0-0 band wavenumber is in agreement with the Bayliss theory at <span class="hlt">pressure</span> higher than 0.2 GPa. The deviation of the linearity at lower <span class="hlt">pressure</span> is ascribed to the reorientation of the solvent molecules. Both the redshift and broadening are stronger in CS{sub 2} than that in n-hexane becausemore » of the more sensitive <span class="hlt">pressure</span> <span class="hlt">dependence</span> of dispersive interactions in CS{sub 2} solution. The effect of <span class="hlt">pressure</span> on the transition moment is explained with the aid of a simple model involving the relative dimension, location, and orientation of the solute and solvent molecules. The implication of these results for light-harvesting functions of carotenoids in photosynthesis is also discussed.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999AcPPB..30..359B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999AcPPB..30..359B"><span>Mass <span class="hlt">Dependence</span> of the HBT Radii <span class="hlt">Observed</span> in e+e- Annihilation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bialas, A.; Zalewski, K.</p> <p>1999-02-01</p> <p>It is shown that the recently established strong mass-<span class="hlt">dependence</span> of the radii of the hadron sources, as <span class="hlt">observed</span> in HBT analyses of the e+e- annihilation, can be explained by assuming a generalized inside--outside cascade, i.e. that (i) the four-momenta and the space-time position four-vectors of the produced particles are approximately proportional to each other and (ii) the ``freeze-out'' times are distributed along the hyperbola t2-z2= τ02.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/3568957','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/3568957"><span>Vibration sensory thresholds <span class="hlt">depend</span> on <span class="hlt">pressure</span> of applied stimulus.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lowenthal, L M; Hockaday, T D</p> <p>1987-01-01</p> <p>Vibration sensory thresholds (VSTs) were estimated in 40 healthy subjects and 8 with diabetic peripheral neuropathy. A vibrameter and a biothesiometer were used at four sites and at differing <span class="hlt">pressures</span>. In normal subjects, with the vibrameter at 200 g, mean VST +/- SE for all sites was 1.87 micron +/- 0.22 and at 400 g dropped to 1.08 micron +/- 0.15 (P less than .0001). In 20 of these subjects with a biothesiometer at 200 and 400 g, mean VST fell from 12.8 +/- 1.5 to 11.1 +/- 1.1 (arbitrary units) (P = .01) when the greater <span class="hlt">pressure</span> was applied. In the 8 subjects with peripheral neuropathy, with the vibrameter at 200 and 400 g, respectively, mean VST fell from 70.7 +/- 26 to 7.2 +/- 1.8. VST in these subjects was estimated again after 1 mo and showed strong correlations with the previous values. Biothesiometer results correlated with vibrameter results at all sites. Thus, VST decreases as the <span class="hlt">pressure</span> of the applied stimulus is increased and this effect appears to be more marked in peripheral neuropathy. This has important consequences in monitoring this condition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002RScI...73.2999C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002RScI...73.2999C"><span>Thermoelectric power measurement under hydrostatic <span class="hlt">pressure</span> using a self-clamped <span class="hlt">pressure</span> cell</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Choi, E. S.; Kang, Haeyong; Jo, Y. J.; Kang, W.</p> <p>2002-08-01</p> <p>A thermoelectric power (TEP) measurement technique in a self-clamped <span class="hlt">pressure</span> cell is presented. Thermal and electrical contacts were glued to heaters by Stycast epoxy, which enhances thermal integration. The <span class="hlt">pressure</span> effect of Chromel-Constantan and Chromel-AuFe0.07% thermocouples are compared to Chromel-Alumel thermocouples, which are known to be <span class="hlt">pressure</span> insensitive between 4.2 and 300 K. The investigated thermocouples are found to have a small <span class="hlt">pressure</span> effect; approx][plus-or-minus4% at maximum in the measured temperature and <span class="hlt">pressure</span> range. Any <span class="hlt">pressure</span> effect on Au wires was also found to be very small from the <span class="hlt">pressure-dependent</span> TEP measurement of YBCO superconductor below Tc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/7369390','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/7369390"><span>Comparison of theoretical and <span class="hlt">observed</span> <span class="hlt">pressure</span> profiles in geothermal wells</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>Marquez M, R.</p> <p></p> <p>Two-phase water-steam flow conditions in geothermal wells are studied aimed at predicting <span class="hlt">pressure</span> drops in these wells. Five prediction methods were selected to be analyzed and compared with each other and with actual <span class="hlt">pressure</span> measurements. These five correlations were tested on five wells: three in New Zealand, one in Mexico, and one in the Philippines.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950023840&hterms=advanced+thermal+batteries&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dadvanced%2Bthermal%2Bbatteries','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950023840&hterms=advanced+thermal+batteries&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dadvanced%2Bthermal%2Bbatteries"><span>Advanced <span class="hlt">Dependent</span> <span class="hlt">Pressure</span> Vessel (DPV) nickel-hydrogen spacecraft cell and battery design</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Coates, Dwaine; Wright, Doug; Repplinger, Ron</p> <p>1995-01-01</p> <p>The <span class="hlt">dependent</span> <span class="hlt">pressure</span> vessel (DPV) nickel-hydrogen (NiH2) battery is being developed as a potential spacecraft battery design for both military and commercial satellites. Individual <span class="hlt">pressure</span> vessel (IPV) NiH2 batteries are currently flying on more than 70 Earth orbital satellites and have accumulated more than 140,000,000 cell-hours in actual spacecraft operation. The limitations of standard NiH2 IPV flight battery technology are primarily related to the internal cell design and the battery packaging issues associated with grouping multiple cylindrical cells. The DPV cell design offers higher specific energy and reduced cost, while retaining the established IPV NiH2 technology flight heritage and database. The advanced cell design offers a more efficient mechanical, electrical and thermal cell configuration and a reduced parts count. The internal electrode stack is a prismatic flat-plate arrangement. The flat individual cell <span class="hlt">pressure</span> vessel provides a maximum direct thermal path for removing heat from the electrode stack. The cell geometry also minimizes multiple-cell battery packaging constraints by using an established end-plateltie-rod battery design. A major design advantage is that the battery support structure is efficiently required to restrain only the force applied to a portion of the end cell. As the cells are stacked in series to achieve the desired system voltage, this increment of the total battery weight becomes small. The geometry of the DPV cell promotes compact, minimum volume packaging and places all cell terminals along the length of the battery. The resulting ability to minimize intercell wiring offers additional design simplicity and significant weight savings. The DPV battery design offers significant cost and weight savings advantages while providing minimal design risks. Cell and battery level design issues will be addressed including mechanical, electrical and thermal design aspects. A design performance analysis will be presented at both</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29323536','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29323536"><span>High Positive End-Expiratory <span class="hlt">Pressure</span> Renders Spontaneous Effort Noninjurious.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Morais, Caio C A; Koyama, Yukiko; Yoshida, Takeshi; Plens, Glauco M; Gomes, Susimeire; Lima, Cristhiano A S; Ramos, Ozires P S; Pereira, Sérgio M; Kawaguchi, Naomasa; Yamamoto, Hirofumi; Uchiyama, Akinori; Borges, João B; Vidal Melo, Marcos F; Tucci, Mauro R; Amato, Marcelo B P; Kavanagh, Brian P; Costa, Eduardo L V; Fujino, Yuji</p> <p>2018-05-15</p> <p>In acute respiratory distress syndrome (ARDS), atelectatic solid-like lung tissue impairs transmission of negative swings in pleural <span class="hlt">pressure</span> (Ppl) that result from diaphragmatic contraction. The localization of more negative Ppl proportionally increases <span class="hlt">dependent</span> lung stretch by drawing gas either from other lung regions (e.g., nondependent lung [pendelluft]) or from the ventilator. Lowering the level of spontaneous effort and/or converting solid-like to fluid-like lung might render spontaneous effort noninjurious. To determine whether spontaneous effort increases <span class="hlt">dependent</span> lung injury, and whether such injury would be reduced by recruiting atelectatic solid-like lung with positive end-expiratory <span class="hlt">pressure</span> (PEEP). Established models of severe ARDS (rabbit, pig) were used. Regional histology (rabbit), inflammation (positron emission tomography; pig), regional inspiratory Ppl (intrabronchial balloon manometry), and stretch (electrical impedance tomography; pig) were measured. Respiratory drive was evaluated in 11 patients with ARDS. Although injury during muscle paralysis was predominantly in nondependent and middle lung regions at low (vs. high) PEEP, strong inspiratory effort increased injury (indicated by positron emission tomography and histology) in <span class="hlt">dependent</span> lung. Stronger effort (vs. muscle paralysis) caused local overstretch and greater tidal recruitment in <span class="hlt">dependent</span> lung, where more negative Ppl was localized and greater stretch was generated. In contrast, high PEEP minimized lung injury by more uniformly distributing negative Ppl, and lowering the magnitude of spontaneous effort (i.e., deflection in esophageal <span class="hlt">pressure</span> <span class="hlt">observed</span> in rabbits, pigs, and patients). Strong effort increased <span class="hlt">dependent</span> lung injury, where higher local lung stress and stretch was generated; effort-<span class="hlt">dependent</span> lung injury was minimized by high PEEP in severe ARDS, which may offset need for paralysis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.T33F..05O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.T33F..05O"><span>Time-<span class="hlt">dependent</span> wellbore breakout growth caused by drilling-induced pore <span class="hlt">pressure</span> transients: Implications for estimations of far field stress magnitude</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Olcott, K. A.; Saffer, D. M.; Elsworth, D.</p> <p>2013-12-01</p> <p>One method used to constrain principal stress orientations and magnitudes in the crust combines estimates of rock strength with <span class="hlt">observations</span> of wellbore failures, including drilling-induced tensile fractures (DITF) and compressional borehole breakouts (BO). This method has been applied at numerous Integrated Ocean Drilling Program (IODP) boreholes drilled into sediments in a wide range of settings, including the Gulf of Mexico, the N. Japan and Costa Rican subduction margins, and the Nankai Trough Accretionary Prism. At Nankai and N. Japan, BO widths defined by logging-while-drilling (LWD) resistivity images have been used to estimate magnitudes of far-field horizontal tectonic stresses. At several drillsites (C0010, C0002, and C0011), sections of the borehole were relogged with LWD after the hole was left open for times ranging from ~30 min to 3 days; times between acquisition were associated with pipe connections (~30 min), cleaning and circulating the hole (up to ~3 hr), and evacuation of the site for weather (~3 days). Relogged portions exhibit widening of BO, hypothesized to reflect time-<span class="hlt">dependent</span> re-equilibration of instantaneous changes in pore fluid <span class="hlt">pressure</span> (Pf) induced by opening the borehole. In this conceptual model, Pf decrease caused by initial excavation of the borehole and resulting changes in the state of stress at the borehole wall lead to an initial strengthening of the sediment. Re-equilibration of Pf results in time-<span class="hlt">dependent</span> weakening of the sediment and subsequent BO growth. If correct, this hypothesis implies that stress magnitudes estimated by BO widths could be significantly underestimated. We test this idea using a finite-element model in COMSOL multiphysics that couples fluid flow and deformation in a poroelastic medium. We specify far-field horizontal principal stresses (SHmax and Shmin) in the model domain. At the start of simulations/at the time of borehole opening, we impose a decreased stress at the borehole wall. We consider a</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('http://adsabs.harvard.edu/abs/2014AGUFMMR41C..04B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMMR41C..04B"><span>Compaction and Permeability Reduction of Castlegate Sandstone under Pore <span class="hlt">Pressure</span> Cycling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bauer, S. J.</p> <p>2014-12-01</p> <p>We investigate time-<span class="hlt">dependent</span> compaction and permeability changes by cycling pore <span class="hlt">pressure</span> with application to compressed air energy storage (CAES) in a reservoir. Preliminary experiments capture the impacts of hydrostatic stress, pore water <span class="hlt">pressure</span>, pore <span class="hlt">pressure</span> cycling, chemical, and time-<span class="hlt">dependent</span> considerations near a borehole in a CAES reservoir analog. CAES involves creating an air bubble in a reservoir. The high <span class="hlt">pressure</span> bubble serves as a mechanical battery to store potential energy. When there is excess grid energy, bubble <span class="hlt">pressure</span> is increased by air compression, and when there is energy needed on the grid, stored air <span class="hlt">pressure</span> is released through turbines to generate electricity. The analog conditions considered are depth ~1 km, overburden stress ~20 MPa and a pore <span class="hlt">pressure</span> ~10MPa. Pore <span class="hlt">pressure</span> is cycled daily or more frequently between ~10 MPa and 6 MPa, consistent with operations of a CAES facility at this depth and may continue for operational lifetime (25 years). The rock can vary from initially fully-to-partially saturated. Pore <span class="hlt">pressure</span> cycling changes the effective stress.Jacketed, room temperature tap water-saturated samples of Castlegate Sandstone are hydrostatically confined (20 MPa) and subjected to a pore <span class="hlt">pressure</span> resulting in an effective <span class="hlt">pressure</span> of ~10 MPa. Pore <span class="hlt">pressure</span> is cycled between 6 to 10 MPa. Sample displacement measurements yielded determinations of volumetric strain and from water flow measurements permeability was determined. Experiments ran for two to four weeks, with 2 to 3 pore <span class="hlt">pressure</span> cycles per day. The Castlegate is a fluvial high porosity (>20%) primarily quartz sandstone, loosely calcite cemented, containing a small amount of clay.Pore <span class="hlt">pressure</span> cycling induces compaction (~.1%) and permeability decreases (~20%). The results imply that time-<span class="hlt">dependent</span> compactive processes are operative. The load path, of increasing and decreasing pore <span class="hlt">pressure</span>, may facilitate local loosening and grain readjustments that results in the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5932982','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5932982"><span>Voltage and partial <span class="hlt">pressure</span> <span class="hlt">dependent</span> defect chemistry in (La,Sr)FeO3–δ thin films investigated by chemical capacitance measurements</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Rupp, Ghislain M.; Fleig, Jürgen</p> <p>2018-01-01</p> <p>La0.6Sr0.4FeO3–δ (LSF) thin films of different thickness were prepared by pulsed laser deposition on yttria stabilized zirconia (YSZ) and characterized by using three electrode impedance spectroscopy. Electrochemical film capacitance was analyzed in relation to oxygen partial <span class="hlt">pressure</span> (0.25 mbar to 1 bar), DC polarization (0 m to –600 m) and temperature (500 to 650 °C). For most measurement parameters, the chemical bulk capacitance dominates the overall capacitive properties and the corresponding defect chemical state <span class="hlt">depends</span> solely on the oxygen chemical potential inside the film, independent of atmospheric oxygen <span class="hlt">pressure</span> and DC polarization. Thus, defect chemical properties (defect concentrations and defect formation enthalpies) could be deduced from such measurements. Comparison with LSF defect chemical bulk data from the literature showed good agreement for vacancy formation energies but suggested larger electronic defect concentrations in the films. From thickness-<span class="hlt">dependent</span> measurements at lower oxygen chemical potentials, an additional capacitive contribution could be identified and attributed to the LSF|YSZ interface. Deviations from simple chemical capacitance models at high <span class="hlt">pressures</span> are most probably due to defect interactions. PMID:29671421</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JVGR..356..264C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JVGR..356..264C"><span>Viscoelastic modeling of deformation and gravity changes induced by <span class="hlt">pressurized</span> magmatic sources</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Currenti, Gilda</p> <p>2018-05-01</p> <p>Gravity and height changes, which reflect magma accumulation in subsurface chambers, are evaluated using analytical and numerical models in order to investigate their relationships and temporal evolutions. The analysis focuses mainly on the exploration of the time-<span class="hlt">dependent</span> response of gravity and height changes to the <span class="hlt">pressurization</span> of ellipsoidal magmatic chambers in viscoelastic media. Firstly, the validation of the numerical Finite Element results is performed by comparison with analytical solutions, which are devised for a simple spherical source embedded in a homogeneous viscoelastic half-space medium. Then, the effect of several model parameters on time-<span class="hlt">dependent</span> height and gravity changes is investigated thanks to the flexibility of the numerical method in handling complex configurations. Both homogeneous and viscoelastic shell models reveal significantly different amplitudes in the ratio between gravity and height changes <span class="hlt">depending</span> on geometry factors and medium rheology. The results show that these factors also influence the relaxation characteristic times of the investigated geophysical changes. Overall, these temporal patterns are compatible with time-<span class="hlt">dependent</span> height and gravity changes <span class="hlt">observed</span> on Etna volcano during the 1994-1997 inflation period. By modeling the viscoelastic response of a <span class="hlt">pressurized</span> prolate magmatic source, a general agreement between computed and <span class="hlt">observed</span> geophysical variations is achieved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JKPS...63..627T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JKPS...63..627T"><span>Magnetic property in the ferromagnetic superconductor UGe2 at <span class="hlt">pressures</span> above the ferromagnetic critical <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>Tateiwa, Naoyuki; Haga, Yoshinori; Matsuda, Tatsuma D.; Yamamoto, Etsuji; Ōnuki, Yoshichika; Fisk, Zachary</p> <p>2013-08-01</p> <p>We have studied the high-<span class="hlt">pressure</span> magnetic property in UGe2 where ferromagnetic superconductivity appears under high <span class="hlt">pressure</span>. In this study, we focus on the magnetic property at <span class="hlt">pressures</span> above the ferromagnetic critical <span class="hlt">pressure</span> P c =1.6 GPa. The temperature and magnetic field <span class="hlt">dependences</span> of the dc-magnetization have been measured under high <span class="hlt">pressures</span> up to 5.1 GPa by using a ceramic anvil high <span class="hlt">pressure</span> cell. At <span class="hlt">pressures</span> above P c , the magnetic susceptibility x shows a broad maximum around T χmax and the magnetization at 2.0 K shows an abrupt increase (metamagnetic transition) at H c . With increasing <span class="hlt">pressure</span>, the peak structure in x becomes broader, and the peak position T χmax moves to the higher temperature region. The metamagnetic field H c increases rapidly with increasing <span class="hlt">pressure</span>. At <span class="hlt">pressures</span> above 4.1 GPa, x shows a simple temperature <span class="hlt">dependence</span>, and the magnetization increases linearly with increasing field. These phenomena in UGe2 resemble to those in the intermetallic compounds of 3 d transition metals such as Co(S1- x Se x ) and YCo2. We discuss the experimental results by using the phenomenological spin-fluctuation theory.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26231250','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26231250"><span>Increased night duty loading of physicians caused elevated blood <span class="hlt">pressure</span> and sympathetic tones in a dose-<span class="hlt">dependent</span> manner.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lee, Hsiu-Hao; Lo, Shih-Hsiang; Chen, Bing-Yu; Lin, Yen-Hung; Chu, Dachen; Cheng, Tsun-Jen; Chen, Pau-Chung; Guo, Yue-Liang</p> <p>2016-04-01</p> <p>Night duty has been recognized as a significantly harmful stressor for physicians. However, the relationship between various levels of duty loading and stress response is unknown. This study examined whether duty load increases cardiovascular stress indicators in a dose-<span class="hlt">dependent</span> manner. An unallocated prospective <span class="hlt">observational</span> study was conducted among physicians performing various levels of duties in a secondary referral medical center between 2011 and 2012. Heart rate variability (HRV), blood <span class="hlt">pressure</span> (BP), and other stress markers of 12 attending physicians were compared during different duty loads: non-duty day (NDD), duty day with one duty area and three wards (1DD), and duty day with two duty areas and six wards (2DD). During the regular sleep time (i.e., 11 p.m. to 5 a.m.), the relative sympathetic modulations measured using the HRV were 59.0 ± 9.3, 61.6 ± 10.4, and 64.4 ± 8.9 for NDD, 1DD, and 2DD, respectively (p = 0.0012); those for relative parasympathetic modulations were 37.4 ± 9.4, 34.8 ± 9.8, and 32.0 ± 8.8 for NDD, 1DD, and 2DD, respectively (p = 0.0015). The percentages of abnormal systolic BPs were 9.7 ± 13.2 %, 25.3 ± 21.8 %, and 31.5 ± 21.0 % for NDD, 1DD, and 2DD, respectively (p = 0.003), and the percentages of abnormal diastolic BP were 6.7 ± 11.0 %, 18.3 ± 11.1 %, and 27.1 ± 30.9 % for NDD, 1DD, and 2DD, respectively (p = 0.002). Total sleep time was negatively associated with sympathetic/parasympathetic balance and the percentage of abnormal diastolic BP. Admitting new patients was positively associated with the percentages of abnormal systolic BP. This <span class="hlt">observational</span> analysis suggests that the dose-<span class="hlt">dependent</span> stress responses of the cardiovascular system in physicians were caused by the duty load.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19..967R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19..967R"><span>DaDyn-RS: a tool for the time-<span class="hlt">dependent</span> simulation of damage, fluid <span class="hlt">pressure</span> and long-term instability in alpine rock slopes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Riva, Federico; Agliardi, Federico; Amitrano, David; Crosta, Giovanni B.</p> <p>2017-04-01</p> <p>Large mountain slopes in alpine environments undergo a complex long-term evolution from glacial to postglacial environments, through a transient period of paraglacial readjustment. During and after this transition, the interplay among rock strength, topographic relief, and morpho-climatic drivers varying in space and time can lead to the development of different types of slope instability, from sudden catastrophic failures to large, slow, long-lasting yet potentially catastrophic rockslides. Understanding the long-term evolution of large rock slopes requires accounting for the time-<span class="hlt">dependence</span> of deglaciation unloading, permeability and fluid <span class="hlt">pressure</span> distribution, displacements and failure mechanisms. In turn, this is related to a convincing description of rock mass damage processes and to their transition from a sub-critical (progressive failure) to a critical (catastrophic failure) character. Although mechanisms of damage occurrence in rocks have been extensively studied in the laboratory, the description of time-<span class="hlt">dependent</span> damage under gravitational load and variable external actions remains difficult. In this perspective, starting from a time-<span class="hlt">dependent</span> model conceived for laboratory rock deformation, we developed Dadyn-RS, a tool to simulate the long-term evolution of real, large rock slopes. Dadyn-RS is a 2D, FEM model programmed in Matlab, which combines damage and time-to-failure laws to reproduce both diffused damage and strain localization meanwhile tracking long-term slope displacements from primary to tertiary creep stages. We implemented in the model the ability to account for rock mass heterogeneity and property upscaling, time-<span class="hlt">dependent</span> deglaciation, as well as damage-<span class="hlt">dependent</span> fluid <span class="hlt">pressure</span> occurrence and stress corrosion. We first tested DaDyn-RS performance on synthetic case studies, to investigate the effect of the different model parameters on the mechanisms and timing of long-term slope behavior. The model reproduces complex interactions between</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25823888','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25823888"><span>Estimation of <span class="hlt">pressure</span>-, temperature- and frictional heating-related effects on proteins' retention under ultra-high-<span class="hlt">pressure</span> liquid chromatographic conditions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fekete, Szabolcs; Guillarme, Davy</p> <p>2015-05-08</p> <p>The goal of this work was to evaluate the changes in retention induced by frictional heating, <span class="hlt">pressure</span> and temperature under ultra high <span class="hlt">pressure</span> liquid chromatography (UHPLC) conditions, for four model proteins (i.e. lysozyme, myoglobin, fligrastim and interferon alpha-2A) possessing molecular weights between 14 and 20kDa. First of all, because the decrease of the molar volume upon adsorption onto a hydrophobic surface was more pronounced for large molecules such as proteins, the impact of <span class="hlt">pressure</span> appears to overcome the frictional heating effects. Nevertheless, we have also demonstrated that the retention decrease due to frictional heating was not negligible with such large biomolecules in the variable inlet <span class="hlt">pressure</span> mode. Secondly, it is clearly shown that the modification of retention under various <span class="hlt">pressure</span> and temperature conditions cannot be explained solely by the frictional heating and <span class="hlt">pressure</span> effects. Indeed, some very uncommon van't Hoff plots (concave plots with a maximum) were recorded for our model/therapeutic proteins. These maximum retention factors values on the van't Hoff plots indicate a probable change of secondary structure/conformation with <span class="hlt">pressure</span> and temperature. Based on these <span class="hlt">observations</span>, it seems that the combination of <span class="hlt">pressure</span> and temperature causes the protein denaturation and this folding-unfolding procedure is clearly protein <span class="hlt">dependent</span>. Copyright © 2015 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26342493','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26342493"><span>Particle-based optical <span class="hlt">pressure</span> sensors for 3D <span class="hlt">pressure</span> mapping.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Banerjee, Niladri; Xie, Yan; Chalaseni, Sandeep; Mastrangelo, Carlos H</p> <p>2015-10-01</p> <p>This paper presents particle-based optical <span class="hlt">pressure</span> sensors for in-flow <span class="hlt">pressure</span> sensing, especially for microfluidic environments. Three generations of <span class="hlt">pressure</span> sensitive particles have been developed- flat planar particles, particles with integrated retroreflectors and spherical microballoon particles. The first two versions suffer from <span class="hlt">pressure</span> measurement <span class="hlt">dependence</span> on particles orientation in 3D space and angle of interrogation. The third generation of microspherical particles with spherical symmetry solves these problems making particle-based manometry in microfluidic environment a viable and efficient methodology. Static and dynamic <span class="hlt">pressure</span> measurements have been performed in liquid medium for long periods of time in a <span class="hlt">pressure</span> range of atmospheric to 40 psi. Spherical particles with radius of 12 μm and balloon-wall thickness of 0.5 μm are effective for more than 5 h in this <span class="hlt">pressure</span> range with an error of less than 5%.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015CliPa..11.1027B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015CliPa..11.1027B"><span>A collection of sub-daily <span class="hlt">pressure</span> and temperature <span class="hlt">observations</span> for the early instrumental period with a focus on the "year without a summer" 1816</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brugnara, Y.; Auchmann, R.; Brönnimann, S.; Allan, R. J.; Auer, I.; Barriendos, M.; Bergström, H.; Bhend, J.; Brázdil, R.; Compo, G. P.; Cornes, R. C.; Dominguez-Castro, F.; van Engelen, A. F. V.; Filipiak, J.; Holopainen, J.; Jourdain, S.; Kunz, M.; Luterbacher, J.; Maugeri, M.; Mercalli, L.; Moberg, A.; Mock, C. J.; Pichard, G.; Řezníčková, L.; van der Schrier, G.; Slonosky, V.; Ustrnul, Z.; Valente, M. A.; Wypych, A.; Yin, X.