Sample records for acoustic pressure gradient

  1. Acoustic waves in gases with strong pressure gradients

    NASA Technical Reports Server (NTRS)

    Zorumski, William E.

    1989-01-01

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

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

    NASA Technical Reports Server (NTRS)

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

    2007-01-01

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

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

    NASA Technical Reports Server (NTRS)

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

    2008-01-01

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

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

    NASA Technical Reports Server (NTRS)

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

    1990-01-01

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

  5. Shaping and timing gradient pulses to reduce MRI acoustic noise.

    PubMed

    Segbers, Marcel; Rizzo Sierra, Carlos V; Duifhuis, Hendrikus; Hoogduin, Johannes M

    2010-08-01

    A method to reduce the acoustic noise generated by gradient systems in MRI has been recently proposed; such a method is based on the linear response theory. Since the physical cause of MRI acoustic noise is the time derivative of the gradient current, a common trapezoid current shape produces an acoustic gradient coil response mainly during the rising and falling edge. In the falling edge, the coil acoustic response presents a 180 degrees phase difference compared to the rising edge. Therefore, by varying the width of the trapezoid and keeping the ramps constant, it is possible to suppress one selected frequency and its higher harmonics. This value is matched to one of the prominent resonance frequencies of the gradient coil system. The idea of cancelling a single frequency is extended to a second frequency, using two successive trapezoid-shaped pulses presented at a selected interval. Overall sound pressure level reduction of 6 and 10 dB is found for the two trapezoid shapes and a single pulse shape, respectively. The acoustically optimized pulse shape proposed is additionally tested in a simulated echo planar imaging readout train, obtaining a sound pressure level reduction of 12 dB for the best case.

  6. Active-passive gradient shielding for MRI acoustic noise reduction.

    PubMed

    Edelstein, William A; Kidane, Tesfaye K; Taracila, Victor; Baig, Tanvir N; Eagan, Timothy P; Cheng, Yu-Chung N; Brown, Robert W; Mallick, John A

    2005-05-01

    An important source of MRI acoustic noise-magnet cryostat warm-bore vibrations caused by eddy-current-induced forces-can be mitigated by a passive metal shield mounted on the outside of a vibration-isolated, vacuum-enclosed shielded gradient set. Finite-element (FE) calculations for a z-gradient indicate that a 2-mm-thick Cu layer wrapped on the gradient assembly can decrease mechanical power deposition in the warm bore and reduce warm-bore acoustic noise production by about 25 dB. Eliminating the conducting warm bore and other magnet parts as significant acoustic noise sources could lead to the development of truly quiet, fully functioning MRI systems with noise levels below 70 dB. Copyright 2005 Wiley-Liss, Inc.

  7. A theoretical prediction of the acoustic pressure generated by turbulence-flame front interactions

    NASA Technical Reports Server (NTRS)

    Huff, R. G.

    1984-01-01

    The equations of momentum annd continuity are combined and linearized yielding the one dimensional nonhomogeneous acoustic wave equation. Three terms in the non-homogeneous equation act as acoustic sources and are taken to be forcing functions acting on the homogeneous wave equation. The three source terms are: fluctuating entropy, turbulence gradients, and turbulence-flame interactions. Each source term is discussed. The turbulence-flame interaction source is used as the basis for computing the source acoustic pressure from the Fourier transformed wave equation. Pressure fluctuations created in turbopump gas generators and turbines may act as a forcing function for turbine and propellant tube vibrations in Earth to orbit space propulsion systems and could reduce their life expectancy. A preliminary assessment of the acoustic pressure fluctuations in such systems is presented.

  8. A theoretical prediction of the acoustic pressure generated by turbulence-flame front interactions

    NASA Technical Reports Server (NTRS)

    Huff, R. G.