</p> <p>2015-08-01</p> <p>The eruption of Mount Tambora (Indonesia) in April 1815 is the largest documented volcanic eruption in history. It is associated with a large global cooling during the following year, felt particularly in parts of Europe and North America, where the year 1816 became known as the "year without a summer". This paper describes an effort made to collect surface meteorological <span class="hlt">observations</span> from the early instrumental period, with a focus on the years of and immediately following the eruption (1815-1817). Although the collection aimed in particular at <span class="hlt">pressure</span> <span class="hlt">observations</span>, correspondent temperature <span class="hlt">observations</span> were also recovered. Some of the series had already been described in the literature, but a large part of the data, recently digitised from original weather diaries and contemporary magazines and newspapers, is presented here for the first time. The collection puts together more than 50 sub-daily series from land observatories in Europe and North America and from ships in the tropics. The <span class="hlt">pressure</span> <span class="hlt">observations</span> have been corrected for temperature and gravity and reduced to mean sea level. Moreover, an additional statistical correction was applied to take into account common error sources in mercury barometers. To assess the reliability of the corrected data set, the variance in the <span class="hlt">pressure</span> <span class="hlt">observations</span> is compared with modern climatologies, and single <span class="hlt">observations</span> are used for synoptic analyses of three case studies in Europe. All raw <span class="hlt">observations</span> will be made available to the scientific community in the International Surface <span class="hlt">Pressure</span> Databank.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950031215&hterms=How+temperature+effect+rate+evaporation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DHow%2Btemperature%2Beffect%2Brate%2Bevaporation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950031215&hterms=How+temperature+effect+rate+evaporation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DHow%2Btemperature%2Beffect%2Brate%2Bevaporation"><span>Theoretical and Experimental Investigations on Droplet Evaporation and Droplet Ignition at High <span class="hlt">Pressures</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ristau, R.; Nagel, U.; Iglseder, H.; Koenig, J.; Rath, H. J.; Normura, H.; Kono, M.; Tanabe, M.; Sato, J.</p> <p>1993-01-01</p> <p>The evaporation of fuel droplets under high ambient <span class="hlt">pressure</span> and temperature in normal gravity and microgravity has been investigated experimentally. For subcritical ambient conditions, droplet evaporation after a heat-up period follows the d(exp 2)-law. For all data the evaporation constant increases as the ambient temperature increases. At identical ambient conditions the evaporation constant under microgravity is smaller compared to normal gravity. This effect can first be <span class="hlt">observed</span> at 1 bar and increases with ambient <span class="hlt">pressure</span>. Preliminary experiments on ignition delay for self-igniting fuel droplets have been performed. Above a 1 s delay time, at identical ambient conditions, significant differences in the results of the normal and microgravity data are <span class="hlt">observed</span>. Self-ignition occurs within different temperature ranges due to the influence of gravity. The time <span class="hlt">dependent</span> behavior of the droplet is examined theoretically. In the calculations two different approaches for the gas phase are applied. In the first approach the conditions at the interface are given using a quasi steady theory approximation. The second approach uses a set of time <span class="hlt">dependent</span> governing equations for the gas phase which are then evaluated. In comparison, the second model shows a better agreement with the drop tower experiments. In both cases a time <span class="hlt">dependent</span> gasification rate is <span class="hlt">observed</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26484744','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26484744"><span>Dorsalis pedis arterial <span class="hlt">pressure</span> is lower than noninvasive arm blood <span class="hlt">pressure</span> in normotensive patients under sevoflurane anesthesia.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Yan; Wang, Enqin; Zhu, Yuan; Li, Yongshuai; Lu, Kaizhi</p> <p>2016-02-01</p> <p>It is widely known that blood <span class="hlt">pressure</span> (BP) in the lower extremity is higher than in the upper extremity. However, whether this phenomenon remains the same during general anesthesia is still unclear. This study aims to investigate the difference between invasive dorsalis pedis artery (DPA) <span class="hlt">pressure</span> and the most commonly used noninvasive arm <span class="hlt">pressure</span> during sevoflurane anesthesia. A total of 50 normotensive Chinese patients were enrolled in this <span class="hlt">observational</span> study. Invasive DPA <span class="hlt">pressure</span>, noninvasive arm <span class="hlt">pressure</span>, and systemic vascular resistance index were assessed simultaneously. BP data during the entire surgery were analyzed through a Bland-Altman plot for repeated measures. The concordance of BP variation in the DPA and the arm was analyzed using four-quadrant plots and linear regression. The time-<span class="hlt">dependent</span> changes in BP and the systemic vascular resistance index were also evaluated. Data from 46 effective cases were analyzed. Bias (95% limits of agreement) was -7.40 mmHg (-20.36 to +5.57 mmHg) for mean blood <span class="hlt">pressure</span>, +3.54 mmHg (-20.32 to +27.41 mmHg) for systolic blood <span class="hlt">pressure</span>, and -10.20 mmHg (-23.66 to +3.26 mmHg) for diastolic blood <span class="hlt">pressure</span>, respectively. The concordance of BP variation at the two measurement sites was clinically acceptable. DPA <span class="hlt">pressure</span> and vascular resistance in the lower limb decreased gradually during surgery. DPA <span class="hlt">pressure</span> tends to be lower than arm <span class="hlt">pressure</span> under sevoflurane anesthesia, especially the mean blood <span class="hlt">pressure</span> and the diastolic blood <span class="hlt">pressure</span>. Hence, noninvasive arm BP monitoring is recommend to be retained when invasive BP is measured at the DPA, so as to allow clinicians to comprehensively evaluate the BP condition of the patients and make appropriate therapeutic decisions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2811046','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2811046"><span>Cerebral flow velocities during daily activities <span class="hlt">depend</span> on blood <span class="hlt">pressure</span> in patients with chronic ischemic infarctions</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Novak, Vera; Hu, Kun; Desrochers, Laura; Novak, Peter; Caplan, Louis; Lipsitz, Lewis; Selim, Magdy</p> <p>2010-01-01</p> <p>Background Target blood <span class="hlt">pressure</span> (BP) values for optimal cerebral perfusion after an ischemic stroke are still debated. We sought to examine the relationship between BP and cerebral blood flow velocities (BFV) during daily activities. Methods We studied 43 patients with chronic large vessel ischemic infarctions in middle cerebral artery (MCA) territory (aged 64.2±8.94 years; at 6.1±4.9 years after stroke), and 67 age-matched controls. BFV in MCAs were measured during supine baseline, sitting, standing and tilt. A regression analysis and a dynamic phase analysis were used to quantify BP-BFV relationship. Results The mean arterial <span class="hlt">pressure</span> was similar between the groups (89±15 mmHg). Baseline BFV were lower by ~ 30% in the stroke patients compared to the controls (p=0.0001). BFV declined further with postural changes, and remained lower in the stroke group during sitting (p=0.003), standing (p=0.003) and tilt (p=0.002) as compared to the control group. Average BFV on the stroke side were positively correlated with BP during baseline (R=0.54, p=0.0022, the slope 0.46 cm/s/mm Hg) and tilt (R=0.52, p=0.0028, the slope 0.40 cm/s/mm Hg). Regression analysis suggested that BFV may increase ~ 30-50% at mean BP > 100 mmHg. Orthostatic hypotension during the first minute of tilt or standing was independently associated with lower BFV on the stroke side (p=0.0008). Baseline BP-BFV phase shift derived from the phase analysis was smaller on the stroke-side (p=0.0006). Conclusion We found that BFV are lower in stroke patients and daily activities such as standing could induce hypoperfusion. BFV increase with mean arterial <span class="hlt">pressure</span> > 100 mmHg. <span class="hlt">Dependency</span> of BFV on arterial <span class="hlt">pressure</span> may have implications for BP management after stroke. Further prospective investigations are needed to determine the impact of these findings on functional recovery and strategies to improve perfusion <span class="hlt">pressure</span> during daily activities after ischemic stroke. PMID:19959536</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19959536','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19959536"><span>Cerebral flow velocities during daily activities <span class="hlt">depend</span> on blood <span class="hlt">pressure</span> in patients with chronic ischemic infarctions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Novak, Vera; Hu, Kun; Desrochers, Laura; Novak, Peter; Caplan, Louis; Lipsitz, Lewis; Selim, Magdy</p> <p>2010-01-01</p> <p>Target blood <span class="hlt">pressure</span> (BP) values for optimal cerebral perfusion after an ischemic stroke are still debated. We sought to examine the relationship between BP and cerebral blood flow velocities (BFVs) during daily activities. We studied 43 patients with chronic large vessel ischemic infarctions in the middle cerebral artery territory (aged 64.2+/-8.94 years; at 6.1+/-4.9 years after stroke) and 67 age-matched control subjects. BFVs in middle cerebral arteries were measured during supine baseline, sitting, standing, and tilt. A regression analysis and a dynamic phase analysis were used to quantify the BP-BFV relationship. The mean arterial <span class="hlt">pressure</span> was similar between the groups (89+/-15 mm Hg). Baseline BFVs were lower by approximately 30% in the patients with stroke compared with the control subjects (P=0.0001). BFV declined further with postural changes and remained lower in the stroke group during sitting (P=0.003), standing (P=0.003), and tilt (P=0.002) as compared with the control group. Average BFVs on the stroke side were positively correlated with BP during baseline (R=0.54, P=0.0022, the slope 0.46 cm/s/mm Hg) and tilt (R=0.52, P=0.0028, the slope 0.40 cm/s/mm Hg). Regression analysis suggested that BFV may increase approximately 30% to 50% at mean BP >100 mm Hg. Orthostatic hypotension during the first minute of tilt or standing was independently associated with lower BFV on the stroke side (P=0.0008). Baseline BP-BFV phase shift derived from the phase analysis was smaller on the stroke side (P=0.0006). We found that BFVs are lower in patients with stroke and daily activities such as standing could induce hypoperfusion. BFVs increase with mean arterial <span class="hlt">pressure</span> >100 mm Hg. <span class="hlt">Dependency</span> of BFV on arterial <span class="hlt">pressure</span> may have implications for BP management after stroke. Further prospective investigations are needed to determine the impact of these findings on functional recovery and strategies to improve perfusion <span class="hlt">pressure</span> during daily activities after ischemic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApJ...844..156R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApJ...844..156R"><span>From Neutron Star <span class="hlt">Observables</span> to the Equation of State. II. Bayesian Inference of Equation of State <span class="hlt">Pressures</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Raithel, Carolyn A.; Özel, Feryal; Psaltis, Dimitrios</p> <p>2017-08-01</p> <p>One of the key goals of <span class="hlt">observing</span> neutron stars is to infer the equation of state (EoS) of the cold, ultradense matter in their interiors. Here, we present a Bayesian statistical method of inferring the <span class="hlt">pressures</span> at five fixed densities, from a sample of mock neutron star masses and radii. We show that while five polytropic segments are needed for maximum flexibility in the absence of any prior knowledge of the EoS, regularizers are also necessary to ensure that simple underlying EoS are not over-parameterized. For ideal data with small measurement uncertainties, we show that the <span class="hlt">pressure</span> at roughly twice the nuclear saturation density, {ρ }{sat}, can be inferred to within 0.3 dex for many realizations of potential sources of uncertainties. The <span class="hlt">pressures</span> of more complicated EoS with significant phase transitions can also be inferred to within ˜30%. We also find that marginalizing the multi-dimensional parameter space of <span class="hlt">pressure</span> to infer a mass-radius relation can lead to biases of nearly 1 km in radius, toward larger radii. Using the full, five-dimensional posterior likelihoods avoids this bias.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/797901','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/797901"><span>Prediction of failure <span class="hlt">pressure</span> and leak rate of stress corrosion.</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>Majumdar, S.; Kasza, K.; Park, J. Y.</p> <p>2002-06-24</p> <p>An ''equivalent rectangular crack'' approach was employed to predict rupture <span class="hlt">pressures</span> and leak rates through laboratory generated stress corrosion cracks and steam generator tubes removed from the McGuire Nuclear Station. Specimen flaws were sized by post-test fractography in addition to a pre-test advanced eddy current technique. The predicted and <span class="hlt">observed</span> test data on rupture and leak rate are compared. In general, the test failure <span class="hlt">pressures</span> and leak rates are closer to those predicted on the basis of fractography than on nondestructive evaluation (NDE). However, the predictions based on NDE results are encouraging, particularly because they have the potential to determinemore » a more detailed geometry of ligamented cracks, from which failure <span class="hlt">pressure</span> and leak rate can be more accurately predicted. One test specimen displayed a time-<span class="hlt">dependent</span> increase of leak rate under constant <span class="hlt">pressure</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160014020','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160014020"><span>Development of a Numerical Model of Hypervelocity Impact into a <span class="hlt">Pressurized</span> Composite Overwrapped <span class="hlt">Pressure</span> Vessel</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Garcia, M. A.; Davis, B. A.; Miller, J. E.</p> <p>2017-01-01</p> <p> considered a catastrophic failure. This assumption is conservative and made due to lack of knowledge on the level of allow-able damage to the composite overwrap that can be sustained and still allow successful completion of the mission. To quantify the allowable damage level to the composite overwrap involves assessing stress redistribution following damage as well as evaluating possible time-<span class="hlt">dependent</span> mechanisms involved in the COPV response to an impact event. Limited published work in this subject has shown that COPV can withstand at least some level of damage due to high energy impacts. These <span class="hlt">observations</span> have been confirmed and expanded upon in recent experimental research performed by NASA. This research has demonstrated that there is not only robustness in a COPV to compensate for CFRP damage, but has also identified two significant failure modes for <span class="hlt">pressurized</span> COPV. The lowest threshold failure mode involves the perforation of the vessel, and the highest threshold failure mode is the catastrophic rupture. While both of these failure modes mean a loss of the COPV, system robustness affords some tolerance to the venting as opposed to the more catastrophic rupture. As a consequence, it is necessary to understand the conditions that result in the transition between these failure modes. The aforementioned experimental research has been performed in both the unpressurized and <span class="hlt">pressurized</span> condition to identify the damage level that triggered the failure thresh-old. This COPV test program was sponsored by the NASA Engineering and Safety Center (NESC), and tests were performed at NASA White Sands Test Facility (WSTF). Planning and coordination were provided by NASA JSC Hypervelocity Impact Technology (HVIT) group, and the COPVs were provided by the ISS Program. Unpressurized testing has been conducted at the <span class="hlt">pressure</span> of the vacuum test chamber, while, the <span class="hlt">pressurized</span> testing has been conducted at 290 +/- 10 bar (4,200 ? 100 psi) using nitrogen as the <span class="hlt">pressurizing</span> gas, which</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020022192&hterms=balance+sheet&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dbalance%2Bsheet','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020022192&hterms=balance+sheet&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dbalance%2Bsheet"><span>Relation Between <span class="hlt">Pressure</span> Balance Structures and Polar Plumes from Ulysses High Latitude <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yamauchi, Y.; Suess, Steven T.; Sakurai, T.; Whitaker, Ann F. (Technical Monitor)</p> <p>2001-01-01</p> <p>Ulysses <span class="hlt">observations</span> have shown that <span class="hlt">pressure</span> balance structures (PBSs) are a common feature in high-latitude, fast solar wind near solar minimum. Previous studies of Ulysses/SWOOPS plasma data suggest these PBSs may be remnants of coronal polar plumes. Here we find support for this suggestion in an analysis of PBS magnetic structure. We used Ulysses magnetometer data and applied a minimum variance analysis to discontinuities. We found that PBSs preferentially contain tangential discontinuities, as opposed to rotational discontinuities and to non-PBS regions in the solar wind. This suggests that PBSs contain structures like current sheets or plasmoids that may be associated with network activity at the base of plumes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920032835&hterms=physical+dependence&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dphysical%2Bdependence','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920032835&hterms=physical+dependence&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dphysical%2Bdependence"><span>Model and <span class="hlt">observation</span> comparison of the universal time and IMF by <span class="hlt">dependence</span> of the ionospheric polar hole</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sojka, J. J.; Schunk, R. W.; Hoegy, W. R.; Grebowsky, J. M.</p> <p>1991-01-01</p> <p>The polar ionospheric F-region often exhibits regions of marked density depletion. These depletions have been <span class="hlt">observed</span> by a variety of polar orbiting ionospheric satellites over a full range of solar cycle, season, magnetic activity, and universal time (UT). An empirical model of these <span class="hlt">observations</span> has recently been developed to describe the polar depletion <span class="hlt">dependence</span> on these parameters. Specifically, the <span class="hlt">dependence</span> has been defined as a function of F10.7 (solar), summer or winter, Kp (magnetic), and UT. Polar cap depletions have also been predicted /1, 2/ and are, hence, present in physical models of the high latitude ionosphere. Using the Utah State University Time <span class="hlt">Dependent</span> Ionospheric Model (TDIM) the predicted polar depletion characteristics are compared with those described by the above empirical model. In addition, the TDIM is used to predict the IMF By <span class="hlt">dependence</span> of the polar hole feature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009JGRB..114.7205L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009JGRB..114.7205L"><span>Effective <span class="hlt">pressure</span> law for permeability of E-bei sandstones</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, M.; Bernabé, Y.; Xiao, W.-I.; Chen, Z.-Y.; Liu, Z.-Q.</p> <p>2009-07-01</p> <p>Laboratory experiments were conducted to determine the effective <span class="hlt">pressure</span> law for permeability of tight sandstone rocks from the E-bei gas reservoir, China. The permeability k of five core samples was measured while cycling the confining <span class="hlt">pressure</span> pc and fluid <span class="hlt">pressure</span> pf. The permeability data were analyzed using the response-surface method, a statistical model-building approach yielding a representation of k in (pc, pf) space that can be used to determine the effective <span class="hlt">pressure</span> law, i.e., peff = pc - κpf. The results show that the coefficient κ of the effective <span class="hlt">pressure</span> law for permeability varies with confining <span class="hlt">pressure</span> and fluid <span class="hlt">pressure</span> as well as with the loading or unloading cycles (i.e., hysteresis effect). Moreover, κ took very small values in some of the samples, even possibly lower than the value of porosity, in contradiction with a well-accepted theoretical model. We also reanalyzed a previously published permeability data set on fissured crystalline rocks and found again that the κ varies with pc but did not <span class="hlt">observe</span> κ values lower than 0.4, a value much larger than porosity. Analysis of the <span class="hlt">dependence</span> of permeability on effective <span class="hlt">pressure</span> suggests that the occurrence of low κ values may be linked to the high-<span class="hlt">pressure</span> sensitivity of E-bei sandstones.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850032109&hterms=free+radicals&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dfree%2Bradicals','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850032109&hterms=free+radicals&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dfree%2Bradicals"><span>Temperature and <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the absolute rate constant for the reactions of NH2 radicals with acetylene and ethylene</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bosco, S. R.; Nava, D. F.; Brobst, W. D.; Stief, L. J.</p> <p>1984-01-01</p> <p>The absolute rate constants for the reaction between the NH2 free radical and acetylene and ethylene is measured experimentally using a flash photolysis technique. The constant is considered to be a function of temperature and <span class="hlt">pressure</span>. At each temperature level of the experiment, the <span class="hlt">observed</span> pseudo-first-order rate constants were assumed to be independent of flash intensity. The results of the experiment indicate that the bimolecular rate constant for the NH2 + C2H2 reaction increases with <span class="hlt">pressure</span> at 373 K and 459 K but not at lower temperatures. Results near the <span class="hlt">pressure</span> limit conform to an Arrhenius expression of 1.11 (+ or -) 0.36 x 10 to the -13th over the temperature range from 241 to 459 K. For the reaction NH2 + C2H4, a smaller rate of increase in the bimolecular rate constant was <span class="hlt">observed</span> over the temperature range 250-465 K. The implications of these results for current theoretical models of NH2 + C2H2 (or H4) reactions in the atmospheres of Jupiter and Saturn are discussed.</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('https://www.ncbi.nlm.nih.gov/pubmed/27723794','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27723794"><span>The Intracranial Volume <span class="hlt">Pressure</span> Response in Increased Intracranial <span class="hlt">Pressure</span> Patients: Clinical Significance of the Volume <span class="hlt">Pressure</span> Indicator.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lai, Hung-Yi; Lee, Ching-Hsin; Lee, Ching-Yi</p> <p>2016-01-01</p> <p>For patients suffering from primary brain injury, monitoring intracranial <span class="hlt">pressure</span> alone is not enough to reflect the dynamic intracranial condition. In our previous study, a segment of the <span class="hlt">pressure</span>-volume curve can be expressed by the parabolic regression model with single indicator "a". The aim of this study is to evaluate if the indicator "a" can reflect intracranial conditions. Patients with traumatic brain injury, spontaneous intracranial hemorrhage, and/or hydrocephalus who had external ventricular drainage from January 2009 to February 2010 were included. The successive volume <span class="hlt">pressure</span> response values were obtained by successive drainage of cerebral spinal fluid from intracranial <span class="hlt">pressure</span> 20-25 mm Hg to 10 mm Hg. The relationship between withdrawn cerebral spinal fluid volume and intracranial <span class="hlt">pressure</span> was analyzed by the parabolic regression model with single parameter "a". The overall mean for indicator "a" was 0.422 ± 0.046. The mean of "a" in hydrocephalus was 0.173 ± 0.024 and in severe intracranial mass with slender ventricle, it was 0.663 ± 0.062. The two extreme intracranial conditions had a statistical significant difference (p<0.001). The indicator "a" of a <span class="hlt">pressure</span>-volume curve can reflect the dynamic intracranial condition and is comparable in different situations. A significantly larger indicator "a" with increased intracranial <span class="hlt">pressure</span> is always <span class="hlt">observed</span> in severe intracranial mass lesions with cerebral edema. A significantly smaller indicator "a" with increased intracranial <span class="hlt">pressure</span> is <span class="hlt">observed</span> in hydrocephalus. Brain computed tomography should be performed early if a rapid elevation of indicator "a" is detected, as it can reveal some ongoing intracranial pathology prior to clinical deterioration. Increased intracranial <span class="hlt">pressure</span> was frequently <span class="hlt">observed</span> in patients with intracranial pathology. The progression can be differentiated using the pattern of the volume <span class="hlt">pressure</span> indicator.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5056694','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5056694"><span>The Intracranial Volume <span class="hlt">Pressure</span> Response in Increased Intracranial <span class="hlt">Pressure</span> Patients: Clinical Significance of the Volume <span class="hlt">Pressure</span> Indicator</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>2016-01-01</p> <p>Background For patients suffering from primary brain injury, monitoring intracranial <span class="hlt">pressure</span> alone is not enough to reflect the dynamic intracranial condition. In our previous study, a segment of the <span class="hlt">pressure</span>-volume curve can be expressed by the parabolic regression model with single indicator “a”. The aim of this study is to evaluate if the indicator “a” can reflect intracranial conditions. Methods Patients with traumatic brain injury, spontaneous intracranial hemorrhage, and/or hydrocephalus who had external ventricular drainage from January 2009 to February 2010 were included. The successive volume <span class="hlt">pressure</span> response values were obtained by successive drainage of cerebral spinal fluid from intracranial <span class="hlt">pressure</span> 20–25 mm Hg to 10 mm Hg. The relationship between withdrawn cerebral spinal fluid volume and intracranial <span class="hlt">pressure</span> was analyzed by the parabolic regression model with single parameter “a”. Results The overall mean for indicator “a” was 0.422 ± 0.046. The mean of “a” in hydrocephalus was 0.173 ± 0.024 and in severe intracranial mass with slender ventricle, it was 0.663 ± 0.062. The two extreme intracranial conditions had a statistical significant difference (p<0.001). Conclusion The indicator “a” of a <span class="hlt">pressure</span>-volume curve can reflect the dynamic intracranial condition and is comparable in different situations. A significantly larger indicator “a” with increased intracranial <span class="hlt">pressure</span> is always <span class="hlt">observed</span> in severe intracranial mass lesions with cerebral edema. A significantly smaller indicator “a” with increased intracranial <span class="hlt">pressure</span> is <span class="hlt">observed</span> in hydrocephalus. Brain computed tomography should be performed early if a rapid elevation of indicator “a” is detected, as it can reveal some ongoing intracranial pathology prior to clinical deterioration. Increased intracranial <span class="hlt">pressure</span> was frequently <span class="hlt">observed</span> in patients with intracranial pathology. The progression can be differentiated using the pattern of the volume</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22713051','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22713051"><span>High <span class="hlt">pressure</span> study of molecular dynamics of protic ionic liquid lidocaine hydrochloride.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Swiety-Pospiech, A; Wojnarowska, Z; Pionteck, J; Pawlus, S; Grzybowski, A; Hensel-Bielowka, S; Grzybowska, K; Szulc, A; Paluch, M</p> <p>2012-06-14</p> <p>In this paper, we investigate the effect of <span class="hlt">pressure</span> on the molecular dynamics of protic ionic liquid lidocaine hydrochloride, a commonly used pharmaceutical, by means of dielectric spectroscopy and <span class="hlt">pressure</span>-temperature-volume methods. We <span class="hlt">observed</span> that near T(g) the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of conductivity relaxation times reveals a peculiar behavior, which can be treated as a manifestation of decoupling between ion migration and structural relaxation times. Moreover, we discuss the validity of thermodynamic scaling in lidocaine HCl. We also employed the temperature-volume Avramov model to determine the value of <span class="hlt">pressure</span> coefficient of glass transition temperature, dT(g)/dP|(P = 0.1). Finally, we investigate the role of thermal and density fluctuations in controlling of molecular dynamics of the examined compound.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JAdD....720002B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JAdD....720002B"><span>Time-<span class="hlt">dependence</span> of the electromechanical bending actuation <span class="hlt">observed</span> in ionic-electroactive polymers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bass, Patrick S.; Zhang, Lin; Cheng, Z.-Y.</p> <p></p> <p>The characteristics of the electromechanical response <span class="hlt">observed</span> in an ionic-electroactive polymer (i-EAP) are represented by the time (t) <span class="hlt">dependence</span> of its bending actuation (y). The electromechanical response of a typical i-EAP — poly(ethylene oxide) (PEO) doped with lithium perchlorate (LP) — is studied. The shortcomings of all existing models describing the electromechanical response obtained in i-EAPs are discussed. A more reasonable model: y=ymaxe-τ/t is introduced to characterize this time <span class="hlt">dependence</span> for all i-EAPs. The advantages and correctness of this model are confirmed using results obtained in PEO-LP actuators with different LP contents and at different temperatures. The applicability and universality of this model are validated using the reported results obtained from two different i-EAPs: one is Flemion and the other is polypyrrole actuators.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25585399','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25585399"><span>Correction for frequency-<span class="hlt">dependent</span> hydrophone response to nonlinear <span class="hlt">pressure</span> waves using complex deconvolution and rarefactional filtering: application with fiber optic hydrophones.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wear, Keith; Liu, Yunbo; Gammell, Paul M; Maruvada, Subha; Harris, Gerald R</p> <p>2015-01-01</p> <p>Nonlinear acoustic signals contain significant energy at many harmonic frequencies. For many applications, the sensitivity (frequency response) of a hydrophone will not be uniform over such a broad spectrum. In a continuation of a previous investigation involving deconvolution methodology, deconvolution (implemented in the frequency domain as an inverse filter computed from frequency-<span class="hlt">dependent</span> hydrophone sensitivity) was investigated for improvement of accuracy and precision of nonlinear acoustic output measurements. Timedelay spectrometry was used to measure complex sensitivities for 6 fiber-optic hydrophones. The hydrophones were then used to measure a <span class="hlt">pressure</span> wave with rich harmonic content. Spectral asymmetry between compressional and rarefactional segments was exploited to design filters used in conjunction with deconvolution. Complex deconvolution reduced mean bias (for 6 fiber-optic hydrophones) from 163% to 24% for peak compressional <span class="hlt">pressure</span> (p+), from 113% to 15% for peak rarefactional <span class="hlt">pressure</span> (p-), and from 126% to 29% for pulse intensity integral (PII). Complex deconvolution reduced mean coefficient of variation (COV) (for 6 fiber optic hydrophones) from 18% to 11% (p+), 53% to 11% (p-), and 20% to 16% (PII). Deconvolution based on sensitivity magnitude or the minimum phase model also resulted in significant reductions in mean bias and COV of acoustic output parameters but was less effective than direct complex deconvolution for p+ and p-. Therefore, deconvolution with appropriate filtering facilitates reliable nonlinear acoustic output measurements using hydrophones with frequency-<span class="hlt">dependent</span> sensitivity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27463696','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27463696"><span>On Localized Vapor <span class="hlt">Pressure</span> Gradients Governing Condensation and Frost Phenomena.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nath, Saurabh; Boreyko, Jonathan B</p> <p>2016-08-23</p> <p>Interdroplet vapor <span class="hlt">pressure</span> 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 <span class="hlt">pressure</span> 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 <span class="hlt">pressure</span> field for all possible modes of condensation and desublimation in order to gain fundamental insight into how <span class="hlt">pressure</span> 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 <span class="hlt">depending</span> upon the temperature and wettability of the surface. The calculated <span class="hlt">pressure</span> 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 <span class="hlt">pressure</span> 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 <span class="hlt">observed</span>; a bimodal phase map is developed, demonstrating its <span class="hlt">dependence</span> 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 <span class="hlt">pressure</span> gradients for the design of spatially controlled or antifrosting phase-change systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ApSS..297..125J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ApSS..297..125J"><span>The electrical properties of low <span class="hlt">pressure</span> chemical vapor deposition Ga doped ZnO thin films <span class="hlt">depending</span> on chemical bonding configuration</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jung, Hanearl; Kim, Doyoung; Kim, Hyungjun</p> <p>2014-04-01</p> <p>The electrical and chemical properties of low <span class="hlt">pressure</span> chemical vapor deposition (LP-CVD) Ga doped ZnO (ZnO:Ga) films were systematically investigated using Hall measurement and X-ray photoemission spectroscopy (XPS). Diethylzinc (DEZ) and O2 gas were used as precursor and reactant gas, respectively, and trimethyl gallium (TMGa) was used as a Ga doping source. Initially, the electrical properties of undoped LP-CVD ZnO films <span class="hlt">depending</span> on the partial <span class="hlt">pressure</span> of DEZ and O2 ratio were investigated using X-ray diffraction (XRD) by changing partial <span class="hlt">pressure</span> of DEZ from 40 to 140 mTorr and that of O2 from 40 to 80 mTorr. The resistivity was reduced by Ga doping from 7.24 × 10-3 Ω cm for undoped ZnO to 2.05 × 10-3 Ω cm for Ga doped ZnO at the TMG <span class="hlt">pressure</span> of 8 mTorr. The change of electric properties of Ga doped ZnO with varying the amount of Ga dopants was systematically discussed based on the structural crystallinity and chemical bonding configuration, analyzed by XRD and XPS, respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JAP...117c3102Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JAP...117c3102Y"><span><span class="hlt">Observation</span> of laser-driven shock propagation by nanosecond time-resolved Raman spectroscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yu, Guoyang; Zheng, Xianxu; Song, Yunfei; Zeng, Yangyang; Guo, Wencan; Zhao, Jun; Yang, Yanqiang</p> <p>2015-01-01</p> <p>An improved nanosecond time-resolved Raman spectroscopy is performed to <span class="hlt">observe</span> laser-driven shock propagation in the anthracene/epoxy glue layer. The digital delay instead of optical delay line is introduced for sake of unlimited time range of detection, which enables the ability to <span class="hlt">observe</span> both shock loading and shock unloading that always lasts several hundred nanoseconds. In this experiment, the peak <span class="hlt">pressure</span> of shock wave, the <span class="hlt">pressure</span> distribution, and the position of shock front in gauge layer were determined by fitting Raman spectra of anthracene using the Raman peak shift simulation. And, the velocity of shock wave was calculated by the time-<span class="hlt">dependent</span> position of shock front.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1995JMMM..140.1253N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1995JMMM..140.1253N"><span>Magnetization at high <span class="hlt">pressure</span> in CeP</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Naka, T.; Matsumoto, T.; Okayama, Y.; Môri, N.; Haga, Y.; Suzuki, T.</p> <p>1995-02-01</p> <p>We have investigated the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of magnetization below 60 K up to 1.6 GPa in the low-carrier concentration system CeP showing two step transitions at T = TL and TH under high <span class="hlt">pressure</span>. At high <span class="hlt">pressure</span>, M( P, T) exhibits a maximum at around the lower transition temperature TL. This behavior implies that the magnetic state changes at TL. The <span class="hlt">pressure</span> <span class="hlt">dependence</span> of isothermal magnetization M( P) is different above and below TL. In fact, M( P) below TL exhibits a maximum at around 1.4 GPa, whereas M( P) above TL increases steeply with <span class="hlt">pressure</span> up to 1.6 GPa.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19791382','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19791382"><span>Adsorption of carbon monoxide on smaller gold-cluster anions in an atmospheric-<span class="hlt">pressure</span> flow-reactor: temperature and humidity <span class="hlt">dependence</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wallace, William T; Wyrwas, Richard B; Leavitt, Andrew J; Whetten, Robert L</p> <p>2005-03-07</p> <p>In the absence of moisture and at room temperature, the activity and saturation of CO on gold cluster anions, Au(N)-, are known to be highly <span class="hlt">dependent</span> on the size of the cluster. Small Au(N)- clusters (N = 2,3) showed no adsorption activity, and the saturation CO adsorption values did not increase proportionately to cluster size or area. Here, we report on the effects of water vapor and temperature on the ability of Au(N)- clusters to adsorb CO in a high-<span class="hlt">pressure</span>, fast-flow reactor. In contrast to all earlier reports, our results using this method show that smaller gold-cluster anions bind single and multiple CO groups at ambient temperature and above. In particular, species previously unseen at room temperature, corresponding to Au2(CO)-, Au3(CO) and Au4(CO)2, have been <span class="hlt">observed</span>. Apparently, the presence of water vapor facilitates the adsorption of CO on the smaller clusters, possibly by aiding in the release of adsorption energy. As the number of studies concerning gold catalysis has continually increased over the past decade, these results provide important new information on the possible role of moisture in gold catalysis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22395475-pressure-dependence-refractive-index-wurtzite-rocksalt-indium-nitride','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22395475-pressure-dependence-refractive-index-wurtzite-rocksalt-indium-nitride"><span><span class="hlt">Pressure</span> <span class="hlt">dependence</span> of the refractive index in wurtzite and rocksalt indium nitride</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>Oliva, R.; MALTA-Consolider Team, Departament de Física Aplicada, ICMUV, Universitat de València, c/Dr. Moliner 50, 46100 Burjassot, València; Segura, A.</p> <p>2014-12-08</p> <p>We have performed high-<span class="hlt">pressure</span> Fourier transform infrared reflectance measurements on a freestanding InN thin film to determine the refractive index of wurtzite InN and its high-<span class="hlt">pressure</span> rocksalt phase as a function of hydrostatic <span class="hlt">pressure</span>. From a fit to the experimental refractive-index curves including the effect of the high-energy optical gaps, phonons, free carriers, and the direct (fundamental) band-gap in the case of wurtzite InN, we obtain <span class="hlt">pressure</span> coefficients for the low-frequency (electronic) dielectric constant ε{sub ∞}. Negative <span class="hlt">pressure</span> coefficients of −8.8 × 10{sup −2 }GPa{sup −1} and −14.8 × 10{sup −2 }GPa{sup −1} are obtained for the wurtzite and rocksalt phases, respectively. The results are discussedmore » in terms of the electronic band structure and the compressibility of both phases.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24188402','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24188402"><span>The flexible focus: whether spatial attention is unitary or divided <span class="hlt">depends</span> on <span class="hlt">observer</span> goals.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jefferies, Lisa N; Enns, James T; Di Lollo, Vincent</p> <p>2014-04-01</p> <p>The distribution of visual attention has been the topic of much investigation, and various theories have posited that attention is allocated either as a single unitary focus or as multiple independent foci. In the present experiment, we demonstrate that attention can be flexibly deployed as either a unitary or a divided focus in the same experimental task, <span class="hlt">depending</span> on the <span class="hlt">observer</span>'s goals. To assess the distribution of attention, we used a dual-stream Attentional Blink (AB) paradigm and 2 target pairs. One component of the AB, Lag-1 sparing, occurs only if the second target pair appears within the focus of attention. By varying whether the first-target-pair could be expected in a predictable location (always in-stream) or not (unpredictably in-stream or between-streams), <span class="hlt">observers</span> were encouraged to deploy a divided or a unitary focus, respectively. When the second-target-pair appeared between the streams, Lag-1 sparing occurred for the Unpredictable group (consistent with a unitary focus) but not for the Predictable group (consistent with a divided focus). Thus, diametrically different outcomes occurred for physically identical displays, <span class="hlt">depending</span> on the expectations of the <span class="hlt">observer</span> about where spatial attention would be required.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28543926','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28543926"><span>Comparative effect of the sites of anterior cervical <span class="hlt">pressure</span> on the geometry of the upper esophageal sphincter high-<span class="hlt">pressure</span> zone.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mei, Ling; Jiao, Hongmei; Sharma, Tarun; Dua, Arshish; Sanvanson, Patrick; Jadcherla, Sudarshan R; Shaker, Reza</p> <p>2017-11-01</p> <p>External cricoid <span class="hlt">pressure</span> is increasingly used to augment the upper esophageal sphincter (UES). Our objective was to determine the effect of 1) <span class="hlt">pressures</span> applied to cricoid, supracricoid, and subcricoid regions on the length and amplitude of the UES high-<span class="hlt">pressure</span> zone (UESHPZ), and 2) the external cricoid <span class="hlt">pressure</span> on lower esophageal sphincter (LES) tone. Case-control study. We studied 11 patients with supraesophageal reflux (mean age 58 ± 12 years) and 10 healthy volunteers (mean age 47 ± 19 years). We tested 20, 30, and 40 mm Hg <span class="hlt">pressures</span> to cricoid, 1 cm proximal and 1 cm distal to the cricoid. In an additional 15 healthy volunteers (mean age 46 ± 23 years), we studied the effect of external cricoid <span class="hlt">pressure</span> on LES tone. UES and LES <span class="hlt">pressures</span> were determined using high-resolution manometry. There was significant increase of UESHPZ length with application of <span class="hlt">pressure</span> at all sites. The increase of UESHPZ length was relatively symmetric, more orad, and more caudad when the <span class="hlt">pressure</span> was applied at the cricoid, supracricoid, and subcricoid levels, respectively. The magnitude of <span class="hlt">pressure</span> increase was greatest at the middle and orad part of the UESHPZ when the <span class="hlt">pressure</span> was applied at the cricoid and supracricoid levels, respectively. The corresponding magnitude of increase in the caudad part of the UESHPZ was not <span class="hlt">observed</span> with <span class="hlt">pressure</span> at the subcricoid level. There was no change of the LES <span class="hlt">pressure</span> with application of cricoid <span class="hlt">pressure</span>. The effect of external <span class="hlt">pressure</span> on the UESHPZ is site <span class="hlt">dependent</span>. Subcricoid <span class="hlt">pressure</span> has the least effect on UESHPZ. External cricoid <span class="hlt">pressure</span> at 20 to 40 mm Hg has no effect on the LES <span class="hlt">pressure</span>. 3b. Laryngoscope, 127:2466-2474, 2017. © 2017 The American Laryngological, Rhinological and Otological Society, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C34B..03T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C34B..03T"><span>Understanding and <span class="hlt">Observing</span> Subglacial Friction Using Seismology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsai, V. C.</p> <p>2017-12-01</p> <p>Glaciology began with a focus on understanding basic mechanical processes and producing physical models that could explain the principal <span class="hlt">observations</span>. Recently, however, more attention has been paid to the wealth of recent <span class="hlt">observations</span>, with many modeling efforts relying on data assimilation and empirical scalings, rather than being based on first-principles physics. Notably, ice sheet models commonly assume that subglacial friction is characterized by a "slipperiness" coefficient that is determined by inverting surface velocity <span class="hlt">observations</span>. Predictions are usually then made by assuming these slipperiness coefficients are spatially and temporally fixed. However, this is only valid if slipperiness is an unchanging material property of the bed and, despite decades of work on subglacial friction, it has remained unclear how to best account for such subglacial physics in ice sheet models. Here, we describe how basic seismological concepts and <span class="hlt">observations</span> can be used to improve our understanding and determination of subglacial friction. First, we discuss how standard models of granular friction can and should be used in basal friction laws for marine ice sheets, where very low effective <span class="hlt">pressures</span> exist. We show that under realistic West Antarctic Ice Sheet conditions, standard Coulomb friction should apply in a relatively narrow zone near the grounding line and that this should transition abruptly as one moves inland to a different, perhaps Weertman-style, <span class="hlt">dependence</span> of subglacial stress on velocity. We show that this subglacial friction law predicts significantly different ice sheet behavior even as compared with other friction laws that include effective <span class="hlt">pressure</span>. Secondly, we explain how seismological <span class="hlt">observations</span> of water flow noise and basal icequakes constrain subglacial physics in important ways. Seismically <span class="hlt">observed</span> water flow noise can provide constraints on water <span class="hlt">pressures</span> and channel sizes and geometry, leading to important data on subglacial friction</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016RJPCA..90..990P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016RJPCA..90..990P"><span>Temperature <span class="hlt">dependences</span> of saturated vapor <span class="hlt">pressure</span> and the enthalpy of vaporization of n-pentyl esters of dicarboxylic acids</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Portnova, S. V.; Krasnykh, E. L.; Levanova, S. V.</p> <p>2016-05-01</p> <p>The saturated vapor <span class="hlt">pressures</span> and enthalpies of vaporization of n-pentyl esters of linear C2-C6 dicarboxylic acids are determined by the transpiration method in the temperature range of 309.2-361.2 K. The <span class="hlt">dependences</span> of enthalpies of vaporization on the number of carbon atoms in the molecule and on the retention indices have been determined. The predictive capabilities of the existing calculation schemes for estimation of enthalpy of vaporization of the studied compounds have been analyzed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29455118','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29455118"><span>Multivariate dynamic Tobit models with lagged <span class="hlt">observed</span> <span class="hlt">dependent</span> variables: An effectiveness analysis of highway safety laws.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dong, Chunjiao; Xie, Kun; Zeng, Jin; Li, Xia</p> <p>2018-04-01</p> <p>Highway safety laws aim to influence driver behaviors so as to reduce the frequency and severity of crashes, and their outcomes. For one specific highway safety law, it would have different effects on the crashes across severities. Understanding such effects can help policy makers upgrade current laws and hence improve traffic safety. To investigate the effects of highway safety laws on crashes across severities, multivariate models are needed to account for the interdependency issues in crash counts across severities. Based on the characteristics of the <span class="hlt">dependent</span> variables, multivariate dynamic Tobit (MVDT) models are proposed to analyze crash counts that are aggregated at the state level. Lagged <span class="hlt">observed</span> <span class="hlt">dependent</span> variables are incorporated into the MVDT models to account for potential temporal correlation issues in crash data. The state highway safety law related factors are used as the explanatory variables and socio-demographic and traffic factors are used as the control variables. Three models, a MVDT model with lagged <span class="hlt">observed</span> <span class="hlt">dependent</span> variables, a MVDT model with unobserved random variables, and a multivariate static Tobit (MVST) model are developed and compared. The results show that among the investigated models, the MVDT models with lagged <span class="hlt">observed</span> <span class="hlt">dependent</span> variables have the best goodness-of-fit. The findings indicate that, compared to the MVST, the MVDT models have better explanatory power and prediction accuracy. The MVDT model with lagged <span class="hlt">observed</span> variables can better handle the stochasticity and <span class="hlt">dependency</span> in the temporal evolution of the crash counts and the estimated values from the model are closer to the <span class="hlt">observed</span> values. The results show that more lives could be saved if law enforcement agencies can make a sustained effort to educate the public about the importance of motorcyclists wearing helmets. Motor vehicle crash-related deaths, injuries, and property damages could be reduced if states enact laws for stricter text messaging rules, higher</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19860000169&hterms=Exciter&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DExciter','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19860000169&hterms=Exciter&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DExciter"><span>Dynamic <span class="hlt">Pressure</span> Calibration Standard</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schutte, P. C.; Cate, K. H.; Young, S. D.</p> <p>1986-01-01</p> <p>Vibrating columns of fluid used to calibrate transducers. Dynamic <span class="hlt">pressure</span> calibration standard developed for calibrating flush diaphragm-mounted <span class="hlt">pressure</span> transducers. <span class="hlt">Pressures</span> up to 20 kPa (3 psi) accurately generated over frequency range of 50 to 1,800 Hz. System includes two conically shaped aluminum columns one 5 cm (2 in.) high for low <span class="hlt">pressures</span> and another 11 cm (4.3 in.) high for higher <span class="hlt">pressures</span>, each filled with viscous fluid. Each column mounted on armature of vibration exciter, which imparts sinusoidally varying acceleration to fluid column. Signal noise low, and waveform highly <span class="hlt">dependent</span> on quality of drive signal in vibration exciter.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JGRD..120.5548H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JGRD..120.5548H"><span>A data assimilation technique to account for the nonlinear <span class="hlt">dependence</span> of scattering microwave <span class="hlt">observations</span> of precipitation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Haddad, Z. S.; Steward, J. L.; Tseng, H.-C.; Vukicevic, T.; Chen, S.-H.; Hristova-Veleva, S.</p> <p>2015-06-01</p> <p>Satellite microwave <span class="hlt">observations</span> of rain, whether from radar or passive radiometers, <span class="hlt">depend</span> in a very crucial way on the vertical distribution of the condensed water mass and on the types and sizes of the hydrometeors in the volume resolved by the instrument. This crucial <span class="hlt">dependence</span> is nonlinear, with different types and orders of nonlinearity that are due to differences in the absorption/emission and scattering signatures at the different instrument frequencies. Because it is not monotone as a function of the underlying condensed water mass, the nonlinearity requires great care in its representation in the <span class="hlt">observation</span> operator, as the inevitable uncertainties in the numerous precipitation variables are not directly convertible into an additive white uncertainty in the forward calculated <span class="hlt">observations</span>. In particular, when attempting to assimilate such data into a cloud-permitting model, special care needs to be applied to describe and quantify the expected uncertainty in the <span class="hlt">observations</span> operator in order not to turn the implicit white additive uncertainty on the input values into complicated biases in the calculated radiances. One approach would be to calculate the means and covariances of the nonlinearly calculated radiances given an a priori joint distribution for the input variables. This would be a very resource-intensive proposal if performed in real time. We propose a representation of the <span class="hlt">observation</span> operator based on performing this moment calculation off line, with a dimensionality reduction step to allow for the effective calculation of the <span class="hlt">observation</span> operator and the associated covariance in real time during the assimilation. The approach is applicable to other remotely sensed <span class="hlt">observations</span> that <span class="hlt">depend</span> nonlinearly on model variables, including wind vector fields. The approach has been successfully applied to the case of tropical cyclones, where the organization of the system helps in identifying the dimensionality-reducing variables.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24118408','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24118408"><span>Physical activity levels and torso orientations of hospitalized patients at risk of developing a <span class="hlt">pressure</span> injury: an <span class="hlt">observational</span> study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chaboyer, Wendy; Mills, Peter M; Roberts, Shelley; Latimer, Sharon</p> <p>2015-02-01</p> <p><span class="hlt">Pressure</span> injury guidelines recommend regular repositioning yet patients' mobility and repositioning patterns are unknown. An <span class="hlt">observational</span> study using activity monitors was undertaken to describe the 24 h activity patterns of 84 hospitalized patients at risk of developing a <span class="hlt">pressure</span> injury. The vast majority of participants' time was spent in the sedentary activity range (94% ± 3%) followed by the light range (5% ± 4 %). Patients changed their posture a median of 94 (interquartile range 48) time in the 24-h period (range 11-154), or ≈ 3.8 times per hour. Although a main focus for <span class="hlt">pressure</span> injury prevention has been on repositioning, this study shows that patients with restricted mobility are actually moving quite often. Therefore, it might be appropriate to focus more attention on other <span class="hlt">pressure</span> injury prevention strategies such as adequate nutrition, appropriate support surfaces and good skin care. © 2013 Wiley Publishing Asia Pty Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRA..123.3170Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRA..123.3170Z"><span>The Detached Auroras Induced by the Solar Wind <span class="hlt">Pressure</span> Enhancement in Both Hemispheres From Imaging and In Situ Particle <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhou, Su; Luan, Xiaoli; Søraas, Finn; Østgaard, Nikolai; Raita, Tero</p> <p>2018-04-01</p> <p>This paper presents simultaneous detached proton auroras that appeared in both hemispheres at 11:06 UT, 08 March 2012, just 2 min after a sudden solar wind <span class="hlt">pressure</span> enhancement ( 11:04 UT) hit the Earth. They were <span class="hlt">observed</span> under northward interplanetary magnetic field Bz condition and during the recovery phase of a moderate geomagnetic storm. In the Northern Hemisphere, Defense Meteorological Satellite Program/Special Sensor Ultraviolet Spectrographic Imager <span class="hlt">observed</span> that the detached arc occurred within 60°-65° magnetic latitude and covered a few magnetic local time (MLT) hours ranging from 0530 to 0830 MLT with a possible extension toward noon. At the same time (11:06 UT), Polar Orbiting Environment Satellites 19 detected a detached proton aurora around 1300 MLT in the Southern Hemisphere, centering 62° magnetic latitude, which was at the same latitudes as the northern detached arc. This southern aurora was most probably a part of a dayside detached arc that was conjugate to the northern one. In situ particle <span class="hlt">observations</span> indicated that the detached auroras were dominated by protons/ions with energies ranging from around 20 keV to several hundreds of keV, without obvious electron precipitations. These detached arcs persisted for less than 6 min, consistent with the impact from <span class="hlt">pressure</span> enhancement and the <span class="hlt">observed</span> electromagnetic ion cyclotron (EMIC) waves. It is suggested that the increasing solar wind <span class="hlt">pressure</span> pushed the hot ions in the ring current closer to Earth where the steep gradient of cold plasma favored EMIC wave growth. By losing energy to EMIC waves the energetic protons (>20 keV) were scattered into the loss cone and produced the <span class="hlt">observed</span> detached proton auroras.