    1984-01-01

    The equations of momentum and continuity are combined and linearized yielding the one dimensional nonhomogeneous acoustic wave equation. Three terms in the non-homogeneous equation act as acoustic sources and are taken to be forcing functions acting on the homogeneous wave equation. The three source terms are: fluctuating entropy, turbulence gradients, and turbulence-flame interactions. Each source term is discussed. The turbulence-flame interaction source is used as the basis for computing the source acoustic pressure from the Fourier transformed wave equation. Pressure fluctuations created in turbopump gas generators and turbines may act as a forcing function for turbine and propellant tube vibrations in earth to orbit space propulsion systems and could reduce their life expectancy. A preliminary assessment of the acoustic pressure fluctuations in such systems is presented.

  9. A model for jet-noise analysis using pressure-gradient correlations on an imaginary cone

    NASA Technical Reports Server (NTRS)

    Norum, T. D.

    1974-01-01

    The technique for determining the near and far acoustic field of a jet through measurements of pressure-gradient correlations on an imaginary conical surface surrounding the jet is discussed. The necessary analytical developments are presented, and their feasibility is checked by using a point source as the sound generator. The distribution of the apparent sources on the cone, equivalent to the point source, is determined in terms of the pressure-gradient correlations.

  10. Acoustic characteristics of the medium with gradient change of impedance

    NASA Astrophysics Data System (ADS)

    Hu, Bo; Yang, Desen; Sun, Yu; Shi, Jie; Shi, Shengguo; Zhang, Haoyang

    2015-10-01

    The medium with gradient change of acoustic impedance is a new acoustic structure which developed from multiple layer structures. In this paper, the inclusion is introduced and a new set of equations is developed. It can obtain better acoustic properties based on the medium with gradient change of acoustic impedance. Theoretical formulation has been systematically addressed which demonstrates how the idea of utilizing this method. The sound reflection and absorption coefficients were obtained. At last, the validity and the correctness of this method are assessed by simulations. The results show that appropriate design of parameters of the medium can improve underwater acoustic properties.

  11. Dispersion of acoustic surface waves by velocity gradients

    NASA Astrophysics Data System (ADS)

    Kwon, S. D.; Kim, H. C.

    1987-10-01

    The perturbation theory of Auld [Acoustic Fields and Waves in Solids (Wiley, New York, 1973), Vol. II, p. 294], which describes the effect of a subsurface gradient on the velocity dispersion of surface waves, has been modified to a simpler form by an approximation using a newly defined velocity gradient for the case of isotropic materials. The modified theory is applied to nitrogen implantation in AISI 4140 steel with a velocity gradient of Gaussian profile, and compared with dispersion data obtained by the ultrasonic right-angle technique in the frequency range from 2.4 to 14.8 MHz. The good agreement between experiments and our theory suggests that the compound layer in the subsurface region plays a dominant role in causing the dispersion of acoustic surface waves.

  12. Manipulation of acoustic wavefront by gradient metasurface based on Helmholtz Resonators.

    PubMed

    Lan, Jun; Li, Yifeng; Xu, Yue; Liu, Xiaozhou

    2017-09-06

    We designed a gradient acoustic metasurface to manipulate acoustic wavefront freely. The broad bandwidth and high efficiency transmission are achieved by the acoustic metasurface which is constructed with a series of unit cells to provide desired discrete acoustic velocity distribution. Each unit cell is composed of a decorated metal plate with four periodically arrayed Helmholtz resonators (HRs) and a single slit. The design employs a gradient velocity to redirect refracted wave and the impedance matching between the metasurface and the background medium can be realized by adjusting the slit width of unit cell. The theoretical and numerical results show that some excellent wavefront manipulations are demonstrated by anomalous refraction, non-diffracting Bessel beam, sub-wavelength flat focusing, and effective tunable acoustic negative refraction. Our designed structure may offer potential applications for the imaging system, beam steering and acoustic lens.

  13. Acoustic cymbal performance under hydrostatic pressure

    NASA Astrophysics Data System (ADS)

    Jenne, Kirk E.; Huang, Dehua; Howarth, Thomas R.