</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('https://www.ncbi.nlm.nih.gov/pubmed/21195361','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21195361"><span>Gender differences in the accuracy of time-<span class="hlt">dependent</span> blood <span class="hlt">pressure</span> indices for predicting coronary heart disease: A random-effects modeling approach.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Brant, Larry J; Ferrucci, Luigi; Sheng, Shan L; Concin, Hans; Zonderman, Alan B; Kelleher, Cecily C; Longo, Dan L; Ulmer, Hanno; Strasak, Alexander M</p> <p>2010-12-01</p> <p>Previous studies on blood <span class="hlt">pressure</span> (BP) indices as a predictor of coronary heart disease (CHD) have provided equivocal results and generally relied on Cox proportional hazards regression methodology, with age and sex accounting for most of the predictive capability of the model. The aim of the present study was to use serially collected BP measurements to examine age-and gender-related differences in BP indices for predicting CHD. The predictive accuracy of time-<span class="hlt">dependent</span> BP indices for CHD was investigated using a method of risk prediction based on posterior probabilities calculated from mixed-effects regression to utilize intraindividual differences in serial BP measurements according to age changes within gender groups. Data were collected prospectively from 2 community-dwelling cohort studies in the United States (Baltimore Longitudinal Study of Aging [BLSA]) and Europe (Vorarlberg Health Monitoring and Promotion Program [VHM&PP]). The study comprised 152,633 participants (aged 30-74 years) and 610,061 BP measurements. During mean follow-up of 7.5 years, 2457 nonfatal and fatal CHD events were <span class="hlt">observed</span>. In both study populations, pulse <span class="hlt">pressure</span> (PP) and systolic blood <span class="hlt">pressure</span> (SBP) performed best as individual predictors of CHD in women (area under the receiver operating characteristic curve [AUC(ROC)] was between 0.83 and 0.85 for PP, and between 0.77 and 0.81 for SBP). Mean arterial <span class="hlt">pressure</span> (MAP) and diastolic blood <span class="hlt">pressure</span> (DBP) performed better for men (AUC(ROC) = 0.67 and 0.65 for MAP and DBP, respectively, in the BLSA; AUC(ROC) = 0.77 and 0.75 in the VHM&PP) than for women (AUC(ROC) = 0.60 for both MAP and DBP in the BLSA; AUC(ROC) = 0.75 and 0.52, respectively, in the VHM&PP). The degree of discrimination in both populations was overall greater but more varied for all BP indices for women (AUC(ROC) estimates between 0.85 [PP in the VHM&PP] and 0.52 [DBP in the VHM&PP]) than for men (AUC(ROC) estimates between 0.78 [MAP + PP in the VHM&PP] and 0.63 [PP</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.G23A0462P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.G23A0462P"><span>Bridging a possible gap of GRACE <span class="hlt">observations</span> in the Arctic Ocean using existing GRACE data and in situ bottom <span class="hlt">pressure</span> sensors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Peralta Ferriz, C.; Morison, J.</p> <p>2014-12-01</p> <p>Since 2003, the Gravity Recovery and Climate Experiment (GRACE) satellite system has provided the means of investigating month-to-month to inter-annual variability of, among many other things, Arctic Ocean circulation over the entire Arctic Basin. Such a comprehensive picture could not have been achieved with the limited in situ <span class="hlt">pressure</span> <span class="hlt">observations</span> available. Results from the first 10 years of ocean bottom <span class="hlt">pressure</span> measurements from GRACE in the Arctic Ocean reveal distinct patterns of ocean variability that are strongly associated with changes in large-scale atmospheric circulation (Peralta-Ferriz et al., 2014): the leading mode of variability being a wintertime basin-coherent mass change driven by winds in the Nordic Seas; the second mode of variability corresponding to a mass signal coherent along the Siberian shelves, and driven by the Arctic Oscillation; and the third mode being a see-saw between western and eastern Arctic shelves, also driven by the large-scale wind patterns. In order to understand Arctic Ocean changes, it is fundamental to continue to track ocean bottom <span class="hlt">pressure</span>. Our concern is what to do if the present GRACE system, which is already well beyond its design lifetime, should fail before its follow-on is launched, currently estimated to be in 2017. In this work, we regress time series of <span class="hlt">pressure</span> from the existing and potential Arctic Ocean bottom <span class="hlt">pressure</span> recorder locations against the fundamental modes of bottom <span class="hlt">pressure</span> variation. Our aim is to determine the optimum combination of in situ measurements to represent the broader scale variability now <span class="hlt">observed</span> by GRACE. With this understanding, we can be better prepared to use in situ <span class="hlt">observations</span> to at least partially cover a possible gap in GRACE coverage. Reference:Peralta-Ferriz, Cecilia, James H. Morison, John M. Wallace, Jennifer A. Bonin, Jinlun Zhang, 2014: Arctic Ocean Circulation Patterns Revealed by GRACE. J. Climate, 27, 1445-1468. doi: http://dx.doi.org/10.1175/JCLI-D-13-00013.1</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24676494','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24676494"><span>Salt-induced epithelial-to-mesenchymal transition in Dahl salt-sensitive rats is <span class="hlt">dependent</span> on elevated blood <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>Wang, Y; Mu, J J; Liu, F Q; Ren, K Y; Xiao, H Y; Yang, Z; Yuan, Z Y</p> <p>2014-02-01</p> <p>Dietary salt intake has been linked to hypertension and cardiovascular disease. Accumulating evidence has indicated that salt-sensitive individuals on high salt intake are more likely to develop renal fibrosis. Epithelial-to-mesenchymal transition (EMT) participates in the development and progression of renal fibrosis in humans and animals. The objective of this study was to investigate the impact of a high-salt diet on EMT in Dahl salt-sensitive (SS) rats. Twenty-four male SS and consomic SS-13(BN) rats were randomized to a normal diet or a high-salt diet. After 4 weeks, systolic blood <span class="hlt">pressure</span> (SBP) and albuminuria were analyzed, and renal fibrosis was histopathologically evaluated. Tubular EMT was evaluated using immunohistochemistry and real-time PCR with E-cadherin and alpha smooth muscle actin (α-SMA). After 4 weeks, SBP and albuminuria were significantly increased in the SS high-salt group compared with the normal diet group. Dietary salt intake induced renal fibrosis and tubular EMT as identified by reduced expression of E-cadherin and enhanced expression of α-SMA in SS rats. Both blood <span class="hlt">pressure</span> and renal interstitial fibrosis were negatively correlated with E-cadherin but positively correlated with α-SMA. Salt intake induced tubular EMT and renal injury in SS rats, and this relationship might <span class="hlt">depend</span> on the increase in blood <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040172696&hterms=Sex&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DSex','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040172696&hterms=Sex&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DSex"><span>Distribution and <span class="hlt">observed</span> associations of orthostatic blood <span class="hlt">pressure</span> changes in elderly general medicine outpatients</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Robertson, D.; DesJardin, J. A.; Lichtenstein, M. J.</p> <p>1998-01-01</p> <p>Factors associated with orthostatic blood <span class="hlt">pressure</span> change in elderly outpatients were determined by surveying 398 medical clinical outpatients aged 65 years and older. Blood <span class="hlt">pressure</span> was measured with random-zero sphygmomanometers after patients were 5 minutes in a supine and 5 minutes in a standing position. Orthostatic blood <span class="hlt">pressure</span> changes were at normally distributed levels with systolic and diastolic <span class="hlt">pressures</span> dropping an average of 4 mm Hg (standard deviation [SD]=15 mm Hg) and 2 mm Hg (SD=11 mm Hg), respectively. Orthostatic blood <span class="hlt">pressure</span> changes were unassociated with age, race, sex, body mass, time since eating, symptoms, or other factors. According to multiple linear regression analysis, supine systolic <span class="hlt">pressure</span>, chronic obstructive pulmonary disease (COPD), and diabetes mellitus were associated with a decrease in systolic <span class="hlt">pressure</span> on standing. Hypertension, antiarthritic drugs, and abnormal heartbeat were associated with an increase in systolic <span class="hlt">pressure</span> on standing. For orthostatic diastolic <span class="hlt">pressure</span> changes, supine diastolic <span class="hlt">pressure</span> and COPD were associated with a decrease in diastolic <span class="hlt">pressure</span> on standing. Congestive heart failure was associated with an increase in standing diastolic <span class="hlt">pressure</span>. Using logistic regression analysis, only supine systolic <span class="hlt">pressure</span> was associated with a greater than 20-mm Hg drop in systolic <span class="hlt">pressure</span> (n=53, prevalence=13%). Supine diastolic <span class="hlt">pressure</span> and COPD were the only variables associated with a greater than 20-mm Hg drop in diastolic <span class="hlt">pressure</span> (n=16, prevalence=4%). These factors may help physicians in identifying older persons at risk for having orthostatic hypotension.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1291220-multi-satellite-simultaneous-observations-magnetopause-atmospheric-losses-radiation-belt-electrons-during-intense-solar-wind-dynamic-pressure-pulse','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1291220-multi-satellite-simultaneous-observations-magnetopause-atmospheric-losses-radiation-belt-electrons-during-intense-solar-wind-dynamic-pressure-pulse"><span>Multi-satellite simultaneous <span class="hlt">observations</span> of magnetopause and atmospheric losses of radiation belt electrons during an intense solar wind dynamic <span class="hlt">pressure</span> pulse</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Xiang, Zheng; Ni, Binbin; Zhou, Chen; ...</p> <p>2016-05-03</p> <p>Radiation belt electron flux dropouts are a kind of drastic variation in the Earth's magnetosphere, understanding of which is of both scientific and societal importance. We report multi-satellite simultaneous <span class="hlt">observations</span> of magnetopause and atmospheric losses of radiation belt electrons during an event of intense solar wind dynamic <span class="hlt">pressure</span> pulse, using electron flux data from a group of 14 satellites. Moreover, when the pulse occurred, magnetopause and atmospheric loss could take effect concurrently contributing to the electron flux dropout. Losses through the magnetopause were <span class="hlt">observed</span> to be efficient and significant at L ≳ 5, owing to the magnetopause intrusion into Lmore » ~6 and outward radial diffusion associated with sharp negative gradient in electron phase space density. Losses to the atmosphere were directly identified from the precipitating electron flux <span class="hlt">observations</span>, for which pitch angle scattering by plasma waves could be mainly responsible. While the convection and substorm injections strongly enhanced the energetic electron fluxes up to hundreds of keV, they could delay other than avoid the occurrence of electron flux dropout at these energies. Finally, we demonstrate that the pulse-time radiation belt electron flux dropout <span class="hlt">depends</span> strongly on the specific interplanetary and magnetospheric conditions and that losses through the magnetopause and to the atmosphere and enhancements of substorm injection play an essential role in combination, which should be incorporated as a whole into future simulations for comprehending the nature of radiation belt electron flux dropouts.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016NatSR...627317Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016NatSR...627317Y"><span>Universal amorphous-amorphous transition in GexSe100-x glasses 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>Yildirim, Can; Micoulaut, Matthieu; Boolchand, Punit; Kantor, Innokenty; Mathon, Olivier; Gaspard, Jean-Pierre; Irifune, Tetsuo; Raty, Jean-Yves</p> <p>2016-06-01</p> <p><span class="hlt">Pressure</span> induced structural modifications in vitreous GexSe100-x (where 10 ≤ x ≤ 25) are investigated using X-ray absorption spectroscopy (XAS) along with supplementary X-ray diffraction (XRD) experiments and ab initio molecular dynamics (AIMD) simulations. Universal changes in distances and angle distributions are <span class="hlt">observed</span> when scaled to reduced densities. All compositions are <span class="hlt">observed</span> to remain amorphous under <span class="hlt">pressure</span> values up to 42 GPa. The Ge-Se interatomic distances extracted from XAS data show a two-step response to the applied <span class="hlt">pressure</span>; a gradual decrease followed by an increase at around 15-20 GPa, <span class="hlt">depending</span> on the composition. This increase is attributed to the metallization event that can be traced with the red shift in Ge K edge energy which is also identified by the principal peak position of the structure factor. The densification mechanisms are studied in details by means of AIMD simulations and compared to the experimental results. The evolution of bond angle distributions, interatomic distances and coordination numbers are examined and lead to similar <span class="hlt">pressure</span>-induced structural changes for any composition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030053447&hterms=balance+sheet&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dbalance%2Bsheet','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030053447&hterms=balance+sheet&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dbalance%2Bsheet"><span>Relation between <span class="hlt">Pressure</span> Balance Structures and Polar Plumes from Ulysses High Latitude <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yamauchi, Yohei; Suess, Steven T.; Sakurai, Takashi</p> <p>2002-01-01</p> <p>Ulysses <span class="hlt">observations</span> have shown that <span class="hlt">pressure</span> balance structures (PBSs) are a common feature in high-latitude, fast solar wind near solar minimum. Previous studies of Ulysses/SWOOPS plasma data suggest these PBSs may be remnants of coronal polar plumes. Here we find support for this suggestion in an analysis of PBS magnetic structure. We used Ulysses magnetometer data and applied a minimum variance analysis to magnetic discontinuities in PBSs. We found that PBSs preferentially contain tangential discontinuities, as opposed to rotational discontinuities and to non-PBS regions in the solar wind. This suggests that PBSs contain structures like current sheets or plasmoids that may be associated with network activity at the base of plumes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhPl...25b3503Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhPl...25b3503Z"><span><span class="hlt">Pressure</span> <span class="hlt">dependence</span> of an ion beam accelerating structure in an expanding helicon plasma</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Xiao; Aguirre, Evan; Thompson, Derek S.; McKee, John; Henriquez, Miguel; Scime, Earl E.</p> <p>2018-02-01</p> <p>We present measurements of the parallel ion velocity distribution function and electric field in an expanding helicon source plasma plume as a function of downstream gas <span class="hlt">pressure</span> and radial and axial positions. The ion beam that appears spontaneously in the plume persists for all downstream <span class="hlt">pressures</span> investigated, with the largest parallel ion beam velocities obtained for the lowest downstream <span class="hlt">pressures</span>. However, the change in ion beam velocity exceeds what would be expected simply for a change in the collisionality of the system. Electric field measurements confirm that it is the magnitude of the potential structure responsible for accelerating the ion beam that changes with downstream <span class="hlt">pressure</span>. Interestingly, the ion density radial profile is hollow close to the end of the plasma source for all <span class="hlt">pressures</span>, but it is hollow at downstream distances far from the source only at the highest downstream neutral <span class="hlt">pressures</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120001479','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120001479"><span>Time-Frequency Analysis of Rocket Nozzle Wall <span class="hlt">Pressures</span> During Start-up Transients</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Baars, Woutijn J.; Tinney, Charles E.; Ruf, Joseph H.</p> <p>2011-01-01</p> <p>Surveys of the fluctuating wall <span class="hlt">pressure</span> were conducted on a sub-scale, thrust- optimized parabolic nozzle in order to develop a physical intuition for its Fourier-azimuthal mode behavior during fixed and transient start-up conditions. These unsteady signatures are driven by shock wave turbulent boundary layer interactions which <span class="hlt">depend</span> on the nozzle <span class="hlt">pressure</span> ratio and nozzle geometry. The focus however, is on the degree of similarity between the spectral footprints of these modes obtained from transient start-ups as opposed to a sequence of fixed nozzle <span class="hlt">pressure</span> ratio conditions. For the latter, statistically converged spectra are computed using conventional Fourier analyses techniques, whereas the former are investigated by way of time-frequency analysis. The findings suggest that at low nozzle <span class="hlt">pressure</span> ratios -- where the flow resides in a Free Shock Separation state -- strong spectral similarities occur between fixed and transient conditions. Conversely, at higher nozzle <span class="hlt">pressure</span> ratios -- where the flow resides in Restricted Shock Separation -- stark differences are <span class="hlt">observed</span> between the fixed and transient conditions and <span class="hlt">depends</span> greatly on the ramping rate of the transient period. And so, it appears that an understanding of the dynamics during transient start-up conditions cannot be furnished by a way of fixed flow analysis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940000069&hterms=whitmore&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dwhitmore','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940000069&hterms=whitmore&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dwhitmore"><span>Estimating Fluctuating <span class="hlt">Pressures</span> From Distorted Measurements</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.; Leondes, Cornelius T.</p> <p>1994-01-01</p> <p>Two algorithms extract estimates of time-<span class="hlt">dependent</span> input (upstream) <span class="hlt">pressures</span> from outputs of <span class="hlt">pressure</span> sensors located at downstream ends of pneumatic tubes. Effect deconvolutions that account for distoring effects of tube upon <span class="hlt">pressure</span> signal. Distortion of <span class="hlt">pressure</span> measurements by pneumatic tubes also discussed in "Distortion of <span class="hlt">Pressure</span> Signals in Pneumatic Tubes," (ARC-12868). Varying input <span class="hlt">pressure</span> estimated from measured time-varying output <span class="hlt">pressure</span> by one of two deconvolution algorithms that take account of measurement noise. Algorithms based on minimum-covariance (Kalman filtering) theory.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011JPCM...23A5901S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011JPCM...23A5901S"><span>High <span class="hlt">pressure</span> ferroelastic phase transition in SrTiO3</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Salje, E. K. H.; Guennou, M.; Bouvier, P.; Carpenter, M. A.; Kreisel, J.</p> <p>2011-07-01</p> <p>High <span class="hlt">pressure</span> measurements of the ferroelastic phase transition of SrTiO3 (Guennou et al 2010 Phys. Rev. B 81 054115) showed a linear <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the transition temperature between the cubic and tetragonal phase. Furthermore, the <span class="hlt">pressure</span> induced transition becomes second order while the temperature <span class="hlt">dependent</span> transition is near a tricritical point. The phase transition mechanism is characterized by the elongation and tilt of the TiO6 octahedra in the tetragonal phase, which leads to strongly nonlinear couplings between the structural order parameter, the volume strain and the applied <span class="hlt">pressure</span>. The phase diagram is derived from the Clausius-Clapeyron relationship and is directly related to a <span class="hlt">pressure</span> <span class="hlt">dependent</span> Landau potential. The nonlinearities of the <span class="hlt">pressure</span> <span class="hlt">dependent</span> strains lead to an increase of the fourth order Landau coefficient with increasing <span class="hlt">pressure</span> and, hence, to a tricritical-second order crossover. This behaviour is reminiscent of the doping related crossover in isostructural KMnF3.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730002206','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730002206"><span>Effects of experimentally measured <span class="hlt">pressure</span> oscillations on the vibration of a solid rocket motor</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schoenster, J. A.; Pierce, H. B.</p> <p>1972-01-01</p> <p>Results are presented of firing a Nike rocket against a backstop for the purpose of obtaining <span class="hlt">pressure</span> fluctuations in the rocket case and determining their relationship to structural vibrations of the case. Special care was required to obtain these <span class="hlt">pressure</span> fluctuations because of the much higher static <span class="hlt">pressure</span> generated in the rocket. Very small <span class="hlt">pressure</span> fluctuations within the rocket case can cause significant vibration levels. A previously <span class="hlt">observed</span> high frequency was shown to decrease with time before completely disappearing at about 1 second of burning time. The vibration of the case itself is probably related to the longitudinal structural modes at frequencies below 500 Hz and is <span class="hlt">dependent</span> on local structural conditions at frequencies above this value.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010HyInt.197..135H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010HyInt.197..135H"><span>Crystallographic and magnetic structure of HAVAR under high-<span class="hlt">pressure</span> using diamond anvil cell (DAC)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Halevy, Itzhak; Haroush, Shlomo; Eisen, Yosef; Silberman, Ido; Moreno, Dany; Hen, Amir; Winterrose, Mike L.; Ghose, Sanjit; Chen, Zhiqiang</p> <p>2010-04-01</p> <p>Annealed (H1) and cold-rolled (H2) HAVAR has been studied using high-<span class="hlt">pressure</span> synchrotron X-ray diffraction. A structural phase transformation was discovered at ˜13 GPa at ambient temperature, transforming from m - 3 m (S.G. 225) to P 63/m m c (S.G. 194) symmetry. The transition was not reversible on <span class="hlt">pressure</span> release. The low-<span class="hlt">pressure</span> cubic phase was found to be more compressible than the high-<span class="hlt">pressure</span> hexagonal phase. Conventional Mössbauer and NFS shows that the HAVAR is not magnetic at room temperature and no splitting is <span class="hlt">observed</span>. The SQUID indicates a huge difference in the temperature <span class="hlt">dependence</span> of the magnetic susceptibility between the cold Rolled HAVAR compared to the annealed HAVAR.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhD...51t5601B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhD...51t5601B"><span>Electroviscous effect and electrokinetic energy conversion in time periodic <span class="hlt">pressure</span>-driven flow through a parallel-plate nanochannel with surface charge-<span class="hlt">dependent</span> slip</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Buren, Mandula; Jian, Yongjun; Zhao, Yingchun; Chang, Long</p> <p>2018-05-01</p> <p>In this paper we analytically investigate the electroviscous effect and electrokinetic energy conversion in the time periodic <span class="hlt">pressure</span>-driven flow of an incompressible viscous Newtonian liquid through a parallel-plate nanochannel with surface charge-<span class="hlt">dependent</span> slip. Analytical and semi-analytical solutions for electric potential, velocity and streaming electric field are obtained and are utilized to compute electrokinetic energy conversion efficiency. The results show that velocity amplitude and energy conversion efficiency are reduced when the effect of surface charge on slip length is considered. The surface charge effect increases with zeta potential and ionic concentration. In addition, the energy conversion efficiency is large when the ratio of channel half-height to the electric double layer thickness is small. The boundary slip results in a large increase in energy conversion. Higher values of the frequency of <span class="hlt">pressure</span> pulsation lead to higher values of the energy conversion efficiency. We also obtain the energy conversion efficiency in constant <span class="hlt">pressure</span>-driven flow and find that the energy conversion efficiency in periodical <span class="hlt">pressure</span>-driven flow becomes larger than that in constant <span class="hlt">pressure</span>-driven flow when the frequency is large enough.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26285002','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26285002"><span>Combined <span class="hlt">pressure</span> and cosolvent effects on enzyme activity - a high-<span class="hlt">pressure</span> stopped-flow kinetic study on α-chymotrypsin.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Luong, Trung Quan; Winter, Roland</p> <p>2015-09-21</p> <p>We investigated the combined effects of cosolvents and <span class="hlt">pressure</span> on the hydrolysis of a model peptide catalysed by α-chymotrypsin. The enzymatic activity was measured in the <span class="hlt">pressure</span> range from 0.1 to 200 MPa using a high-<span class="hlt">pressure</span> stopped-flow systems with 10 ms time resolution. A kosmotropic (trimethalymine-N-oxide, TMAO) and chaotropic (urea) cosolvent and mixtures thereof were used as cosolvents. High <span class="hlt">pressure</span> enhances the hydrolysis rate as a consequence of a negative activation volume, ΔV(#), which, <span class="hlt">depending</span> on the cosolvent system, amounts to -2 to -4 mL mol(-1). A more negative activation volume can be explained by a smaller compression of the ES complex relative to the transition state. Kinetic constants, such as kcat and the Michaelis constant KM, were determined for all solution conditions as a function of <span class="hlt">pressure</span>. With increasing <span class="hlt">pressure</span>, kcat increases by about 35% and its <span class="hlt">pressure</span> <span class="hlt">dependence</span> by a factor of 1.9 upon addition of 2 M urea, whereas 1 M TMAO has no significant effect on kcat and its <span class="hlt">pressure</span> <span class="hlt">dependence</span>. Similarly, KM increases upon addition of urea 6-fold. Addition of TMAO compensates the urea-effect on kcat and KM to some extent. The maximum rate of the enzymatic reaction increases with increasing <span class="hlt">pressure</span> in all solutions except in the TMAO : urea 1 : 2 mixture, where, remarkably, <span class="hlt">pressure</span> is found to have no effect on the rate of the enzymatic reaction anymore. Our data clearly show that compatible solutes can easily override deleterious effects of harsh environmental conditions, such as high hydrostatic <span class="hlt">pressures</span> in the 100 MPa range, which is the maximum <span class="hlt">pressure</span> encountered in the deep biosphere on Earth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22490788-pressure-induced-kinetics-transition-zirconium','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22490788-pressure-induced-kinetics-transition-zirconium"><span><span class="hlt">Pressure</span>-induced kinetics of the α to ω transition in zirconium</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>Jacobsen, M. K.; Velisavljevic, N., E-mail: nenad@lanl.gov; Sinogeikin, S. V.</p> <p></p> <p>Diamond anvil cells (DAC) coupled with x-ray diffraction (XRD) measurements are one of the primary techniques for investigating structural stability of materials at high <span class="hlt">pressure</span>-temperature (P-T) conditions. DAC-XRD has been predominantly used to resolve structural information at set P-T conditions and, consequently, provides P-T phase diagram information on a broad range of materials. With advances in large scale synchrotron x-ray facilities and corresponding x-ray diagnostic capabilities, it is now becoming possible to perform sub-second time resolved measurements on micron sized DAC samples. As a result, there is an opportunity to gain valuable information about the kinetics of structural phase transformationsmore » and extend our understanding of material behavior at high P-T conditions. Using DAC-XRD time resolved measurements, we have investigated the kinetics of the α to ω transformation in zirconium. We <span class="hlt">observe</span> a clear time and <span class="hlt">pressure</span> <span class="hlt">dependence</span> in the martensitic α-ω transition as a function of <span class="hlt">pressure</span>-jump, i.e., drive <span class="hlt">pressure</span>. The resulting data are fit using available kinetics models, which can provide further insight into transformation mechanism that influence transformation kinetics. Our results help shed light on the discrepancies <span class="hlt">observed</span> in previous measurements of the α-ω transition <span class="hlt">pressure</span> in zirconium.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1209152-pressure-induced-kinetics-transition-zirconium','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1209152-pressure-induced-kinetics-transition-zirconium"><span><span class="hlt">Pressure</span>-induced kinetics of the α to ω transition in zirconium</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Jacobsen, M. K.; Velisavljevic, N.; Sinogeikin, S. V.</p> <p>2015-07-13</p> <p>Diamond anvil cells (DAC) coupled with x-ray diffraction (XRD) measurements are one of the primary techniques for investigating structural stability of materials at high <span class="hlt">pressure</span>-temperature (P-T) conditions. DAC-XRD has been predominantly used to resolve structural information at set P-T conditions and, consequently, provides P-T phase diagram information on a broad range of materials. With advances in large scale synchrotron x-ray facilities and corresponding x-ray diagnostic capabilities, it is now becoming possible to perform sub-second time resolved measurements on micron sized DAC samples. As a result, there is an opportunity to gain valuable information about the kinetics of structural phase transformationsmore » and extend our understanding of material behavior at high P-T conditions. Using DAC-XRD time resolved measurements, we have investigated the kinetics of the α to ω transformation in zirconium. We <span class="hlt">observe</span> a clear time and <span class="hlt">pressure</span> <span class="hlt">dependence</span> in the martensitic α-ω transition as a function of <span class="hlt">pressure</span>-jump, i.e., drive <span class="hlt">pressure</span>. The resulting data are fit using available kinetics models, which can provide further insight into transformation mechanism that influence transformation kinetics. Our results help shed light on the discrepancies <span class="hlt">observed</span> in previous measurements of the α-ω transition <span class="hlt">pressure</span> in zirconium.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSM11A2136M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSM11A2136M"><span>The Role of Convection in the Buildup of the Ring Current <span class="hlt">Pressure</span> during the March 17, 2013 Storm</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Menz, A.; Kistler, L. M.; Mouikis, C.; Spence, H. E.; Skoug, R. M.; Funsten, H. O.; Larsen, B.; Mitchell, D. G.; Gkioulidou, M.; Lanzerotti, L. J.</p> <p>2016-12-01</p> <p>On March 17, 2013, the Van Allen Probes, with their apogee 1 hour post-midnight, measured the H+ and O+ fluxes of ring current during a large geomagnetic storm. Detailed examination of the <span class="hlt">pressure</span> build-up during the storm shows that there can be large differences in the <span class="hlt">pressure</span> measured by the two spacecraft with measurements separated by only an hour, and large differences in the <span class="hlt">pressure</span> measured at different local times. In addition, while the H+ and O+ <span class="hlt">pressure</span> contributions are about equal during the main phase in the near-earth plasma sheet outside L=5.5, the O+ <span class="hlt">pressure</span> becomes dominant at lower L-values. We test whether adiabatic convective transport from the near earth plasma sheet (L>5.5) to the inner magnetosphere can explain these <span class="hlt">observations</span> by comparing the <span class="hlt">observed</span> inner magnetospheric distributions with the source distribution at constant magnetic moment, mu. We find that adiabatic convection can account for the enhanced <span class="hlt">pressure</span> <span class="hlt">observed</span> during the storm. Using a Weimer '96 electric field we model the drift trajectories to show that the key features can be explained by the drift of a changing source population and energy and L-shell <span class="hlt">dependent</span> access and drift times. Finally, we show that the dominance of O+ at low L-shells is due partly to a plasma sheet source that is preferentially enhanced in O+ at lower energies (5-10 keV) and partly due to the time <span class="hlt">dependence</span> in the source, combined with the longer drift times to low L-shells. No source of O+ inside L=5.5 is required.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19827806','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19827806"><span><span class="hlt">Pressure-dependent</span> decomposition kinetics of the energetic material HMX up to 3.6 GPa.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Glascoe, Elizabeth A; Zaug, Joseph M; Burnham, Alan K</p> <p>2009-12-03</p> <p>The effect of <span class="hlt">pressure</span> on the global thermal decomposition rate of the energetic material HMX was studied. HMX was precompressed in a diamond anvil cell (DAC) and heated at various rates. The parent species population was monitored as a function of time and temperature using Fourier transform infrared (FTIR) spectroscopy. Global decomposition rates were determined by fitting the fraction reacted to the extended-Prout-Tompkins nucleation-growth model and the Friedman isoconversional method. The results of these experiments and analysis indicate that <span class="hlt">pressure</span> accelerates the decomposition at low-to-moderate <span class="hlt">pressures</span> (i.e., between ambient <span class="hlt">pressure</span> and 0.1 GPa) and decelerates the decomposition at higher <span class="hlt">pressures</span>. The decomposition acceleration is attributed to <span class="hlt">pressure</span>-enhanced autocatalysis, whereas the deceleration at high <span class="hlt">pressures</span> is attributed to <span class="hlt">pressure</span>-inhibiting bond homolysis step(s), which would result in an increase in volume. These results indicate that both the beta- and delta-polymorphs of HMX are sensitive to <span class="hlt">pressure</span> in the thermally induced decomposition kinetics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730011862','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730011862"><span>Quantitative <span class="hlt">observations</span> of hydrogen-induced, slow crack growth in a low alloy steel</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nelson, H. G.; Williams, D. P.</p> <p>1973-01-01</p> <p>Hydrogen-induced slow crack growth, da/dt, was studied in AISI-SAE 4130 low alloy steel in gaseous hydrogen and distilled water environments as a function of applied stress intensity, K, at various temperatures, hydrogen <span class="hlt">pressures</span>, and alloy strength levels. At low values of K, da/dt was found to exhibit a strong exponential K <span class="hlt">dependence</span> (Stage 1 growth) in both hydrogen and water. At intermediate values of K, da/dt exhibited a small but finite K <span class="hlt">dependence</span> (Stage 2), with the Stage 2 slope being greater in hydrogen than in water. In hydrogen, at a constant K, (da/dt) sub 2 varied inversely with alloy strength level and varied essentially in the same complex manner with temperature and hydrogen <span class="hlt">pressure</span> as noted previously. The results of this study provide support for most of the qualitative predictions of the lattice decohesion theory as recently modified by Oriani. The lack of quantitative agreement between data and theory and the inability of theory to explain the <span class="hlt">observed</span> <span class="hlt">pressure</span> <span class="hlt">dependence</span> of slow crack growth are mentioned and possible rationalizations to account for these differences are presented.</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('https://www.osti.gov/biblio/1417380-pressure-induced-polymorphic-optical-electronic-transitions-formamidinium-lead-iodide-perovskite','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1417380-pressure-induced-polymorphic-optical-electronic-transitions-formamidinium-lead-iodide-perovskite"><span><span class="hlt">Pressure</span>-Induced Polymorphic, Optical, and Electronic Transitions of Formamidinium Lead Iodide Perovskite</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>Wang, Pan; Guan, Jiwen; Galeschuk, Draven T. K.</p> <p>2017-04-28</p> <p>Formamidinium lead iodide (FAPbI3) perovskite as a superior solar cell material was investigated in two polymorphs at high <span class="hlt">pressures</span> using in situ synchrotron X-ray diffraction, FTIR spectroscopy, photoluminescence (PL) spectroscopy, electrical conductivity (EC) measurements, and ab initio calculations. We identified two new structures (i.e., Imm2 and Immm) for α-FAPbI3 but only a structural distortion (in C2/c) for δ-FAPbI3 upon compression. A <span class="hlt">pressure</span>-enhanced hydrogen bond plays a prominent role in structural modifications, as corroborated by FTIR spectroscopy. PL measurements and calculations consistently show the structure and <span class="hlt">pressure</span> <span class="hlt">dependences</span> of the band gap energies. Finally, EC measurements reveal drastically different transport propertiesmore » of α- and δ-FAPbI3 at low <span class="hlt">pressures</span> but a common trend to metallic states at high <span class="hlt">pressures</span>. All of these <span class="hlt">observations</span> suggest strongly contrasting structural stabilities and <span class="hlt">pressure</span>-tuned optoelectric properties of the two FAPbI3 polymorphs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA538038','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA538038"><span><span class="hlt">Observation</span> of an Ultrahard Phase of Graphite Quenched from High-<span class="hlt">pressure</span></span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2011-02-01</p> <p>Polycrystalline NaCl at High <span class="hlt">Pressures</span> and 300 °K. J. Geophys. Res. 1978, 83, 1257–1268. 23. Selvi , E.; Ma, Y.; Askoy, R.; Ertas, A.; White, A. High...<span class="hlt">Pressure</span> X-ray Diffraction Study of Tungsten Disulfide. J. Phys. Chem. Solids 2006, 67, 2183–2186. 24. Askoy, R.; Ma, Y.; Selvi , E.; Chyu, M. C</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.T51E0530F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.T51E0530F"><span>Evaluating the use of seafloor <span class="hlt">pressure</span> data for the study of slow slip earthquakes; insights from the 2011-2015 Cascadia Initiative deployment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fredrickson, E. K.; Wilcock, W. S. D.; MacCready, P.; Roland, E. C.; Schmidt, D. A.; Zumberge, M. A.; Sasagawa, G. S.; Kurapov, A. L.</p> <p>2017-12-01</p> <p>The Cascadia subduction zone produces M8-9 megathrust earthquakes with a recurrence interval of 500 years. While land-based geodetic measurements indicate a large degree of locking offshore, these <span class="hlt">observations</span> cannot resolve the extent of locking nearest the trench. One method for detecting displacement at shallow depths on the megathrust is through the use of seafloor <span class="hlt">pressure</span> to track uplift and subsidence of the seafloor, a technique that shows potential for both constraining long term plate locking behavior and searching for slow slip transients. Past studies using seafloor <span class="hlt">pressure</span> for geodesy have used differenced pairs of <span class="hlt">pressure</span> records to eliminate oceanographic noise, a primary noise source of seafloor <span class="hlt">pressure</span>, on the assumption that oceanographic signals are uniform between stations. These studies have identified vertical displacements associated with slow slip on the order of 1-5 cm over instrument separations from 1-50 km in subduction zone settings across the globe. We present an analysis of <span class="hlt">pressure</span> records from 30 stations in the 2011-2015 Cascadia Initiative experiment and regional physical oceanographic hind cast models developed using the Regional Ocean Modeling System, which have been validated with oceanographic <span class="hlt">observations</span>, but not previously analyzed for seafloor <span class="hlt">pressure</span>. We study the root mean square (RMS) amplitude of time series of <span class="hlt">pressure</span> and <span class="hlt">pressure</span> differences at periods of 5-30 days to assess the scale, spatial <span class="hlt">dependence</span>, and temporal <span class="hlt">dependence</span> of seafloor <span class="hlt">pressure</span> oceanographic signals. The results indicate that these signals are strongly depth <span class="hlt">dependent</span>, with filtered <span class="hlt">pressure</span> RMS values decreasing with depth from >4.5 cm on the continental shelf to <1.5 cm on the abyssal plane for the <span class="hlt">pressure</span> <span class="hlt">observations</span> and from >2.5 cm to <1 cm for the model. In contrast, oceanographic signals vary more slowly along depth contours and both data and model show RMS values varying <1 cm at separations >100 km. Based on our noise analysis</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH51D2534R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH51D2534R"><span>Determining the Dimensions of the Heliosphere from the Time-Correlation of IBEX ENA <span class="hlt">Observations</span> with Variations in the Solar Wind Dynamic <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>Reisenfeld, D. B.; Bzowski, M.; Funsten, H. O.; Janzen, P. H.; Kubiak, M. A.; McComas, D. J.; Schwadron, N.; Sokol, J. M.</p> <p>2017-12-01</p> <p>The IBEX mission has shown that variations in the ENA flux from the outer heliosphere are associated with the solar cycle. In particular, there is a good correlation between the dynamic <span class="hlt">pressure</span> of the outbound solar wind and variations in the <span class="hlt">observed</span> IBEX ENA flux (McComas et al, 2017; Reisenfeld et al., 2016). There is, of course, a time difference between <span class="hlt">observations</span> of the outbound SW and the heliospheric ENAs with which they correlate, ranging from approximately two to four years, <span class="hlt">depending</span> on ENA energy and look direction. In this study, we use this time difference as a means of "sounding" the heliosheath, that is, finding the average distance to the ENA source region in a particular direction. We use data from the first seven years of the IBEX mission. As each point in the sky is sampled once every six months, this gives us a time series of 14 points per look direction on which to time correlate. Fluxes are transformed from the spacecraft frame into a heliospheric inertial frame to remove the effects of spacecraft/Earth motion. Fluxes are also corrected for ENA extinction due to charge exchange. To improve statistics, we divide the sky into "macropixels" spanning 30 degrees in longitude and varying ranges of latitude to maintain comparable counting statistics per pixel. In calculating the response time, we account for the varying speed of the outbound solar wind by using a time and latitude <span class="hlt">dependent</span> set of solar wind speeds derived from interplanetary scintillation data (Sokol et al. 2015). Consistent with heliospheric models, we determine the shortest distance to the heliopause is in the nose direction, with a flaring toward the flanks and poles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20146357','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20146357"><span>Studying <span class="hlt">pressure</span> denaturation of a protein by molecular dynamics simulations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sarupria, Sapna; Ghosh, Tuhin; García, Angel E; Garde, Shekhar</p> <p>2010-05-15</p> <p>Many globular proteins unfold when subjected to several kilobars of hydrostatic <span class="hlt">pressure</span>. This "unfolding-up-on-squeezing" is counter-intuitive in that one expects mechanical compression of proteins with increasing <span class="hlt">pressure</span>. Molecular simulations have the potential to provide fundamental understanding of <span class="hlt">pressure</span> effects on proteins. However, the slow kinetics of unfolding, especially at high <span class="hlt">pressures</span>, eliminates the possibility of its direct <span class="hlt">observation</span> by molecular dynamics (MD) simulations. Motivated by experimental results-that <span class="hlt">pressure</span> denatured states are water-swollen, and theoretical results-that water transfer into hydrophobic contacts becomes favorable with increasing <span class="hlt">pressure</span>, we employ a water insertion method to generate unfolded states of the protein Staphylococcal Nuclease (Snase). Structural characteristics of these unfolded states-their water-swollen nature, retention of secondary structure, and overall compactness-mimic those <span class="hlt">observed</span> in experiments. Using conformations of folded and unfolded states, we calculate their partial molar volumes in MD simulations and estimate the <span class="hlt">pressure-dependent</span> free energy of unfolding. The volume of unfolding of Snase is negative (approximately -60 mL/mol at 1 bar) and is relatively insensitive to <span class="hlt">pressure</span>, leading to its unfolding in the <span class="hlt">pressure</span> range of 1500-2000 bars. Interestingly, once the protein is sufficiently water swollen, the partial molar volume of the protein appears to be insensitive to further conformational expansion or unfolding. Specifically, water-swollen structures with relatively low radii of gyration have partial molar volume that are similar to that of significantly more unfolded states. We find that the compressibility change on unfolding is negligible, consistent with experiments. We also analyze hydration shell fluctuations to comment on the hydration contributions to protein compressibility. Our study demonstrates the utility of molecular simulations in estimating volumetric properties</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3328721','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3328721"><span>Microscopic Analysis of Bacterial Motility at High <span class="hlt">Pressure</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>Nishiyama, Masayoshi; Sowa, Yoshiyuki</p> <p>2012-01-01</p> <p>The bacterial flagellar motor is a molecular machine that converts an ion flux to the rotation of a helical flagellar filament. Counterclockwise rotation of the filaments allows them to join in a bundle and propel the cell forward. Loss of motility can be caused by environmental factors such as temperature, pH, and solvation. Hydrostatic <span class="hlt">pressure</span> is also a physical inhibitor of bacterial motility, but the detailed mechanism of this inhibition is still unknown. Here, we developed a high-<span class="hlt">pressure</span> microscope that enables us to acquire high-resolution microscopic images, regardless of applied <span class="hlt">pressures</span>. We also characterized the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the motility of swimming Escherichia coli cells and the rotation of single flagellar motors. The fraction and speed of swimming cells decreased with increased <span class="hlt">pressure</span>. At 80 MPa, all cells stopped swimming and simply diffused in solution. After the release of <span class="hlt">pressure</span>, most cells immediately recovered their initial motility. Direct <span class="hlt">observation</span> of the motility of single flagellar motors revealed that at 80 MPa, the motors generate torque that should be sufficient to join rotating filaments in a bundle. The discrepancy in the behavior of free swimming cells and individual motors could be due to the applied <span class="hlt">pressure</span> inhibiting the formation of rotating filament bundles that can propel the cell body in an aqueous environment. PMID:22768943</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950053399&hterms=air+pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dair%2Bpressure','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950053399&hterms=air+pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dair%2Bpressure"><span>Temperature <span class="hlt">dependence</span> of Lorentz air-broadening and <span class="hlt">pressure</span>-shift coefficients of (12)CH4 lines in the 2.3-micron spectral region</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Devi, V. Malathy; Benner, D. Chris; Smith, M. A. H.; Rinsland, C. P.</p> <p>1994-01-01</p> <p>High-resolution (0.01/cm) absorption spectra of lean mixtures of CH4 in dry air were recorded with the McMath-Pierce Fourier transform spectrometer (FTS) of the National Solar Observatory on Kitt Peak at various temperatures between 24 and -61 C. The spectra have been analyzed to determine the values at room temperature of <span class="hlt">pressure</span>-broadened widths and <span class="hlt">pressure</span>-induced shifts of more than 740 transitions. The temperature <span class="hlt">dependence</span> of air-broadened widths and <span class="hlt">pressure</span>-induced shifts was deduced for approx. 370 transitions in the nu(sub 1) + nu(sub 4), nu(sub 3) + nu(sub 4), and nu(sub 2) + nu(sub 3) bands of (12)CH4 located between 4118 and 4615/cm. These results were obtained by analyzing a total of 29 spectra simultaneously using a multi-spectral non-linear least-squares fitting technique. This new technique allowed the determination of correlated spectral line parameters (e.g. intensity and broadening coefficient) better than the procedure of averaging values obtained by fitting the spectra individually. This method also provided a direct determination of the uncertainties in the retrieved parameters due to random errors. For each band analysed in this study the <span class="hlt">dependence</span> of the various spectral line parameters upon the tetrahedral symmetry species and the rotational quantum numbers of the transitions is also presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JCoPh.359..137M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JCoPh.359..137M"><span>A scalable variational inequality approach for flow through porous media models with <span class="hlt">pressure-dependent</span> viscosity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mapakshi, N. K.; Chang, J.; Nakshatrala, K. B.</p> <p>2018-04-01</p> <p>Mathematical models for flow through porous media typically enjoy the so-called maximum principles, which place bounds on the <span class="hlt">pressure</span> field. It is highly desirable to preserve these bounds on the <span class="hlt">pressure</span> field in predictive numerical simulations, that is, one needs to satisfy discrete maximum principles (DMP). Unfortunately, many of the existing formulations for flow through porous media models do not satisfy DMP. This paper presents a robust, scalable numerical formulation based on variational inequalities (VI), to model non-linear flows through heterogeneous, anisotropic porous media without violating DMP. VI is an optimization technique that places bounds on the numerical solutions of partial differential equations. To crystallize the ideas, a modification to Darcy equations by taking into account <span class="hlt">pressure-dependent</span> viscosity will be discretized using the lowest-order Raviart-Thomas (RT0) and Variational Multi-scale (VMS) finite element formulations. It will be shown that these formulations violate DMP, and, in fact, these violations increase with an increase in anisotropy. It will be shown that the proposed VI-based formulation provides a viable route to enforce DMP. Moreover, it will be shown that the proposed formulation is scalable, and can work with any numerical discretization and weak form. A series of numerical benchmark problems are solved to demonstrate the effects of heterogeneity, anisotropy and non-linearity on DMP violations under the two chosen formulations (RT0 and VMS), and that of non-linearity on solver convergence for the proposed VI-based formulation. Parallel scalability on modern computational platforms will be illustrated through strong-scaling studies, which will prove the efficiency of the proposed formulation in a parallel setting. Algorithmic scalability as the problem size is scaled up will be demonstrated through novel static-scaling studies. The performed static-scaling studies can serve as a guide for users to be able to select</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23092624','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23092624"><span>The time-<span class="hlt">dependent</span> accumulation of protoporphyrin IX fluorescence in nodular basal cell carcinoma following application of methyl aminolevulinate with an oxygen <span class="hlt">pressure</span> injection device.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Blake, E; Campbell, S; Allen, J; Mathew, J; Helliwell, P; Curnow, A</p> <p>2012-12-05</p> <p>Topical protoporphyrin (PpIX)-induced photodynamic therapy (PDT) relies on the penetration of the prodrug into the skin lesion and subsequent accumulation of the photosensitizer. Methyl aminolevulinate (MAL)-PDT is an established treatment for thinner and superficial non-melanoma skin cancers (NMSCs) but for the treatment of the thicker nodular basal cell carcinoma (nBCC) enhanced penetration of the prodrug is required. This study employed a new higher <span class="hlt">pressure</span>, oxygen <span class="hlt">pressure</span> injection (OPI) device, at the time of Metvix® application with a view to enhancing the penetration of MAL into the tumors. Each patient had Metvix® applied to a single nBCC followed by application of a higher <span class="hlt">pressure</span> OPI device. Following different time intervals (0, 30, 60, 120 or 180 min) the tumors were excised. The maximum depth and area of MAL penetration achieved in each lesion was measured using PpIX fluorescence microscopy. As expected, an increase in the depth of MAL-induced PpIX accumulation and area of tumor sensitized was <span class="hlt">observed</span> over time; when the Metvix® cream was applied for 0, 30, 60, 120 and 180 min the median depth of PpIX fluorescence was 0%, 21%, 26.5%, 75.5% and 90%, respectively and the median area of tumor sensitized was 0%, 4%, 6%, 19% and 60%, respectively. As the investigation presented here did not include a control arm, the relative depths of fluorescence <span class="hlt">observed</span> in this study were statistically compared (using the non-parametric Mann Whitney U test) with the results of our previous study where patients had Metvix® cream applied either with or without the standard <span class="hlt">pressure</span> OPI device. When the higher <span class="hlt">pressure</span> OPI device was employed compared to without OPI this increase was <span class="hlt">observed</span> to be greater following 30, 120, and 180 min although overall not significantly (p=0.835). In addition, no significant difference between the higher <span class="hlt">pressure</span> OPI device employed here and the previously investigated standard <span class="hlt">pressure</span> OPI device was <span class="hlt">observed</span> (p=0.403). However</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26113719','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26113719"><span>HIGH-<span class="hlt">PRESSURE</span> PHYSICS. Direct <span class="hlt">observation</span> of an abrupt insulator-to-metal transition in dense liquid deuterium.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Knudson, M D; Desjarlais, M P; Becker, A; Lemke, R W; Cochrane, K R; Savage, M E; Bliss, D E; Mattsson, T R; Redmer, R</p> <p>2015-06-26</p> <p>Eighty years ago, it was proposed that solid hydrogen would become metallic at sufficiently high density. Despite numerous investigations, this transition has not yet been experimentally <span class="hlt">observed</span>. More recently, there has been much interest in the analog of this predicted metallic transition in the dense liquid, due to its relevance to planetary science. Here, we show direct <span class="hlt">observation</span> of an abrupt insulator-to-metal transition in dense liquid deuterium. Experimental determination of the location of this transition provides a much-needed benchmark for theory and may constrain the region of hydrogen-helium immiscibility and the boundary-layer <span class="hlt">pressure</span> in standard models of the internal structure of gas-giant planets. Copyright © 2015, American Association for the Advancement of Science.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPCM...30o5403C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPCM...30o5403C"><span>Investigation of iron spin crossover <span class="hlt">pressure</span> in Fe-bearing MgO using hybrid functional</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cheng, Ya; Wang, Xianlong; Zhang, Jie; Yang, Kaishuai; Zhang, Chuanguo; Zeng, Zhi; Lin, Haiqin</p> <p>2018-04-01</p> <p><span class="hlt">Pressure</span>-induced spin crossover behaviors of Fe-bearing MgO were widely investigated by using an LDA  +  U functional for describing the strongly correlated Fe–O bonding. Moreover, the simulated spin crossover <span class="hlt">pressures</span> <span class="hlt">depend</span> on the applied U values, which are sensitive to environments and parameters. In this work, the spin crossover <span class="hlt">pressures</span> of (Mg1‑x ,Fe x )O are investigated by using the hybrid functional with a uniform parameter. Our results indicate that the spin crossover <span class="hlt">pressures</span> increase with increasing iron concentration. For example, the spin crossover <span class="hlt">pressure</span> of (Mg0.03125,Fe0.96875)O and FeO was 56 GPa and 127 GPa, respectively. The calculated crossover <span class="hlt">pressures</span> agreed well with the experimental <span class="hlt">observations</span>. Therefore, the hybrid functional should be an effective method for describing the <span class="hlt">pressure</span>-induced spin crossover behaviors in transition metal oxides.