    2004-05-01

    Continual awareness about the need to develop light-weight, low-volume, broadband, underwater acoustic projector and receive arrays that perform consistently in diverse environments is evident in recent Navy acoustic system initiatives. Acoustic cymbals, so named for resemblance to the percussive musical instruments, are miniature flextensional transducers that may perhaps meet the performance criteria for consistent performance under hydrostatic pressure after modifications in the design. These acoustic cymbals consist of a piezoceramic disk (or ring) bonded to two opposing cymbal-shaped metal shells. Operating as mechanical transformers, the two metal shells convert the large generative force inherently within the disk's radial mode into increased volume displacement at the metal shell surface to obtain volume displacement that translates into usable source levels and/or sensitivities at sonar frequencies in a relatively broad band. The air-backed design for standard acoustic cymbal transducers presents a barrier to deepwater applications. A new acoustic cymbal design for high-pressure applications will be presented for the first time. This practical pressure compensation is designed to diminish the effects of hydrostatic pressure to maintain consistent acoustic cymbal performance. Transmit and receive performance data, determined at the Naval Undersea Warfare Center's (NUWC) Acoustic Pressure Tank Facility (APTF), is presented.

  14. Near-field multiple traps of paraxial acoustic vortices with strengthened gradient force generated by sector transducer array

    NASA Astrophysics Data System (ADS)

    Wang, Qingdong; Li, Yuzhi; Ma, Qingyu; Guo, Gepu; Tu, Juan; Zhang, Dong

    2018-01-01

    In order to improve the capability of particle trapping close to the source plane, theoretical and experimental studies on near-field multiple traps of paraxial acoustic vortices (AVs) with a strengthened acoustic gradient force (AGF) generated by a sector transducer array were conducted. By applying the integration of point source radiation, numerical simulations for the acoustic fields generated by the sector transducer array were conducted and compared with those produced by the circular transducer array. It was proved that strengthened AGFs of near-field multiple AVs with higher peak pressures and smaller vortex radii could be produced by the sector transducer array with a small topological charge. The axial distributions of the equivalent potential gradient indicated that the AGFs of paraxial AVs in the near field were much higher than those in the far field, and the distances at the near-field vortex antinodes were also proved to be the ideal trapping positions with relatively higher AGFs. With the established 8-channel AV generation system, theoretical studies were also verified by the experimental measurements of pressure and phase for AVs with various topological charges. The formation of near-field multiple paraxial AVs was verified by the cross-sectional circular pressure distributions with perfect phase spirals around central pressure nulls, and was also proved by the vortex nodes and antinodes along the center axis. The favorable results demonstrated the feasibility of generating near-field multiple traps of paraxial AVs with strengthened AGF using the sector transducer array, and suggested the potential applications of close-range particle trapping in biomedical engineering.

  15. Directional Reflective Surface Formed via Gradient-Impeding Acoustic Meta-Surfaces

    PubMed Central

    Song, Kyungjun; Kim, Jedo; Hur, Shin; Kwak, Jun-Hyuk; Lee, Seong-Hyun; Kim, Taesung

    2016-01-01

    Artificially designed acoustic meta-surfaces have the ability to manipulate sound energy to an extraordinary extent. Here, we report on a new type of directional reflective surface consisting of an array of sub-wavelength Helmholtz resonators with varying internal coiled path lengths, which induce a reflection phase gradient along a planar acoustic meta-surface. The acoustically reshaped reflective surface created by the gradient-impeding meta-surface yields a distinct focal line similar to a parabolic cylinder antenna, and is used for directive sound beamforming. Focused beam steering can be also obtained by repositioning the source (or receiver) off axis, i.e., displaced from the focal line. Besides flat reflective surfaces, complex surfaces such as convex or conformal shapes may be used for sound beamforming, thus facilitating easy application in sound reinforcement systems. Therefore, directional reflective surfaces have promising applications in fields such as acoustic imaging, sonic weaponry, and underwater communication. PMID:27562634

  16. All-angle Negative Reflection with An Ultrathin Acoustic Gradient Metasurface: Floquet-Bloch Modes Perspective and Experimental Verification.