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25546675','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25546675"><span>Does the position or contact <span class="hlt">pressure</span> of the stethoscope make any difference to clinical blood <span class="hlt">pressure</span> measurements: an <span class="hlt">observational</span> study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pan, Fan; Zheng, Dingchang; He, Peiyu; Murray, Alan</p> <p>2014-12-01</p> <p>This study aimed to investigate the effect of stethoscope position and contact <span class="hlt">pressure</span> on auscultatory blood <span class="hlt">pressure</span> (BP) measurement. Thirty healthy subjects were studied. Two identical stethoscopes (one under the cuff, the other outside the cuff) were used to simultaneously and digitally record 2 channels of Korotkoff sounds during linear cuff <span class="hlt">pressure</span> deflation. For each subject, 3 measurements with different contact <span class="hlt">pressures</span> (0, 50, and 100 mm Hg) on the stethoscope outside the cuff were each recorded at 3 repeat sessions. The Korotkoff sounds were replayed twice on separate days to each of 2 experienced listeners to determine systolic and diastolic BPs (SBP and DBP). Variance analysis was performed to study the measurement repeatability and the effect of stethoscope position and contact <span class="hlt">pressure</span> on BPs. There was no significant BP difference between the 3 repeat sessions, between the 2 determinations from each listener, between the 2 listeners and between the 3 stethoscope contact <span class="hlt">pressures</span> (all P > 0.06). There was no significant SBP difference between the 2 stethoscope positions at the 2 lower stethoscope <span class="hlt">pressures</span> (P = 0.23 and 0.45), but there was a small (0.4 mm Hg, clinically unimportant) significant difference (P = 0.005) at the highest stethoscope <span class="hlt">pressure</span>. The key result was that, DBP from the stethoscope under the cuff was significantly lower than that from outside the cuff by 2.8 mm Hg (P < 0.001, 95% confidence interval -3.5 to -2.1 mm Hg). Since it is known that the traditional Korotkoff sound method, with the stethoscope outside the cuff, tends to give a higher DBP than the true intra-arterial <span class="hlt">pressure</span>, this study could suggest that the stethoscope position under the cuff, and closer to the arterial occlusion, might yield measurements closer to the actual invasive DBP.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170001222','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170001222"><span>Some <span class="hlt">Observations</span> on Damage Tolerance Analyses in <span class="hlt">Pressure</span> Vessels</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Raju, Ivatury S.; Dawicke, David S.; Hampton, Roy W.</p> <p>2017-01-01</p> <p>AIAA standards S080 and S081 are applicable for certification of metallic <span class="hlt">pressure</span> vessels (PV) and composite overwrap <span class="hlt">pressure</span> vessels (COPV), respectively. These standards require damage tolerance analyses with a minimum reliable detectible flaw/crack and demonstration of safe life four times the service life with these cracks at the worst-case location in the PVs and oriented perpendicular to the maximum principal tensile stress. The standards require consideration of semi-elliptical surface cracks in the range of aspect ratios (crack depth a to half of the surface length c, i.e., (a/c) of 0.2 to 1). NASA-STD-5009 provides the minimum reliably detectible standard crack sizes (90/95 probability of detection (POD) for several non-destructive evaluation (NDE) methods (eddy current (ET), penetrant (PT), radiography (RT) and ultrasonic (UT)) for the two limits of the aspect ratio range required by the AIAA standards. This paper tries to answer the questions: can the safe life analysis consider only the life for the crack sizes at the two required limits, or endpoints, of the (a/c) range for the NDE method used or does the analysis need to consider values within that range? What would be an appropriate method to interpolate 90/95 POD crack sizes at intermediate (a/c) values? Several procedures to develop combinations of a and c within the specified range are explored. A simple linear relationship between a and c is chosen to compare the effects of seven different approaches to determine combinations of aj and cj that are between the (a/c) endpoints. Two of the seven are selected for evaluation: Approach I, the simple linear relationship, and a more conservative option, Approach III. For each of these two Approaches, the lives are computed for initial semi-elliptic crack configurations in a plate subjected to remote tensile fatigue loading with an R-ratio of 0.1, for an assumed material evaluated using NASGRO (registered 4) version 8.1. These calculations demonstrate</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23182282','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23182282"><span>The effect of <span class="hlt">pressure</span> and mobile phase velocity on the retention properties of small analytes and large biomolecules 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>Fekete, Szabolcs; Veuthey, Jean-Luc; McCalley, David V; Guillarme, Davy</p> <p>2012-12-28</p> <p>A possible complication of ultra-high <span class="hlt">pressure</span> liquid chromatography (UHPLC) is related to the effect of <span class="hlt">pressure</span> and mobile phase velocity on the retention properties of the analytes. In the present work, numerous model compounds have been selected including small molecules, peptides, and proteins (such as monoclonal antibodies). Two instrumental setups were considered to attain elevated <span class="hlt">pressure</span> drops, firstly the use of a post-column restrictor capillary at low mobile phase flow rate (pure effect of <span class="hlt">pressure</span>) and secondly the increase of mobile phase flow rate without restrictor (i.e. a combined effect of <span class="hlt">pressure</span> and frictional heating). In both conditions, the goal was to assess differences in retention behaviour, <span class="hlt">depending</span> on the type or character of the analyte. An important conclusion is that the effect of <span class="hlt">pressure</span> and mobile phase velocity on retention varied in proportion with the size of the molecule and in some cases showed very different behaviour. In isocratic mode, the pure effect of <span class="hlt">pressure</span> (experiments with a post-column restrictor capillary) induces an increase in retention by 25-100% on small molecules (MW<300 g/mol), 150% for peptides (~1.3 kDa), 800% for insulin (~6 kDa) and up to >3000% for myoglobin (~17 kDa) for an increase in <span class="hlt">pressure</span> from 100 bar up to 1100 bar. The important effect <span class="hlt">observed</span> for the isocratic elution of proteins is probably related to conformational changes of the protein in addition to the effect of molecular size. Working in gradient elution mode, the <span class="hlt">pressure</span> related effects on retention were found to be less pronounced but still present (an increase of apparent retention factor between 0.2 and 2.5 was <span class="hlt">observed</span>). Copyright © 2012 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSM33C2527M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSM33C2527M"><span>The O+ contribution and role on the ring current <span class="hlt">pressure</span> development for CMEs and CIRs using Van Allen Probes <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mouikis, C.; Bingham, S.; Kistler, L. M.; Farrugia, C. J.; Spence, H. E.; Gkioulidou, M.</p> <p>2016-12-01</p> <p>The ring current responds differently to the different solar and interplanetary storm drivers such as coronal mass injections, (CME's), co-rotating interaction regions (CIR's), high-speed streamers and other structures. The resulting changes in the ring current particle <span class="hlt">pressure</span> change the global magnetic field, which affects the transport of the radiation belts. In order to determine the field changes during a storm, it is necessary to understand the transport, sources and losses of the particles that contribute to the ring current. The source population of the storm time ring current is the night side plasma sheet. We use Van Allen Probes <span class="hlt">observations</span> to determine the ring current <span class="hlt">pressure</span> contribution of the convecting plasma sheet H+ and O+ particles in the storm time development of the ring current. We compare storms that are related to different interplanetary drivers, CMEs and CIRs, as <span class="hlt">observed</span> at different local times. We find that during the storm main phase most of the ring current <span class="hlt">pressure</span> in the pre-midnight inner magnetosphere is contributed by particles on open drift paths that cause the development of a strong partial ring current that causes most of the main phase Dst drop. These particles can reach as deep as L 2 and their <span class="hlt">pressure</span> compares to the local magnetic field <span class="hlt">pressure</span> as deep as L 3. During the recovery phase, if these particles are not lost at the magnetopause, will become trapped and will contribute to the symmetric ring current. However, the largest difference between the CME and CIR ring current responses during the storm main and early recovery phases is caused by how the 15 - 60 keV O+ responds to these drivers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24003733','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24003733"><span>[Features of arterial blood <span class="hlt">pressure</span> in elderly persons of different ethnic groups in Yakutsk].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nikitin, Iu P; Tatarinova, O V; Neustroeva, V N; Shcherbakova, L V; Sidorov, A S</p> <p>2013-01-01</p> <p>The differences in arterial blood <span class="hlt">pressure</span> in the sample of population in the age of 60 and older of different ethnic groups in Yakutsk, as well as its connection with the other cardiovascular diseases risk factors have been analyzed. It was shown that the average values of systolic and diastolic blood <span class="hlt">pressure</span> in subsample of the Yakuts appeared to be lower than in Caucasoid gerontic persons. The average values of systolic arterial blood <span class="hlt">pressure</span> both in the Yakuts and in the Caucasoids were detected higher than normal values in all age-<span class="hlt">dependent</span> subgroups. The average values of diastolic blood <span class="hlt">pressure</span> in both ethnic groups were within the limits of high normal level. From 60 to 90 years and older the decrease in systolic and diastolic arterial blood <span class="hlt">pressure</span> was detected; it was more marked in Caucasoid gerontic persons. The average values of pulse <span class="hlt">pressure</span> in the Yakuts and in the Caucasoids appeared to be higher than the existing standard and didn't have any differences in ethnic groups. In both ethnical subsamples, pulse <span class="hlt">pressure</span> values increase was <span class="hlt">observed</span> in persons of 60-89 years old and its decrease after 90. Persons with overweight, obesity, central (abdominal) obesity, dyslypoproteidemias irrespective of belonging to ethnical group were characterized as having higher levels of arterial blood <span class="hlt">pressure</span>. Statistically significant differences in the levels of arterial blood <span class="hlt">pressure</span> in the Yakuts and in the Caucasoids <span class="hlt">depending</span> on hyperglycemia, smoking, the presence of burdened anamnesis, educational level, marital status was not detected.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23742488','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23742488"><span>Effect of <span class="hlt">pressure</span> on decoupling of ionic conductivity from structural relaxation in hydrated protic ionic liquid, lidocaine HCl.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Swiety-Pospiech, A; Wojnarowska, Z; Hensel-Bielowka, S; Pionteck, J; Paluch, M</p> <p>2013-05-28</p> <p>Broadband dielectric spectroscopy and <span class="hlt">pressure</span>-temperature-volume methods are employed to investigate the effect of hydrostatic <span class="hlt">pressure</span> on the conductivity relaxation time (τσ), both in the supercooled and glassy states of protic ionic liquid lidocaine hydrochloride monohydrate. Due to the decoupling between the ion conductivity and structural dynamics, the characteristic change in behavior of τσ(T) <span class="hlt">dependence</span>, i.e., from Vogel-Fulcher-Tammann-like to Arrhenius-like behavior, is <span class="hlt">observed</span>. This crossover is a manifestation of the liquid-glass transition of lidocaine HCl. The similar pattern of behavior was also found for <span class="hlt">pressure</span> <span class="hlt">dependent</span> isothermal measurements. However, in this case the transition from one simple volume activated law to another was noticed. Additionally, by analyzing the changes of conductivity relaxation times during isothermal densification of the sample, it was found that compression enhances the decoupling of electrical conductivity from the structural relaxation. Herein, we propose a new parameter, dlogRτ∕dP, to quantify the <span class="hlt">pressure</span> sensitivity of the decoupling phenomenon. Finally, the temperature and volume <span class="hlt">dependence</span> of τσ is discussed in terms of thermodynamic scaling concept.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018InJPh..92..731I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018InJPh..92..731I"><span><span class="hlt">Pressure</span>-induced elastic, electronic and optical properties of Ba(Mg1/3Nb2/3)O3 using first principles calculations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Islam, A. K. M. Farid Ul; Liton, M. N. H.; Anowar, M. G. M.</p> <p>2018-06-01</p> <p>The <span class="hlt">pressure</span> <span class="hlt">dependent</span> mechanical stability, electronic structure and optical properties of Ba(Mg1/3Nb2/3)O3 (BMN) perovskite have been investigated in the framework of the density functional theory. Geometry optimization shows that the BMN possesses more compressibility along c-axis. The <span class="hlt">dependency</span> of the elastic constants, the aggregated elastic moduli (B, G) and the elastic anisotropy on <span class="hlt">pressure</span> has also been studied. BMN shows brittle character at ambient <span class="hlt">pressure</span> but it becomes ductile, and also stiffer and anisotropic nature due to external <span class="hlt">pressure</span>. Electronic structure indicates the conversion of indirect to direct band gap with increasing <span class="hlt">pressure</span>. Dominated ionic character of BMN is confirmed from the bond population analysis. By analyzing the optical spectra, a red shift at the band edge is <span class="hlt">observed</span> in the visible range indicating the band gap tuning. It is seen that the static dielectric constant increases with <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.A54F..01N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.A54F..01N"><span>Further Studies of <span class="hlt">Observational</span> Undersampling of the Surface Wind and <span class="hlt">Pressure</span> Fields in the Hurricane Inner-Core</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nolan, D. S.; Klotz, B.</p> <p>2016-12-01</p> <p>Obtaining the best estimate of tropical cyclone (TC) intensity is vital for operational forecasting centers to produce accurate forecasts and to issue appropriate warnings. Aircraft data traditionally provide the most reliable information about the TC inner core and surrounding environment, but sampling strategies and <span class="hlt">observing</span> platforms associated with reconnaissance aircraft have inherent deficiencies that contribute to the uncertainty of the intensity estimate. One such instrument, the stepped frequency microwave radiometer (SFMR) on the NOAA WP-3D aircraft, provides surface wind speeds along the aircraft flight track. However, the standard "figure-4" flight pattern substantially limits the azimuthal coverage of the eyewall, such that the chance of <span class="hlt">observing</span> the true peak wind speeds is actually quite small. By simulating flights through a high-resolution simulation of Hurricane Isabel (2003), a previous study found that the 1-minute mean (maximum) SFMR winds underestimate a 6-hour running mean maximum wind (i.e. best track) by 7.5-10%. This project applies the same methodology to a suite of hurricane simulations with even higher resolution and more sophisticated physical parameterizations. These include the hurricane nature run of Nolan et al. (2013), the second hurricane nature run, a simulation of Hurricane Bill (2009), and additional idealized simulations. For the nature run cases, we find that the mean underestimate of the best-track estimate is 12-15%, considerably higher than determined from the Isabel simulation, while the other cases are similar to the previous result. Comparisons of the various cases indicates that the primary factors that lead to greater undersampling rates are storm size and storm asymmetry. Minimum surface <span class="hlt">pressure</span> is also frequently estimated from <span class="hlt">pressures</span> reported by dropsondes released into the eye, with a standard correction of 1 hPa per 10 knots of wind at the time of "splash." Statistics from thousands of simulated splash</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010ITNS...57.3694T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010ITNS...57.3694T"><span><span class="hlt">Pressure</span> Measurement Based on Thermocouples</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Thomsen, K.</p> <p>2010-12-01</p> <p>Measuring gas <span class="hlt">pressures</span> reliably in a harsh radiation environment was confirmed to be tricky during operation of the liquid spallation target of MEGAPIE at the Paul Scherrer Institute (PSI). Severe drift of calibration and the loss of a sensor were experienced. At the same time, the only instrumentation that worked flawlessly in the system were thermocouples. Motivated by this experience, a novel <span class="hlt">pressure</span> sensor for application in high radiation fields has been developed, which is based on temperature measurement. The new sensor takes advantage of the fact that the thermal conductivity over a mechanical joint exhibits a strong <span class="hlt">dependence</span> on the contact <span class="hlt">pressure</span>. In the novel sensor heating is applied at one point and temperatures are measured at different specific locations of the <span class="hlt">pressure</span> gage; in particular, the temperatures on the two sides of a mechanical contact are monitored. From the <span class="hlt">observed</span> temperature distribution the gas <span class="hlt">pressure</span> can be derived. By choosing specific mechanical details in the lay-out, it is possible to tailor the useful measurement range. In addition to yielding <span class="hlt">pressure</span> values, the new sensor concept admits for obtaining a measure for the accuracy of the result. This is done by continuous self monitoring of the device. The health status and based thereupon the plausibility of the indicated <span class="hlt">pressure</span> value can be deducted by comparing sensed temperatures to expectation values for any given heating power. Malfunctioning of the <span class="hlt">pressure</span> gage is reliably detected from the diverse readings of only one device; this can be seen as providing internal redundancy while at the same time immunity to common mode failure. After some analytical and finite element studies to verify the concept in principle, a first prototype of such a novel <span class="hlt">pressure</span> sensor has been built at PSI. Initial measurement campaigns demonstrated the correct operation of the device as anticipated. Further potential for optimization, like designing a gage for high temperature</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://www.ncbi.nlm.nih.gov/pubmed/26765007','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26765007"><span>Negative <span class="hlt">Pressure</span> Vitrification of the Isochorically Confined Liquid in Nanopores.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Adrjanowicz, K; Kaminski, K; Koperwas, K; Paluch, M</p> <p>2015-12-31</p> <p>Dielectric relaxation studies for model glass-forming liquids confined to nanoporous alumina matrices were examined together with high-<span class="hlt">pressure</span> results. For confined liquids which show the deviation from bulk dynamics upon approaching the glass transition (the change from the Vogel-Fulcher-Tammann to the Arrhenius law), we have <span class="hlt">observed</span> a striking agreement between the temperature <span class="hlt">dependence</span> of the α-relaxation time in the Arrhenius-like region and the isochoric relaxation times extrapolated from the positive range of <span class="hlt">pressure</span> to the negative <span class="hlt">pressure</span> domain. Our finding provides strong evidence that glass-forming liquid confined to native nanopores enters the isochoric conditions once the mobility of the interfacial layer becomes frozen in. This results in the negative <span class="hlt">pressure</span> effects on cooling. We also demonstrate that differences in the sensitivity of various glass-forming liquids to the "confinement effects" can be rationalized by considering the relative importance of thermal energy and density contributions in controlling the α-relaxation dynamics (the E(v)/E(p) ratio).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28488864','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28488864"><span>Temperature and <span class="hlt">Pressure</span> <span class="hlt">Dependences</span> of the Reactions of Fe+ with Methyl Halides CH3X (X = Cl, Br, I): Experiments and Kinetic Modeling Results.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ard, Shaun G; Shuman, Nicholas S; Martinez, Oscar; Keyes, Nicholas R; Viggiano, Albert A; Guo, Hua; Troe, Jürgen</p> <p>2017-06-01</p> <p>The <span class="hlt">pressure</span> and temperature <span class="hlt">dependences</span> of the reactions of Fe + with methyl halides CH 3 X (X = Cl, Br, I) in He were measured in a selected ion flow tube over the ranges 0.4 to 1.2 Torr and 300-600 K. FeX + was <span class="hlt">observed</span> for all three halides and FeCH 3 + was <span class="hlt">observed</span> for the CH 3 I reaction. FeCH 3 X + adducts (for all X) were detected in all reactions. The results were interpreted assuming two-state reactivity with spin-inversions between sextet and quartet potentials. Kinetic modeling allowed for a quantitative representation of the experiments and for extrapolation to conditions outside the experimentally accessible range. The modeling required quantum-chemical calculations of molecular parameters and detailed accounting of angular momentum effects. The results show that the FeX + products come via an insertion mechanism, while the FeCH 3 + can be produced from either insertion or S N 2 mechanisms, but the latter we conclude is unlikely at thermal energies. A statistical modeling cannot reproduce the competition between the bimolecular pathways in the CH 3 I reaction, indicating that some more direct process must be important.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007JMMM..310E.163I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007JMMM..310E.163I"><span>Unusual <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the multipolar interactions in CexLa1-xB6</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ikeda, S.; Umeo, K.; Tou, H.; Sera, M.; Iga, F.; Kunii, S.</p> <p></p> <p>We performed the mean field calculation of the magnetization under <span class="hlt">pressure</span> for the four sublattice model to understand the unusual <span class="hlt">pressure</span> effect of CeB6. The calculated results are in good agreement with the experimental results and the canted ferromagnetic ground state is predicted to appear at higher <span class="hlt">pressure</span>. We studied the electrical resistivity of Ce0.75La0.25B6 under <span class="hlt">pressure</span>. We found that the phase III is rapidly suppressed by <span class="hlt">pressure</span> and T increases with <span class="hlt">pressure</span>. At P=0.6 GPa, the direct phase transition from IV to II is found, which will be the clue to understanding the phase IV.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013APS..MARN45010J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013APS..MARN45010J"><span>Cellular <span class="hlt">pressure</span> and volume regulation and implications for cell mechanics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jiang, Hongyuan; Sun, Sean</p> <p>2013-03-01</p> <p>In eukaryotic cells, small changes in cell volume can serve as important signals for cell proliferation, death and migration. Volume and shape regulation also directly impacts the mechanics of the cell and multi-cellular tissues. Recent experiments found that during mitosis, eukaryotic cells establish a preferred steady volume and <span class="hlt">pressure</span>, and the steady volume and <span class="hlt">pressure</span> can robustly adapt to large osmotic shocks. Here we develop a mathematical model of cellular <span class="hlt">pressure</span> and volume regulation, incorporating essential elements such as water permeation, mechano-sensitive channels, active ion pumps and active stresses in the actomyosin cortex. The model can fully explain the available experimental data, and predicts the cellular volume and <span class="hlt">pressure</span> for several models of cell cortical mechanics. Furthermore, we show that when cells are subjected to an externally applied load, such as in an AFM indentation experiment, active regulation of volume and <span class="hlt">pressure</span> leads to complex cellular response. We found the cell stiffness highly <span class="hlt">depends</span> on the loading rate, which indicates the transport of water and ions might contribute to the <span class="hlt">observed</span> viscoelasticity of cells.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3754940','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3754940"><span>Glycine Insertion Makes Yellow Fluorescent Protein Sensitive to Hydrostatic <span class="hlt">Pressure</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>Watanabe, Tomonobu M.; Imada, Katsumi; Yoshizawa, Keiko; Nishiyama, Masayoshi; Kato, Chiaki; Abe, Fumiyoshi; Morikawa, Takamitsu J.; Kinoshita, Miki; Fujita, Hideaki; Yanagida, Toshio</p> <p>2013-01-01</p> <p>Fluorescent protein-based indicators for intracellular environment conditions such as pH and ion concentrations are commonly used to study the status and dynamics of living cells. Despite being an important factor in many biological processes, the development of an indicator for the physicochemical state of water, such as <span class="hlt">pressure</span>, viscosity and temperature, however, has been neglected. We here found a novel mutation that dramatically enhances the <span class="hlt">pressure</span> <span class="hlt">dependency</span> of the yellow fluorescent protein (YFP) by inserting several glycines into it. The crystal structure of the mutant showed that the tyrosine near the chromophore flipped toward the outside of the β-can structure, resulting in the entry of a few water molecules near the chromophore. In response to changes in hydrostatic <span class="hlt">pressure</span>, a spectrum shift and an intensity change of the fluorescence were <span class="hlt">observed</span>. By measuring the fluorescence of the YFP mutant, we succeeded in measuring the intracellular <span class="hlt">pressure</span> change in living cell. This study shows a new strategy of design to engineer fluorescent protein indicators to sense hydrostatic <span class="hlt">pressure</span>. PMID:24014139</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28764421','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28764421"><span>A variational data assimilation system for the range <span class="hlt">dependent</span> acoustic model using the representer method: Theoretical derivations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ngodock, Hans; Carrier, Matthew; Fabre, Josette; Zingarelli, Robert; Souopgui, Innocent</p> <p>2017-07-01</p> <p>This study presents the theoretical framework for variational data assimilation of acoustic <span class="hlt">pressure</span> <span class="hlt">observations</span> into an acoustic propagation model, namely, the range <span class="hlt">dependent</span> acoustic model (RAM). RAM uses the split-step Padé algorithm to solve the parabolic equation. The assimilation consists of minimizing a weighted least squares cost function that includes discrepancies between the model solution and the <span class="hlt">observations</span>. The minimization process, which uses the principle of variations, requires the derivation of the tangent linear and adjoint models of the RAM. The mathematical derivations are presented here, and, for the sake of brevity, a companion study presents the numerical implementation and results from the assimilation simulated acoustic <span class="hlt">pressure</span> <span class="hlt">observations</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=atmospheric+AND+pressure&pg=4&id=EJ512571','ERIC'); return false;" href="https://eric.ed.gov/?q=atmospheric+AND+pressure&pg=4&id=EJ512571"><span>Atmospheric <span class="hlt">Pressure</span> Indicator.</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>Salzsieder, John C.</p> <p>1995-01-01</p> <p>Discusses <span class="hlt">observable</span> phenomena related to air <span class="hlt">pressure</span>. Describes a simple, unobtrusive, semiquantitative device to monitor the changes in air <span class="hlt">pressure</span> that are associated with altitude, using a soft-drink bottle and a balloon. (JRH)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17652750','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17652750"><span>Regulation of choroidal blood flow during combined changes in intraocular <span class="hlt">pressure</span> and arterial blood <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>Polska, Elzbieta; Simader, Christian; Weigert, Günter; Doelemeyer, Arno; Kolodjaschna, Julia; Scharmann, Ole; Schmetterer, Leopold</p> <p>2007-08-01</p> <p>To test the hypothesis that human choroidal blood flow (ChBF) may <span class="hlt">depend</span>, not only on ocular perfusion <span class="hlt">pressure</span> (OPP), but also on absolute mean arterial <span class="hlt">pressure</span> (MAP) and intraocular <span class="hlt">pressure</span> (IOP). There were two study days in an open design. On the first day, OPP was varied by elevating IOP during a squatting-induced increase in MAP (28 subjects). On the second day, only the IOP was increased (17 subjects). IOP was raised in stepwise increments by using the suction cup Subfoveal ChBF (laser Doppler flowmetry), MAP, and IOP were assessed, and OPP was calculated as (2/3)(MAP - IOP). For correlation analysis, data from all subjects were pooled according to IOP and MAP, and correlation analyses were performed. When data from study day 1 were grouped according to IOP, no correlation was <span class="hlt">observed</span> between ChBF and MAP; but ChBFs were lower, the higher the IOP (P < 0.001). When data were grouped according to MAP, a significant correlation was found between ChBF and IOP (P < 0.001), but correlations were independent of MAP. When data of study day 2 were pooled according to IOP, a correlation between ChBF and OPP was seen only at IOP > 40 mm Hg (P < 0.05). The data confirm previously published <span class="hlt">observations</span> that the choroid shows some autoregulatory capacity during changes in OPP. In addition, the data indicate that the choroid regulates its blood flow better during exercise-induced changes in MAP than during an experimental increase in IOP.