    PubMed

    Liu, Bingyi; Zhao, Jiajun; Xu, Xiaodong; Zhao, Wenyu; Jiang, Yongyuan

    2017-10-23

    Metasurface with gradient phase response offers new alternative for steering the propagation of waves. Conventional Snell's law has been revised by taking the contribution of local phase gradient into account. However, the requirement of momentum matching along the metasurface sets its nontrivial beam manipulation functionality within a limited-angle incidence. In this work, we theoretically and experimentally demonstrate that the acoustic gradient metasurface supports the negative reflection for all-angle incidence. The mode expansion theory is developed to help understand how the gradient metasurface tailors the incident beams, and the all-angle negative reflection occurs when the first negative order Floquet-Bloch mode dominates inside the metasurface slab. The coiling-up space structures are utilized to build desired acoustic gradient metasurface, and the all-angle negative reflections have been perfectly verified by experimental measurements. Our work offers the Floquet-Bloch modes perspective for qualitatively understanding the reflection behaviors of the acoustic gradient metasurface, and the all-angle negative reflection characteristic possessed by acoustic gradient metasurface could enable a new degree of the acoustic wave manipulating and be applied in the functional diffractive acoustic elements, such as the all-angle acoustic back reflector.

  17. Acoustical power amplification and damping by temperature gradients.

    PubMed

    Biwa, Tetsushi; Komatsu, Ryo; Yazaki, Taichi

    2011-01-01

    Ceperley proposed a concept of a traveling wave heat engine ["A pistonless Stirling engine-The traveling wave heat engine," J. Acoust. Soc. Am. 66, 1508-1513 (1979).] that provided a starting point of thermoacoustics today. This paper verifies experimentally his idea through observation of amplification and strong damping of a plane acoustic traveling wave as it passes through axial temperature gradients. The acoustic power gain is shown to obey a universal curve specified by a dimensionless parameter ωτα; ω is the angular frequency and τα is the relaxation time for the gas to thermally equilibrate with channel walls. As an application of his idea, a three-stage acoustic power amplifier is developed, which attains the gain up to 10 with a moderate temperature ratio of 2.3.

  18. A spatiotemporally controllable chemical gradient generator via acoustically oscillating sharp-edge structures.

    PubMed

    Huang, Po-Hsun; Chan, Chung Yu; Li, Peng; Nama, Nitesh; Xie, Yuliang; Wei, Cheng-Hsin; Chen, Yuchao; Ahmed, Daniel; Huang, Tony Jun

    2015-11-07

    The ability to generate stable, spatiotemporally controllable concentration gradients is critical for resolving the dynamics of cellular response to a chemical microenvironment. Here we demonstrate an acoustofluidic gradient generator based on acoustically oscillating sharp-edge structures, which facilitates in a step-wise fashion the rapid mixing of fluids to generate tunable, dynamic chemical gradients. By controlling the driving voltage of a piezoelectric transducer, we demonstrated that the chemical gradient profiles can be conveniently altered (spatially controllable). By adjusting the actuation time of the piezoelectric transducer, moreover, we generated pulsatile chemical gradients (temporally controllable). With these two characteristics combined, we have developed a spatiotemporally controllable gradient generator. The applicability and biocompatibility of our acoustofluidic gradient generator are validated by demonstrating the migration of human dermal microvascular endothelial cells (HMVEC-d) in response to a generated vascular endothelial growth factor (VEGF) gradient, and by preserving the viability of HMVEC-d cells after long-term exposure to an acoustic field. Our device features advantages such as simple fabrication and operation, compact and biocompatible device, and generation of spatiotemporally tunable gradients.

  19. Acoustic Radiation Pressure

    NASA Technical Reports Server (NTRS)

    Cantrell, John H.

    2018-01-01

    The theoretical foundation of acoustic radiation pressure in plane wave beams is reexamined. It is shown from finite deformation theory and the Boltzmann-Ehrenfest Adiabatic Principle that the Brillouin stress tensor (BST) is the radiation stress in Lagrangian coordinates (not Eulerian coordinates) and that the terms in the BST are not the momentum flux density and mean excess Eulerian stress but are simply contributions to the variation in the wave oscillation period resulting from changes in path length and true wave velocity, respectively, from virtual variations in the strain. It is shown that the radiation stress in Eulerian coordinates is the mean Cauchy stress (not the momentum flux density, as commonly assumed) and that Langevin's second relation does not yield an assessment of the mean Eulerian pressure, since the enthalpy used in the traditional derivations is a function of the thermodynamic tensions - not the Eulerian pressure. It is shown that the transformation between Lagrangian and Eulerian quantities cannot be obtained from the commonly-used expansion of one of the quantities in terms of the particle displacement, since the expansion provides only the difference between the value of the quantity at two different points in Cartesian space separated by the displacement. The proper transformation is obtained only by employing the transformation coefficients of finite deformation theory, which are defined in terms of the displacement gradients. Finite deformation theory leads to the result that for laterally unconfined, plane waves the Lagrangian and Eulerian radiation pressures are equal with the value (1/4)(2K) along the direction of wave propagation, where (K) is the mean kinetic energy density, and zero in directions normal to the propagation direction. This is contrary to the Langevin result that the Lagrangian radiation pressure in the propagation direction is equal to (2K) and the BST result that the Eulerian radiation pressure in that direction

  20. Acoustical and optical radiation pressure and the development of single beam acoustical tweezers

    NASA Astrophysics Data System (ADS)

    Thomas, Jean-Louis; Marchiano, Régis; Baresch, Diego

    2017-07-01

    Studies on radiation pressure in acoustics and optics have enriched one another and have a long common history. Acoustic radiation pressure is used for metrology, levitation, particle trapping and actuation. However, the dexterity and selectivity of single-beam optical tweezers are still to be matched with acoustical devices. Optical tweezers can trap, move and position micron size particles, biological samples or even atoms with subnanometer accuracy in three dimensions. One limitation of optical tweezers is the weak force that can be applied without thermal damage due to optical absorption. Acoustical tweezers overcome this limitation since the radiation pressure scales as the field intensity divided by the speed of propagation of the wave. However, the feasibility of single beam acoustical tweezers was demonstrated only recently. In this paper, we propose a historical review of the strong similarities but also the specificities of acoustical and optical radiation pressures, from the expression of the force to the development of single-beam acoustical tweezers.

  1. Detection of acoustic waves by NMR using a radiofrequency field gradient.

    PubMed

    Madelin, Guillaume; Baril, Nathalie; Lewa, Czeslaw J; Franconi, Jean Michel; Canioni, Paul; Thiaudiére, Eric; de Certaines, Jacques D

    2003-03-01

    A B(1) field gradient-based method previously described for the detection of mechanical vibrations has been applied to detect oscillatory motions in condensed matter originated from acoustic waves. A ladder-shaped coil generating a quasi-constant RF-field gradient was associated with a motion-encoding NMR sequence consisting in a repetitive binomial 13;31; RF pulse train (stroboscopic acquisition). The NMR response of a gel phantom subject to acoustic wave excitation in the 20-200 Hz range was investigated. Results showed a linear relationship between the NMR signal and the wave amplitude and a spectroscopic selectivity of the NMR sequence with respect to the input acoustic frequency. Spin displacements as short as a few tens of nanometers were able to be detected with this method.

  2. Detection of acoustic waves by NMR using a radiofrequency field gradient

    NASA Astrophysics Data System (ADS)

    Madelin, Guillaume; Baril, Nathalie; Lewa, Czeslaw J.; Franconi, Jean-Michel; Canioni, Paul; Thiaudiére, Eric; de Certaines, Jacques D.