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22657898-design-principles-highpressure-force-fields-aqueous-tmao-solutions-from-ambient-kilobar-pressures','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22657898-design-principles-highpressure-force-fields-aqueous-tmao-solutions-from-ambient-kilobar-pressures"><span>Design principles for high–<span class="hlt">pressure</span> force fields: Aqueous TMAO solutions from ambient to kilobar <span class="hlt">pressures</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>Hölzl, Christoph; Horinek, Dominik, E-mail: dominik.horinek@ur.de; Kibies, Patrick</p> <p></p> <p>Accurate force fields are one of the major pillars on which successful molecular dynamics simulations of complex biomolecular processes rest. They have been optimized for ambient conditions, whereas high-<span class="hlt">pressure</span> simulations become increasingly important in <span class="hlt">pressure</span> perturbation studies, using <span class="hlt">pressure</span> as an independent thermodynamic variable. Here, we explore the design of non-polarizable force fields tailored to work well in the realm of kilobar <span class="hlt">pressures</span> – while avoiding complete reparameterization. Our key is to first compute the <span class="hlt">pressure</span>-induced electronic and structural response of a solute by combining an integral equation approach to include <span class="hlt">pressure</span> effects on solvent structure with a quantum-chemical treatmentmore » of the solute within the embedded cluster reference interaction site model (EC-RISM) framework. Next, the solute’s response to compression is taken into account by introducing <span class="hlt">pressure-dependence</span> into selected parameters of a well-established force field. In our proof-of-principle study, the full machinery is applied to N,N,N-trimethylamine-N-oxide (TMAO) in water being a potent osmolyte that counteracts <span class="hlt">pressure</span> denaturation. EC-RISM theory is shown to describe well the charge redistribution upon compression of TMAO(aq) to 10 kbar, which is then embodied in force field molecular dynamics by <span class="hlt">pressure-dependent</span> partial charges. The performance of the high <span class="hlt">pressure</span> force field is assessed by comparing to experimental and ab initio molecular dynamics data. Beyond its broad usefulness for designing non-polarizable force fields for extreme thermodynamic conditions, a good description of the <span class="hlt">pressure</span>-response of solutions is highly recommended when constructing and validating polarizable force fields.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27083705','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27083705"><span>Design principles for high-<span class="hlt">pressure</span> force fields: Aqueous TMAO solutions from ambient to kilobar <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>Hölzl, Christoph; Kibies, Patrick; Imoto, Sho; Frach, Roland; Suladze, Saba; Winter, Roland; Marx, Dominik; Horinek, Dominik; Kast, Stefan M</p> <p>2016-04-14</p> <p>Accurate force fields are one of the major pillars on which successful molecular dynamics simulations of complex biomolecular processes rest. They have been optimized for ambient conditions, whereas high-<span class="hlt">pressure</span> simulations become increasingly important in <span class="hlt">pressure</span> perturbation studies, using <span class="hlt">pressure</span> as an independent thermodynamic variable. Here, we explore the design of non-polarizable force fields tailored to work well in the realm of kilobar <span class="hlt">pressures</span>--while avoiding complete reparameterization. Our key is to first compute the <span class="hlt">pressure</span>-induced electronic and structural response of a solute by combining an integral equation approach to include <span class="hlt">pressure</span> effects on solvent structure with a quantum-chemical treatment of the solute within the embedded cluster reference interaction site model (EC-RISM) framework. Next, the solute's response to compression is taken into account by introducing <span class="hlt">pressure-dependence</span> into selected parameters of a well-established force field. In our proof-of-principle study, the full machinery is applied to N,N,N-trimethylamine-N-oxide (TMAO) in water being a potent osmolyte that counteracts <span class="hlt">pressure</span> denaturation. EC-RISM theory is shown to describe well the charge redistribution upon compression of TMAO(aq) to 10 kbar, which is then embodied in force field molecular dynamics by <span class="hlt">pressure-dependent</span> partial charges. The performance of the high <span class="hlt">pressure</span> force field is assessed by comparing to experimental and ab initio molecular dynamics data. Beyond its broad usefulness for designing non-polarizable force fields for extreme thermodynamic conditions, a good description of the <span class="hlt">pressure</span>-response of solutions is highly recommended when constructing and validating polarizable force fields.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23409919','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23409919"><span>Index of refraction, density, and solubility of ammonium iodide solutions at high <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>Lamelas, F J</p> <p>2013-03-07</p> <p>An asymmetric moissanite anvil cell is used to study aqueous solutions of ammonium iodide at <span class="hlt">pressures</span> up to 10 kbar. The index of refraction is measured using the rotating Fabry-Perot technique, with an accuracy of approximately 1%. The mass density and molar volume of the solutions are estimated using the measured index values, and the molar volume is used to predict the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the solubility. The solubility derived from the index of refraction measurements is shown to agree with that which is determined by direct <span class="hlt">observation</span> of the onset of crystallization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950012572','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950012572"><span>A preliminary analysis of low frequency <span class="hlt">pressure</span> oscillations in hybrid rocket motors</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jenkins, Rhonald M.</p> <p>1994-01-01</p> <p>Past research with hybrid rockets has suggested that certain motor operating conditions are conducive to the formation of <span class="hlt">pressure</span> oscillations, or flow instabilities, within the motor combustion chamber. These combustion-related vibrations or <span class="hlt">pressure</span> oscillations may be encountered in virtually any type of rocket motor and typically fall into three frequency ranges: low frequency oscillations (0-300 Hz); intermediate frequency oscillations (400-1000 Hz); and high frequency oscillations (greater than 1000 Hz). In general, combustion instability is characterized by organized <span class="hlt">pressure</span> oscillations occurring at well-defined intervals with <span class="hlt">pressure</span> peaks that may maintain themselves, grow, or die out. Usually, such peaks exceed +/- 5% of the mean chamber <span class="hlt">pressure</span>. For hybrid motors, these oscillations have been <span class="hlt">observed</span> to grow to a limiting amplitude which may be <span class="hlt">dependent</span> on factors such as fuel characteristics, oxidizer injector characteristics, average chamber <span class="hlt">pressure</span>, oxidizer mass flux, combustion chamber length, and grain geometry. The approach taken in the present analysis is to develop a modified chamber length, L, instability theory which accounts for the relationship between <span class="hlt">pressure</span> and oxidizer to fuel concentration ratio in the motor.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PCM....44..615S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PCM....44..615S"><span>Structural behavior of Tl-exchanged natrolite at high <span class="hlt">pressure</span> <span class="hlt">depending</span> on the composition of <span class="hlt">pressure</span>-transmitting medium</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Seryotkin, Yu. V.; Bakakin, V. V.; Likhacheva, A. Yu.; Dementiev, S. N.; Rashchenko, S. V.</p> <p>2017-10-01</p> <p>The structural evolution of Tl-exchanged natrolite with idealized formula Tl2[Al2Si3O10]·2H2O, compressed in penetrating (water:ethanol 1:1) and non-penetrating (paraffin) media, was studied up to 4 GPa. The presence of Tl+ with non-bonded electron lone pairs, which can be either stereo-chemically active or passive, determines distinctive features of the high-<span class="hlt">pressure</span> behavior of the Tl-form. The effective volume of assemblages Tl+(O,H2O) n <span class="hlt">depends</span> on the E-pairs activity: single-sided coordination correlates with smaller volumes. At ambient conditions, there are two types of Tl positions, only one of them having a nearly single-sided coordination as a characteristic of stereo-activity of the Tl+ E pair. Upon the compression in paraffin, a phase transition occurs: a 5% volume contraction of flexible natrolite framework is accompanied by the conversion of all the Tl+ cations into stereo-chemically active state with a single-sided coordination. This effect requires the reconstruction of all the extra-framework subsystems with the inversion of the cation and H2O positions. The compression in water-containing medium leads to the increase of H2O content up to three molecules pfu through the filling of partly vacant positions. This hinders a single-sided coordination of Tl ions and preserves the configuration of their ion-molecular subsystem. It is likely that the extra-framework subsystem is responsible for the super-structure modulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19960021431&hterms=jump&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Djump','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19960021431&hterms=jump&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Djump"><span>Anisotropic shock jump conditions: Theory and <span class="hlt">observations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chao, J. K.; Zhang, X. X.; Song, P.</p> <p>1995-01-01</p> <p>The MHD Rankine-Hugoniot (RH) relations for shock waves in a collisionless plasma with bi-Maxwellian distribution functions are considered. While by introducing the <span class="hlt">pressure</span> anisotropy parameter xi in the RH relations, the number of unknowns -- B, V, n, p and xi (a total of 9) -- becomes one more than the total number of the conservation equations, it is possible to use the <span class="hlt">observed</span> quantities on both sides of the shock to study the anisotropy changes across the shock. A simple relation for the anisotropy change across the shock is derived as a function of the ratio of magnetic fields m(= B'/B), the shock normal angle theta(sub Bn) and the plasma beta and beta' (primes are downstream values). Since m and theta(sub Bn) can be determined accurately in <span class="hlt">observation</span>, the reliability of the anisotropy change deduced is mostly <span class="hlt">dependent</span> on the accuracy of the measurements beta and beta'. We have applied the results to six low-beta quasi-perpendicular (Q perpendicular) laminar bow shock crossings with temperature anisotropy measured in the magnetosheath. In the six test cases, it is found that the predicted <span class="hlt">pressure</span> anisotropies agree well with those <span class="hlt">observed</span> in the magnetosheath.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29800486','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29800486"><span>Education of healthcare professionals for preventing <span class="hlt">pressure</span> ulcers.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Porter-Armstrong, Alison P; Moore, Zena Eh; Bradbury, Ian; McDonough, Suzanne</p> <p>2018-05-25</p> <p> home settings, or nursing home and hospital wards, compared to no intervention, or usual practices. Educational intervention in one of these studies was embedded within a broader, quality improvement bundle. The other two individually randomised controlled trials explored the effectiveness of educational intervention, delivered in two formats, to nursing staff cohorts.Due to the heterogeneity of the studies identified, pooling was not appropriate and we have presented a narrative overview. We explored a number of comparisons (1) education versus no education (2) components of educational intervention in a number of combinations and (3) education delivered in different formats. There were three primary outcomes: change in healthcare professionals' knowledge, change in healthcare professionals' clinical behaviour and incidence of new <span class="hlt">pressure</span> ulcers.We are uncertain whether there is a difference in health professionals' knowledge <span class="hlt">depending</span> on whether they receive education or no education on <span class="hlt">pressure</span> ulcer prevention (hospital group: mean difference (MD) 0.30, 95% confidence interval (CI) -1.00 to 1.60; 10 participants; nursing home group: MD 0.30, 95% CI -0.77 to 1.37; 10 participants). This was based on very low-certainty evidence from one study, which we downgraded for serious study limitations, indirectness and imprecision.We are uncertain whether there is a difference in <span class="hlt">pressure</span> ulcer incidence with the following comparisons: training, monitoring and <span class="hlt">observation</span>, versus monitoring and <span class="hlt">observation</span> (risk ratio (RR) 0.63, 95% CI 0.37 to 1.05; 345 participants); training, monitoring and <span class="hlt">observation</span>, versus <span class="hlt">observation</span> alone (RR 1.21, 95% CI 0.60 to 2.43; 325 participants) or, monitoring and <span class="hlt">observation</span> versus <span class="hlt">observation</span> alone (RR 1.93, 95% CI 0.96 to 3.88; 232 participants). This was based on very low-certainty evidence from one study, which we downgraded for very serious study limitations and imprecision. We are uncertain whether multilevel intervention versus</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JAP...123t4701S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JAP...123t4701S"><span>Effect of weakly ionized plasma on osmotic <span class="hlt">pressure</span> on cell membranes in a saline</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shneider, M. N.; Pekker, M.</p> <p>2018-05-01</p> <p>In this paper, attention is drawn to the importance of accounting for osmotic <span class="hlt">pressure</span> when analyzing physiological effects on cellular structures in plasma medicine. Interaction of a weakly ionized plasma jet with a saline solution leads to detectable changes in the saline's ion-molecular composition and hence changes in the osmotic <span class="hlt">pressure</span>. This, in turn, leads to a stretching or compression of the membrane, <span class="hlt">depending</span> on the difference of total external and internal <span class="hlt">pressures</span>. The selective effect of plasma on cells, <span class="hlt">observed</span> in experiments, is associated with the change in the mechanical properties of membranes (and thereby, a weakening of their protective properties). Corresponding estimates are given in the article.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.T54B..04H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.T54B..04H"><span>Permeability - Fluid <span class="hlt">Pressure</span> - Stress Relationship in Fault Zones in Shales</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Henry, P.; Guglielmi, Y.; Morereau, A.; Seguy, S.; Castilla, R.; Nussbaum, C.; Dick, P.; Durand, J.; Jaeggi, D.; Donze, F. V.; Tsopela, A.</p> <p>2016-12-01</p> <p>Fault permeability is known to <span class="hlt">depend</span> strongly on stress and fluid <span class="hlt">pressures</span>. Exponential relationships between permeability and effective <span class="hlt">pressure</span> have been proposed to approximate fault response to fluid <span class="hlt">pressure</span> variations. However, the applicability of these largely empirical laws remains questionable, as they do not take into account shear stress and shear strain. A series of experiments using mHPP probes have been performed within fault zones in very low permeability (less than 10-19 m2) Lower Jurassic shale formations at Tournemire (France) and Mont Terri (Switzerland) underground laboratories. These probes allow to monitor 3D displacement between two points anchored to the borehole walls at the same time as fluid <span class="hlt">pressure</span> and flow rate. In addition, in the Mont-Terri experiment, passive <span class="hlt">pressure</span> sensors were installed in <span class="hlt">observation</span> boreholes. Fracture transmissivity was estimated from single borehole pulse test, constant <span class="hlt">pressure</span> injection tests, and cross-hole tests. It is found that the transmissivity-<span class="hlt">pressure</span> <span class="hlt">dependency</span> can be approximated with an exponential law, but only above a <span class="hlt">pressure</span> threshold that we call the Fracture Opening Threshold (F.O.P). The displacement data show a change of the mechanical response across the F.O.P. The displacement below the F.O.P. is dominated by borehole response, which is mostly elastic. Above F.O.P., the poro-elasto-plastic response of the fractures dominates. Stress determinations based on previous work and on the analysis of slip data from mHPPP probe indicate that the F.O.P. is lower than the least principal stress. Below the F.O.P., uncemented fractures retain some permeability, as pulse tests performed at low <span class="hlt">pressures</span> yield diffusivities in the range 10-2 to 10-5 m2/s. Overall, this dual behavior appears consistent with the results of CORK experiments performed in accretionary wedge decollements. Results suggest (1) that fault zones become highly permeable when approaching the critical Coulomb threshold (2</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/24780','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/24780"><span>Advective transport of CO2 in permeable media induced by atmospheric <span class="hlt">pressure</span> fluctuations: 2. <span class="hlt">Observational</span> evidence under snowpacks</span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>W. J. Massman; J. M. Frank</p> <p>2006-01-01</p> <p>Meadow and forest CO2 amounts sampled beneath an approximately meter deep (steady state) snowpack at a subalpine site in southern Rocky Mountains of Wyoming are <span class="hlt">observed</span> to vary by nearly 200 ppm over periods ranging from 4 to 15 days. This work employs the model of periodic, <span class="hlt">pressure</span>-induced, advective transport in permeable media developed in...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.3491B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.3491B"><span>Comparisons of Fabric Strength and Development in Polycrystalline Ice at Atmospheric and Basal Hydrostatic <span class="hlt">Pressures</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Breton, Daniel; Baker, Ian; Cole, David</p> <p>2013-04-01</p> <p>Understanding and predicting the flow of polycrystalline ice is crucial to ice sheet modeling and paleoclimate reconstruction from ice cores. Ice flow rates <span class="hlt">depend</span> strongly on the fabric (i.e. the distribution of grain sizes and crystallographic orientations) which evolves over time and enhances the flow rate in the direction of applied stress. The mechanisms for fabric evolution in ice have been extensively studied at atmospheric <span class="hlt">pressures</span>, but little work has been done to <span class="hlt">observe</span> these processes at the high <span class="hlt">pressures</span> experienced deep within ice sheets where long-term changes in ice rheology are expected to have significance. We conducted compressive creep tests to ~10% strain on 917 kg m-3, initially randomly-oriented polycrystalline ice specimens at 0.1 (atmospheric) and 20 MPa (simulating ~2,000 m depth) hydrostatic <span class="hlt">pressures</span>, performing microstructural analyses on the resulting deformed specimens to characterize the evolution and strength of crystal fabric. Our microstructural analysis technique simultaneously collects grain shape and size data from Scanning Electron Microscope (SEM) micrographs and obtains crystallographic orientation data via Electron BackScatter Diffraction (EBSD). Combining these measurements allows rapid analysis of the ice fabric over large numbers of grains, yielding statistically useful numbers of grain size and orientation data. We present creep and microstructural data to demonstrate <span class="hlt">pressure-dependent</span> effects on the mechanical and microstructural evolution of polycrystalline ice and discuss possible mechanisms for the <span class="hlt">observed</span> differences.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18853700','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18853700"><span>Aerophagia and gastroesophageal reflux disease in patients using continuous positive airway <span class="hlt">pressure</span>: a preliminary <span class="hlt">observation</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Watson, Nathaniel F; Mystkowski, Sue K</p> <p>2008-10-15</p> <p>Aerophagia is a complication of continuous positive airway <span class="hlt">pressure</span> (CPAP) therapy for sleep disordered breathing (SDB), whereupon air is forced into the stomach and bowel. Associated discomfort can result in CPAP discontinuation. We hypothesize that aerophagia is associated with gastroesophageal reflux disease (GERD) via mechanisms involving GERD related lower esophageal sphincter (LES) compromise. Twenty-two subjects with aerophagia and 22 controls, matched for age, gender, and body mass index, who were being treated with CPAP for SDB were compared in regard to clinical aspects of GERD, GERD associated habits, SDB severity as measured by polysomnography, and mean CPAP <span class="hlt">pressure</span>. More subjects with aerophagia had symptoms of GERD (77.3% vs. 36.4%; p < 0.01) and were on GERD related medications (45.5% vs. 18.2%, p < 0.05) than controls. Regarding polysomnography, mean oxygen saturation percentages were lower in the aerophagia group than controls (95.0% vs. 96.5%, p < 0.05). No other differences were <span class="hlt">observed</span>, including mean CPAP <span class="hlt">pressures</span>. No one in the aerophagia group (vs. 27.3% of the control group) was a current tobacco user (p < 0.01). There was no difference in caffeine or alcohol use between the 2 groups. These results imply aerophagia is associated with GERD symptoms and GERD related medication use. This finding suggests a relationship between GERD related LES pathophysiology and the development of aerophagia in patients with SDB treated with CPAP.</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('http://adsabs.harvard.edu/abs/2017JGRA..122.9705Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRA..122.9705Z"><span>Latitude <span class="hlt">Dependence</span> of Low-Altitude O+ Ion Upflow: Statistical Results From FAST <span class="hlt">Observations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, K.; Chen, K. W.; Jiang, Y.; Chen, W. J.; Huang, L. F.; Fu, S.</p> <p>2017-09-01</p> <p>We introduce a statistical model to explain the latitudinal <span class="hlt">dependence</span> of the occurrence rate and energy flux of the ionospheric escaping ions, taking advantage of advances in the spatial coverage and accuracy of FAST <span class="hlt">observations</span>. We use a weighted piecewise Gaussian function to fit the <span class="hlt">dependence</span>, because two probability peaks are located in the dayside polar cusp source region and the nightside auroral oval zone source region. The statistical results show that (1) the Gaussian Mixture Model suitably describes the dayside polar cusp upflows, and the dayside and the nightside auroral oval zone upflows. (2) The magnetic latitudes of the ionospheric upflow source regions expand toward the magnetic equator as Kp increases, from 81° magnetic latitude (MLAT) (cusp upflows) and 63° MLAT (auroral oval upflows) during quiet times to 76° MLAT and 61° MLAT, respectively. (3) The dayside polar cusp region provides only 3-5% O+ upflows among all the source regions, which include the dayside auroral oval zone, dayside polar cusp, nightside auroral oval zone, and even the polar cap. However, <span class="hlt">observations</span> show that more than 70% of upflows occur in the auroral oval zone and that the occurrence probability increases at the altitudes of 3500-4200 km, which is considered to be the lower altitude boundary of ion beams. This <span class="hlt">observed</span> result suggests that soft electron precipitation and transverse wave heating are the most efficient ion energization/acceleration mechanisms at the altitudes of FAST orbit, and that the parallel acceleration caused by field-aligned potential drops becomes effective above that altitude.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006PhyB..383...37S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006PhyB..383...37S"><span><span class="hlt">Pressure</span> effect on the long-range order in CeB6</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sera, M.; Ikeda, S.; Iwakubo, H.; Uwatoko, Y.; Hane, S.; Kosaka, M.; Kunii, S.</p> <p>2006-08-01</p> <p>The <span class="hlt">pressure</span> effect of CeB6 was investigated. The <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the Néel temperature, TN and the critical field from the antiferro-magnetic phase III to antiferro-quadrupolar phase II, HcIII-II of CeB6 exhibits the unusual <span class="hlt">pressure</span> <span class="hlt">dependence</span> that the suppression rate of HcIII-II is much larger than that of TN. In order to explain this unusual result, we have performed the mean field calculation for the 4-sublattice model assuming that the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of TN, the antiferro-octupolar and quadrupolar temperatures, Toct and TQ as follows; dTN/dP<0, dToct/dP>dTQ/dP>0 and could explain the unusual <span class="hlt">pressure</span> <span class="hlt">dependence</span> of TN and HcIII-II.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24329369','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24329369"><span>Geometrical feature of the scaling behavior of the limit-point <span class="hlt">pressure</span> of inflated hyperelastic membranes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tamadapu, Ganesh; Dhavale, Nikhil Nandkumar; DasGupta, Anirvan</p> <p>2013-11-01</p> <p>The occurrence of the limit-point instability is an intriguing phenomenon <span class="hlt">observed</span> during stretching of hyperelastic membranes. In toy rubber balloons, this phenomenon may be experienced in the sudden reduction in the level of difficulty of blowing the balloon accompanied by its rapid inflation. The present paper brings out a link between the geometry and strain-hardening parameter of the membrane, and the occurrence of the limit-point instability. Inflation of membranes with different geometries and boundary conditions is considered, and the corresponding limit-point <span class="hlt">pressures</span> are obtained for different strain-hardening parameter values. Interestingly, it is <span class="hlt">observed</span> that the limit-point <span class="hlt">pressure</span> for the different geometries is inversely proportional to a geometric parameter of the uninflated membrane. This <span class="hlt">dependence</span> is shown analytically, which can be extended to a general membrane geometry. More surprisingly, the proportionality constant has a power-law <span class="hlt">dependence</span> on the nondimensional material strain-hardening parameter. The constants involved in the power-law relation are universal constants for a particular membrane geometry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27793545','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27793545"><span>Chronic binge alcohol consumption during pregnancy alters rat maternal uterine artery <span class="hlt">pressure</span> response.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Naik, Vishal D; Lunde-Young, Emilie R; Davis-Anderson, Katie L; Orzabal, Marcus; Ivanov, Ivan; Ramadoss, Jayanth</p> <p>2016-11-01</p> <p>We aimed to investigate <span class="hlt">pressure-dependent</span> maternal uterine artery responses and vessel remodeling following gestational binge alcohol exposure. Two groups of pregnant rats were used: the alcohol group (28.5% wt/v, 6.0 g/kg, once-daily orogastric gavage in a binge paradigm between gestational day (GD) 5-19) and pair-fed controls (isocalorically matched). On GD20, excised, <span class="hlt">pressurized</span> primary uterine arteries were studied following equilibration (60 mm Hg) using dual chamber arteriograph. The uterine artery diameter stabilized at 20 mm Hg, showed passive distension at 40 mm Hg, and redeveloped tone at 60 mm Hg. An alcohol effect (P = 0.0025) was <span class="hlt">observed</span> on the percent constriction of vessel diameter with greater <span class="hlt">pressure-dependent</span> myogenic constriction. Similar alcohol effect was noted with lumen diameter response (P = 0.0020). The percent change in media:lumen ratio was higher in the alcohol group (P < 0.0001). Thus, gestational alcohol affects <span class="hlt">pressure</span>-induced uterine artery reactivity, inward-hypotrophic remodeling, and adaptations critical for nutrient delivery to the fetus. Copyright © 2016 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25756709','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25756709"><span>A look at the effect of sequence complexity on <span class="hlt">pressure</span> destabilisation of DNA polymers.