    2003-03-01

    A B1 field gradient-based method previously described for the detection of mechanical vibrations has been applied to detect oscillatory motions in condensed matter originated from acoustic waves. A ladder-shaped coil generating a quasi-constant RF-field gradient was associated with a motion-encoding NMR sequence consisting in a repetitive binomial 1 3¯3 1¯ RF pulse train (stroboscopic acquisition). The NMR response of a gel phantom subject to acoustic wave excitation in the 20-200 Hz range was investigated. Results showed a linear relationship between the NMR signal and the wave amplitude and a spectroscopic selectivity of the NMR sequence with respect to the input acoustic frequency. Spin displacements as short as a few tens of nanometers were able to be detected with this method.

  3. Acoustic wave propagation in high-pressure system.

    PubMed

    Foldyna, Josef; Sitek, Libor; Habán, Vladimír

    2006-12-22

    Recently, substantial attention is paid to the development of methods of generation of pulsations in high-pressure systems to produce pulsating high-speed water jets. The reason is that the introduction of pulsations into the water jets enables to increase their cutting efficiency due to the fact that the impact pressure (so-called water-hammer pressure) generated by an impact of slug of water on the target material is considerably higher than the stagnation pressure generated by corresponding continuous jet. Special method of pulsating jet generation was developed and tested extensively under the laboratory conditions at the Institute of Geonics in Ostrava. The method is based on the action of acoustic transducer on the pressure liquid and transmission of generated acoustic waves via pressure system to the nozzle. The purpose of the paper is to present results obtained during the research oriented at the determination of acoustic wave propagation in high-pressure system. The final objective of the research is to solve the problem of transmission of acoustic waves through high-pressure water to generate pulsating jet effectively even at larger distances from the acoustic source. In order to be able to simulate numerically acoustic wave propagation in the system, it is necessary among others to determine dependence of the sound speed and second kinematical viscosity on operating pressure. Method of determination of the second kinematical viscosity and speed of sound in liquid using modal analysis of response of the tube filled with liquid to the impact was developed. The response was measured by pressure sensors placed at both ends of the tube. Results obtained and presented in the paper indicate good agreement between experimental data and values of speed of sound calculated from so-called "UNESCO equation". They also show that the value of the second kinematical viscosity of water depends on the pressure.

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

    NASA Technical Reports Server (NTRS)

    Gotoh, T.; Rogallo, R. S.

    1994-01-01

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

  5. Inherent losses induced absorptive acoustic rainbow trapping with a gradient metasurface

    NASA Astrophysics Data System (ADS)

    Liu, Tuo; Liang, Shanjun; Chen, Fei; Zhu, Jie

    2018-03-01

    Acoustic rainbow trapping represents the phenomenon of strong acoustic dispersion similar to the optical "trapped rainbow," which allows spatial-spectral modulation and broadband trapping of sound. It can be realized with metamaterials that provide the required strong dispersion absent in natural materials. However, as the group velocity cannot be reduced to exactly zero before the forward mode being coupled to the backward mode, such trapping is temporary and the local sound oscillation ultimately radiates backward. Here, we propose a gradient metasurface, a rigid surface structured with gradient perforation along the wave propagation direction, in which the inherent thermal and viscous losses inside the holes are considered. We show that the gradually diminished group velocity of the structure-induced surface acoustic waves (SSAWs) supported by the metasurface becomes anomalous at the trapping position, induced by the existence of the inherent losses, which implies that the system's absorption reaches its maximum. Together with the progressively increased attenuation of the SSAWs along the gradient direction, reflectionless spatial-spectral modulation and sound enhancement are achieved in simulation. Such phenomenon, which we call as absorptive trapped rainbow, results from the balanced interplay among the local resonance inside individual holes, the mutual coupling of adjacent unit cells, and the inherent losses due to thermal conductivity and viscosity. This study deepens the understanding of the SSAWs propagation at a lossy metasurface and may contribute to the practical design of acoustic devices for high performance sensing and filtering.