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rayan, Gamal; Macgregor, Robert B</p> <p>2015-04-01</p> <p>Our previous studies on the helix-coil transition of double-stranded DNA polymers have demonstrated that molar volume change (ΔV) accompanying the thermally-induced transition can be positive or negative <span class="hlt">depending</span> on the experimental conditions, that the <span class="hlt">pressure</span>-induced transition is more cooperative than the heat-induced transition [Rayan and Macgregor, J Phys Chem B2005, 109, 15558-15565], and that the <span class="hlt">pressure</span>-induced transition does not occur in the absence of water [Rayan and Macgregor, Biophys Chem, 2009, 144, 62-66]. Additionally, we have shown that ΔV values obtained by <span class="hlt">pressure-dependent</span> techniques differ from those obtained by ambient <span class="hlt">pressure</span> techniques such as PPC [Rayan et al. J Phys Chem B2009, 113, 1738-1742] thus shedding light on the effects of <span class="hlt">pressure</span> on DNA polymers. Herein, we examine the effect of sequence complexity, and hence cooperativity on <span class="hlt">pressure</span> destabilisation of DNA polymers. Working with Clostridium perfringes DNA under conditions such that the estimated ΔV of the helix-coil transition corresponds to -1.78 mL/mol (base pair) at atmospheric <span class="hlt">pressure</span>, we do not <span class="hlt">observe</span> the <span class="hlt">pressure</span>-induced helix-coil transition of this DNA polymer, whereas synthetic copolymers poly[d(A-T)] and poly[d(I-C)] undergo cooperative <span class="hlt">pressure</span>-induced transitions at similar ΔV values. We hypothesise that the reason for the lack of <span class="hlt">pressure</span>-induced helix-coil transition of C. perfringens DNA under these experimental conditions lies in its sequence complexity. Copyright © 2015 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1916285M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1916285M"><span>Influence of wind-induced air <span class="hlt">pressure</span> fluctuations on topsoil gas concentrations within a Scots pine forest</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mohr, Manuel; Laemmel, Thomas; Maier, Martin; Schindler, Dirk</p> <p>2017-04-01</p> <p>Commonly it is assumed that soil gas transport is dominated by molecular diffusion. Few recent studies indicate that the atmosphere above the soil triggers non-diffusive gas transport processes in the soil, which can enhance soil gas transport and therefore soil gas efflux significantly. During high wind speed conditions, the so called <span class="hlt">pressure</span> pumping effect has been <span class="hlt">observed</span>: the enhancement of soil gas transport through dynamic changes in the air <span class="hlt">pressure</span> field above the soil. However, the amplitudes and frequencies of the air <span class="hlt">pressure</span> fluctuations responsible for <span class="hlt">pressure</span> pumping are still uncertain. Moreover, an in situ <span class="hlt">observation</span> of the <span class="hlt">pressure</span> pumping effect is still missing. To investigate the <span class="hlt">pressure</span> pumping effect, airflow measurements above and below the canopy of a Scots pine forest and high-precision relative air <span class="hlt">pressure</span> measurements were conducted in the below-canopy space and in the soil over a measurement period of 16 weeks. To monitor the soil gas transport, a newly developed gas measurement system was used. The gas measurement system continuously injects helium as a tracer gas into the soil until a diffusive steady state is reached. With the steady state concentration profile of the tracer gas, it is possible to inversely model the gas diffusion coefficient profile of the soil. If the gas diffusion coefficient profile differed from steady state, we deduced that the soil gas transport is not only diffusive, but also influenced by non-diffusive processes. Results show that the occurrence of small air <span class="hlt">pressure</span> fluctuations is strongly <span class="hlt">dependent</span> on the mean above-canopy wind speed. The wind-induced air <span class="hlt">pressure</span> fluctuations have mean amplitudes up to 10 Pa and lie in the frequency range 0.01-0.1 Hz. To describe the pumping motion of the air <span class="hlt">pressure</span> field, the <span class="hlt">pressure</span> pumping coefficient (PPC) was defined as the mean change in <span class="hlt">pressure</span> per second. The PPC shows a clear quadratic <span class="hlt">dependence</span> on mean above-canopy wind speed. Empirical modelling of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29118342','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29118342"><span>Physical understanding of the tropical cyclone wind-<span class="hlt">pressure</span> relationship.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chavas, Daniel R; Reed, Kevin A; Knaff, John A</p> <p>2017-11-08</p> <p>The relationship between the two common measures of tropical cyclone intensity, the central <span class="hlt">pressure</span> deficit and the peak near-surface wind speed, is a long-standing problem in tropical meteorology that has been approximated empirically yet lacks physical understanding. Here we provide theoretical grounding for this relationship. We first demonstrate that the central <span class="hlt">pressure</span> deficit is highly predictable from the low-level wind field via gradient wind balance. We then show that this relationship reduces to a <span class="hlt">dependence</span> on two velocity scales: the maximum azimuthal-mean azimuthal wind speed and half the product of the Coriolis parameter and outer storm size. This simple theory is found to hold across a hierarchy of models spanning reduced-complexity and Earth-like global simulations and <span class="hlt">observations</span>. Thus, the central <span class="hlt">pressure</span> deficit is an intensity measure that combines maximum wind speed, storm size, and background rotation rate. This work has significant implications for both fundamental understanding and risk analysis, including why the central <span class="hlt">pressure</span> better explains historical economic damages than does maximum wind speed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009EGUGA..11.9485H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009EGUGA..11.9485H"><span>Digibaro <span class="hlt">pressure</span> instrument onboard the Phoenix Lander</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harri, A.-M.; Polkko, J.; Kahanpää, H. H.; Schmidt, W.; Genzer, M. M.; Haukka, H.; Savijarv1, H.; Kauhanen, J.</p> <p>2009-04-01</p> <p>The Phoenix Lander landed successfully on the Martian northern polar region. The mission is part of the National Aeronautics and Space Administration's (NASA's) Scout program. <span class="hlt">Pressure</span> <span class="hlt">observations</span> onboard the Phoenix lander were performed by an FMI (Finnish Meteorological Institute) instrument, based on a silicon diaphragm sensor head manufactured by Vaisala Inc., combined with MDA data processing electronics. The <span class="hlt">pressure</span> instrument performed successfully throughout the Phoenix mission. The <span class="hlt">pressure</span> instrument had 3 <span class="hlt">pressure</span> sensor heads. One of these was the primary sensor head and the other two were used for monitoring the condition of the primary sensor head during the mission. During the mission the primary sensor was read with a sampling interval of 2 s and the other two were read less frequently as a check of instrument health. The <span class="hlt">pressure</span> sensor system had a real-time data-processing and calibration algorithm that allowed the removal of temperature <span class="hlt">dependent</span> calibration effects. In the same manner as the temperature sensor, a total of 256 data records (8.53 min) were buffered and they could either be stored at full resolution, or processed to provide mean, standard deviation, maximum and minimum values for storage on the Phoenix Lander's Meteorological (MET) unit.The time constant was approximately 3s due to locational constraints and dust filtering requirements. Using algorithms compensating for the time constant effect the temporal resolution was good enough to detect <span class="hlt">pressure</span> drops associated with the passage of nearby dust devils.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009JPhCS.176a2035S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009JPhCS.176a2035S"><span>Effect of <span class="hlt">pressure</span> and magnetic field on the electrical resistivity of TbB6</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sakai, Takeshi; Oomi, Gendo; Kunii, Satoru</p> <p>2009-06-01</p> <p>Electrical resistivity of a single crystal of TbB6 was studied under hydrostatic <span class="hlt">pressures</span> up to 2.1 GPa and magnetic fields up to 9 T. The Néel temperature, rN, decreases linearly with increasing <span class="hlt">pressure</span>: \\ddiff lnTN/\\ddiff P = 3.14×10-2 GPa-1 at zero external field. This <span class="hlt">pressure</span> <span class="hlt">dependence</span> of TN weakens as external fields increase. At ambient <span class="hlt">pressure</span>, the magnetoresistance at 4.2 K is positive up to 4.8 T and becomes negative above 4.8 T. The positive magnetoresistance <span class="hlt">observed</span> at ambient <span class="hlt">pressure</span> is suppressed by applying <span class="hlt">pressure</span>, which enhances the negative magnetoresistance. These results are interpreted in terms of the reduction of the scattering of conduction electrons, due to disordered magnetic moment being suppressed by derealization of 4f electrons at high <span class="hlt">pressure</span>, and the magnetic field variation of the large transition probability between the ground state and the excited levels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25682151','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25682151"><span>Assessment of changes in crystallization properties of <span class="hlt">pressurized</span> milk fat.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Staniewski, Bogusław; Smoczyński, Michał; Staniewska, Katarzyna; Baranowska, Maria; Kiełczewska, Katarzyna; Zulewska, Justyna</p> <p>2015-04-01</p> <p>The aim of the study was to demonstrate the use of fractal image analysis as a possible tool to monitor the effect of <span class="hlt">pressurization</span> on the crystallization pattern of anhydrous milk fat. This approach can be useful when developing new products based on milk fat. The samples were subjected to different hydrostatic <span class="hlt">pressure</span> (100, 200, 300, and 400 MPa) and temperature (10 and 40 °C) treatments. The crystallization microphotographs were taken with a scanning electron microscope. The image analysis of scanning electron microscope photographs was done to determine a fractal dimension. Milk-fat <span class="hlt">pressurization</span> under the applied parameters resulted in slight, but statistically significant, changes in the course of crystallization curves, related to the triacylglycerol fraction crystallizing in the lowest temperature (I exothermic effect). These changes were <span class="hlt">dependent</span> on the value of <span class="hlt">pressure</span> but not <span class="hlt">dependent</span> on the temperatures applied during the process of <span class="hlt">pressurization</span> (at either 10 or 40 °C). In turn, significant differences were <span class="hlt">observed</span> in crystallization images of milk-fat samples subjected to this process compared with the control sample. The results of additional fractal analysis additionally demonstrated the highest degree of irregularity of the surface of the crystalline form for the nonpressurized sample and the samples <span class="hlt">pressurized</span> at 200 and 300 MPa at 10 °C. The lowest value of fractal dimension-indicative of the least irregularity-was achieved for the fat samples <span class="hlt">pressurized</span> at 400 MPa, 10 °C and at 100 MPa, 40 °C. The possibilities of wider application of the fractal analysis for the evaluation of effects of parameters of various technological processes on crystallization properties of milk fat require further extensive investigations. Copyright © 2015 American Dairy Science Association. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018InJPh.tmp..546P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018InJPh.tmp..546P"><span>Equations of state and <span class="hlt">pressure</span> <span class="hlt">dependence</span> of bulk modulus for aggregated diamond nanorods</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Patel, G. R.; Thakar, N. A.; Pandya, T. C.</p> <p>2018-04-01</p> <p>In the present paper study of the high <span class="hlt">pressure</span> behaviour of aggregated diamond nanorods (ADNRs) and diamond have been carried out. A comparative study of different equations of state is discussed to understand the high <span class="hlt">pressure</span> behaviour of diamond and the aggregated diamond nanorods. In the present study the usual Tait's equation of state has been modified to predict the high <span class="hlt">pressure</span> behaviour of carbon material ADNRs and diamond. The results obtained in the present study are compared with available experimental evidences. Bulk moduli as a function of <span class="hlt">pressure</span> are also computed for ADNRs and natural diamond in the light of recent investigations. Present study reveals that ADNRs are less compressible than diamond.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhyB..407.2861N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhyB..407.2861N"><span>Theoretical study of band gap in CuAlO2: <span class="hlt">Pressure</span> <span class="hlt">dependence</span> and self-interaction correction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nakanishi, Akitaka; Katayama-Yoshida, Hiroshi</p> <p>2012-08-01</p> <p>By using first-principles calculations, we studied the energy gaps of delafossite CuAlO2: (1) <span class="hlt">pressure</span> <span class="hlt">dependence</span> and (2) self-interaction correction (SIC). Our simulation shows that CuAlO2 transforms from a delafossite structure to a leaning delafossite structure at 60 GPa. The energy gap of CuAlO2 increases through the structural transition due to the enhanced covalency of Cu 3d and O 2p states. We implemented a self-interaction correction (SIC) into first-principles calculation code to go beyond local density approximation and applied it to CuAlO2. The energy gap calculated within the SIC is close to experimental data while one calculated without the SIC is about 1 eV smaller than the experimental data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PhDT........10T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PhDT........10T"><span>Composition, Temperature, and <span class="hlt">Pressure</span> <span class="hlt">Dependence</span> of the Phonon (Thermal) Conductivity of Silicate Geoliquids</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tikunoff, Dane Michael</p> <p></p> <p>The study of geoliquids and their transport properties is a burgeoning field that sheds light on many critical geological problems. One such property, the thermal conductivity, measures the heat conduction capacity of a material and plays an important role in mantle and crust dynamics. Previous research has suggested that an increased insulation factor in rocks of the crust, regulated by relatively small values of the thermal conductivity, promotes anatexis and alleviates radiogenic heating requirements for the inducement of dehydration-triggered partial melting (Whittington et al., 2009). At greater depths, the proposed existence of melt patches along and immediately above the Core-Mantle Boundary (CMB) at ~2900 km depth could explain the discrete rather than graduated thermal gradient seen across the CMB (Murakami and Bass, 2011). This thesis describes the use of Molecular Dynamics (MD) simulations to compute thermal conductivity for three liquid silicates: CaMgSi2O6, NaAlSi3 O8 and MgSi2O4. The motivation for this study was to examine the temperature, <span class="hlt">pressure</span> and compositional <span class="hlt">dependencies</span> of thermal conductivity approximating conditions in the upper mantle (0-30 GPa, 2000-4500 K) for a few end member geosilicate liquids of natural importance. Results at low <span class="hlt">pressure</span> and temperature show good agreement with recent laboratory measurements on CaMgSi2O6 and NaAlSi3O8 suggesting that MD simulation can provide realistic values at elevated <span class="hlt">pressure</span> and temperature, conditions not readily accessible without great expense and time in the laboratory. For example, simulation results for molten diopside at 1763+/-13 K and 0.36+/-0.017 GPa provide a thermal conductivity value of k=1.186+/-0.019 W/m K while laser-flash data from Hofmeister et al. (2009) provides a value of k=1.178 +/-0.06 W/m K, agreement to within a percent. Further, a positive correlation between atomic structure and thermal conductivity is confirmed. At low <span class="hlt">pressure</span>, the polymeric liquid NaAlSi3O8, in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AcSpA.193...47S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AcSpA.193...47S"><span><span class="hlt">Pressure</span>-induced phase transition and fracture in α-MoO3 nanoribbons</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Silveira, Jose V.; Vieira, Luciana L.; Aguiar, Acrisio L.; Freire, Paulo T. C.; Mendes Filho, Josue; Alves, Oswaldo L.; Souza Filho, Antonio G.</p> <p>2018-03-01</p> <p>MoO3 nanoribbons were studied under different <span class="hlt">pressure</span> conditions ranging from 0 to 21 GPa at room temperature. The effect of the applied <span class="hlt">pressure</span> on the spectroscopic and morphologic properties of the MoO3 nanoribbons was investigated by means of Raman spectroscopy and scanning electron microscopy techniques. The <span class="hlt">pressure</span> <span class="hlt">dependent</span> Raman spectra of the MoO3 nanoribbons indicate that a structural phase transition occurs at 5 GPa from the orthorhombic α-MoO3 phase (Pbnm) to the monoclinic MoO3-II phase (P21/m), which remains stable up to 21 GPa. Such phase transformation occurs at considerably lower <span class="hlt">pressure</span> than the critical <span class="hlt">pressure</span> for α-MoO3 microcrystals (12 GPa). We suggested that the applanate morphology combined with the presence of crystalline defects in the sample play an important role in the phase transition of the MoO3 nanoribbons. Frequencies and linewidths of the Raman bands as a function of <span class="hlt">pressure</span> also suggest a <span class="hlt">pressure</span>-induced morphological change and the decreasing of the nanocrystal size. The <span class="hlt">observed</span> spectroscopic changes are supported by electron microscopy images, which clearly show a <span class="hlt">pressure</span>-induced morphologic change in MoO3 nanoribbons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1249336-solidification-loss-hydrostaticity-liquid-media-used-pressure-measurements','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1249336-solidification-loss-hydrostaticity-liquid-media-used-pressure-measurements"><span>Solidification and loss of hydrostaticity in liquid media used for <span class="hlt">pressure</span> measurements</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Torikachvili, M. S.; Kim, S. K.; Colombier, E.; ...</p> <p>2015-12-16</p> <p>We carried out a study of the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the solidification temperature in nine <span class="hlt">pressure</span> transmitting media that are liquid at ambient temperature, under <span class="hlt">pressures</span> up to 2.3 GPa. These fluids are 1:1 isopentane/n-pentane, 4:6 light mineral oil/n-pentane, 1:1 isoamyl alcohol/n-pentane, 4:1 methanol/ethanol, 1:1 FC72/FC84 (Fluorinert), Daphne 7373, isopentane, and Dow Corning PMX silicone oils 200 and 60,000 cS. We relied on the high sensitivity of the electrical resistivity of Ba(Fe 1–xRu x) 2As 2 single crystals to the freezing of the <span class="hlt">pressure</span> media and cross-checked with corresponding anomalies <span class="hlt">observed</span> in the resistance of the manganin coil that servedmore » as the ambient temperature resistive manometer. In addition to establishing the temperature-<span class="hlt">pressure</span> line separating the liquid (hydrostatic) and frozen (non-hydrostatic) phases, these data permit rough estimates of the freezing <span class="hlt">pressure</span> of these media at ambient temperature. As a result, this <span class="hlt">pressure</span> establishes the extreme limit for the medium to be considered hydrostatic. For higher applied <span class="hlt">pressures</span>, the medium has to be treated as non-hydrostatic.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1249336','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1249336"><span>Solidification and loss of hydrostaticity in liquid media used for <span class="hlt">pressure</span> measurements</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>Torikachvili, M. S.; Kim, S. K.; Colombier, E.</p> <p></p> <p>We carried out a study of the <span class="hlt">pressure</span> <span class="hlt">dependence</span> of the solidification temperature in nine <span class="hlt">pressure</span> transmitting media that are liquid at ambient temperature, under <span class="hlt">pressures</span> up to 2.3 GPa. These fluids are 1:1 isopentane/n-pentane, 4:6 light mineral oil/n-pentane, 1:1 isoamyl alcohol/n-pentane, 4:1 methanol/ethanol, 1:1 FC72/FC84 (Fluorinert), Daphne 7373, isopentane, and Dow Corning PMX silicone oils 200 and 60,000 cS. We relied on the high sensitivity of the electrical resistivity of Ba(Fe 1–xRu x) 2As 2 single crystals to the freezing of the <span class="hlt">pressure</span> media and cross-checked with corresponding anomalies <span class="hlt">observed</span> in the resistance of the manganin coil that servedmore » as the ambient temperature resistive manometer. In addition to establishing the temperature-<span class="hlt">pressure</span> line separating the liquid (hydrostatic) and frozen (non-hydrostatic) phases, these data permit rough estimates of the freezing <span class="hlt">pressure</span> of these media at ambient temperature. As a result, this <span class="hlt">pressure</span> establishes the extreme limit for the medium to be considered hydrostatic. For higher applied <span class="hlt">pressures</span>, the medium has to be treated as non-hydrostatic.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29791881','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29791881"><span>Effect of methane partial <span class="hlt">pressure</span> on the performance of a membrane biofilm reactor coupling methane-<span class="hlt">dependent</span> denitrification and anammox.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cai, Chen; Hu, Shihu; Chen, Xueming; Ni, Bing-Jie; Pu, Jiaoyang; Yuan, Zhiguo</p> <p>2018-10-15</p> <p>Complete nitrogen removal has recently been demonstrated by integrating anaerobic ammonium oxidation (anammox) and denitrifying anaerobic methane oxidation (DAMO) processes. In this work, the effect of methane partial <span class="hlt">pressure</span> on the performance of a membrane biofilm reactor (MBfR) consisting of DAMO and anammox microorganisms was evaluated. The activities of DAMO archaea and DAMO bacteria in the biofilm increased significantly with increased methane partial <span class="hlt">pressure</span>, from 367 ± 9 and 58 ± 22 mg-N L -1 d -1 to 580 ± 12 and 222 ± 22 mg-N L -1 d -1 , respectively, while the activity of anammox bacteria only increased slightly, when the methane partial <span class="hlt">pressure</span> was elevated from 0.24 to 1.39 atm in the short-term batch tests. The results were supported by a long-term (seven weeks) continuous test, when the methane partial <span class="hlt">pressure</span> was dropped from 1.39 to 0.78 atm. The methane utilization efficiency was always above 96% during both short-term and long-term tests. Taken together, nitrogen removal rate (especially the nitrate reduction rate by DAMO archaea) and methane utilization efficiency could be maintained at high levels in a broad range of methane partial <span class="hlt">pressure</span> (0.24-1.39 atm in this study). In addition, a previously established DAMO/anammox biofilm model was used to analyze the experimental data. The <span class="hlt">observed</span> impacts of methane partial <span class="hlt">pressure</span> on biofilm activity were well explained by the modeling results. These results suggest that methane partial <span class="hlt">pressure</span> can potentially be used as a manipulated variable to control reaction rates, ultimately to maintain high nitrogen removal efficiency, according to nitrogen loading rate. Copyright © 2018 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1980PhRvL..44.1076A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1980PhRvL..44.1076A"><span><span class="hlt">Pressure</span> <span class="hlt">Dependence</span> of the Specific-Heat Jump at the Superfluid Transition and the Effective Mass of 3He</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Alvesalo, T. A.; Haavasoja, T.; Manninen, M. T.; Soinne, A. T.</p> <p>1980-04-01</p> <p>The specific heat of liquid 3He has been measured from 1 to 10 mK between 0 and 32.5 bars. The values implied for the effective mass are considerably smaller than the currently accepted ones. Near zero <span class="hlt">pressure</span> the specific-heat jump is close to the BCS value 1.43, and at 32.5 bars it has reached 1.90 in the B phase and 2.04 in the A phase. The temperature <span class="hlt">dependence</span> of the specific heat in the B phase agrees with a model of Serene and Rainer. The latent heat at the A-B transition has been measured.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22271104-cavitation-erosion-silver-plated-coating-different-temperatures-pressures','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22271104-cavitation-erosion-silver-plated-coating-different-temperatures-pressures"><span>Cavitation erosion of silver plated coating at different temperatures and <span class="hlt">pressures</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>Hattori, Shuji; Motoi, Yoshihiro; Kikuta, Kengo</p> <p>2014-04-11</p> <p>Cavitation often occurs in inducer pumps used for space rockets. Silver plated coating on the inducer liner faces the damage of cavitation. Therefore, it is important to study about the cavitation erosion resistance for silver plated coating at several operating conditions in the inducer pumps. In this study, the cavitation erosion tests were carried for silver plated coating in deionized water and ethanol at several liquid temperatures (273K–400K) and <span class="hlt">pressures</span> (0.10MPa–0.48MPa). The mass loss rate is evaluated in terms of thermodynamic parameter Σ proposed by Brennen [9], suppression <span class="hlt">pressure</span> p–p{sub v} (p{sub v}: saturated vapor <span class="hlt">pressure</span>) and acoustic impedance ρcmore » (ρ: density and c: sound speed). Cavitation bubble behaviors <span class="hlt">depending</span> on the thermodynamic effect and the liquid type were <span class="hlt">observed</span> by high speed video camera. The mass loss rate is formulated by thermodynamic parameter Σ, suppression <span class="hlt">pressure</span> p–p{sub v} and acoustic impedance ρc.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMOS13B1730B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMOS13B1730B"><span>Long-term <span class="hlt">observations</span> of seafloor <span class="hlt">pressure</span> variations at Lucky Strike volcano, Mid-Atlantic Ridge</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ballu, V.; de Viron, O.; Crawford, W. C.; Cannat, M.; Escartin, J.</p> <p>2012-12-01</p> <p>Lucky Strike volcano is a segment-center volcano on the Mid-Atlantic Ridge at 37°N. Extensive faulting reveals an important tectonic component in its formation, while a seismically imaged axial magma chamber reflector and active high-temperature hydrothermal vents reveal an important present-day magmatic component. Lucky Strike volcano has been the subject of long-term multidisciplinary seafloor <span class="hlt">observations</span> to understand relations between magmatism, tectonism, hydrothermal circulation, biology and chemistry as part of the MoMAR (Monitoring of the Mid-Atlantic Ridge) program. Absolute <span class="hlt">pressure</span> gauges have been recording on the volcano since 2007, to identify deformations associated with tectonism or magmatism. Deformation measurements are one of the principal means of determining volcanic activity, but the amount of deformation associated with volcanic events varies greatly between different volcanos. We installed two sites: one in the volcano's summit "lava lake" (1700 m depth) and another on the volcano's flank (2000 m depth). <span class="hlt">Pressure</span> is recorded every thirty seconds, giving a data set that constrains movements on the scale from minutes to years. No major deformation event has been detected by the instruments since their installation (nor has any significant tectonic event been detected by a seismic network in place since 2007), so we concentrate here on the detection limit of these instruments and on variations in the long-period ocean wave climate. Using the statistical characteristics of the <span class="hlt">pressure</span> signal, modeled by an auto-regressive process, we determine that a movement between the sites of 1 cm over less than 10 days is detectable; the detection threshold decreases to about 0.2 cm for the shortest time periods and increases for longer time periods due to instrumental drift. We compare the statistical characteristics and short- and long-term sensitivity of three different types of gauges used during the experiment: Paroscientific standard</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>