  6. Ares I Scale Model Acoustic Tests Instrumentation for Acoustic and Pressure Measurements

    NASA Technical Reports Server (NTRS)

    Vargas, Magda B.; Counter, Douglas D.

    2011-01-01

    The Ares I Scale Model Acoustic Test (ASMAT) was a development test performed at the Marshall Space Flight Center (MSFC) East Test Area (ETA) Test Stand 116. The test article included a 5% scale Ares I vehicle model and tower mounted on the Mobile Launcher. Acoustic and pressure data were measured by approximately 200 instruments located throughout the test article. There were four primary ASMAT instrument suites: ignition overpressure (IOP), lift-off acoustics (LOA), ground acoustics (GA), and spatial correlation (SC). Each instrumentation suite incorporated different sensor models which were selected based upon measurement requirements. These requirements included the type of measurement, exposure to the environment, instrumentation check-outs and data acquisition. The sensors were attached to the test article using different mounts and brackets dependent upon the location of the sensor. This presentation addresses the observed effect of the sensors and mounts on the acoustic and pressure measurements.

  7. Acoustic performance of low pressure axial fan rotors with different blade chord length and radial load distribution

    NASA Astrophysics Data System (ADS)

    Carolus, Thomas

    The paper examines the acoustic and aerodynamic performance of low-pressure axial fan rotors with a hub/tip ratio of 0.45. Six rotors were designed for the same working point by means of the well-known airfoil theory. The condition of an equilibrium between the static pressure gradient and the centrifugal forces is maintained. All rotors have unequally spaced blades to diminish tonal noise. The rotors are tested in a short cylindrical housing without guide vanes. All rotors show very similar flux-pressure difference characteristics. The peak efficiency and the noise performance is considerably influenced by the chosen blade design. The aerodynamically and acoustically optimal rotor is the one with the reduced load at the hub and increased load in the tip region under satisfied equilibrium conditions. It runs at the highest aerodynamic efficiency, and its noise spectrum is fairly smooth. The overall sound pressure level of this rotor is up to 8 dB (A) lower compared to the other rotors under consideration.

  8. TU-F-CAMPUS-I-04: Head-Only Asymmetric Gradient System Evaluation: ACR Image Quality and Acoustic Noise

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

    Weavers, P; Shu, Y; Tao, S

    Purpose: A high-performance head-only magnetic resonance imaging gradient system with an acquisition volume of 26 cm employing an asymmetric design for the transverse coils has been developed. It is able to reach a magnitude of 85 mT/m at a slew rate of 700 T/m/s, but operated at 80 mT/m and 500 T/m/s for this test. A challenge resulting from this asymmetric design is that the gradient nonlinearly exhibits both odd- and even-ordered terms, and as the full imaging field of view is often used, the nonlinearity is pronounced. The purpose of this work is to show the system can producemore » clinically useful images after an on-site gradient nonlinearity calibration and correction, and show that acoustic noise levels fall within non-significant risk (NSR) limits for standard clinical pulse sequences. Methods: The head-only gradient system was inserted into a standard 3T wide-bore scanner without acoustic damping. The ACR phantom was scanned in an 8-channel receive-only head coil and the standard American College of Radiology (ACR) MRI quality control (QC) test was performed. Acoustic noise levels were measured for several standard pulse sequences. Results: Images acquired with the head-only gradient system passed all ACR MR image quality tests; Both even and odd-order gradient distortion correction terms were required for the asymmetric gradients to pass. Acoustic noise measurements were within FDA NSR guidelines of 99 dBA (with assumed 20 dBA hearing protection) A-weighted and 140 dB for peak for all but one sequence. Note the gradient system was installed without any shroud or acoustic batting. We expect final system integration to greatly reduce noise experienced by the patient. Conclusion: A high-performance head-only asymmetric gradient system operating at 80 mT/m and 500 T/m/s conforms to FDA acoustic noise limits in all but one case, and passes all the ACR MR image quality control tests. This work was supported in part by the NIH grant 5R01EB010065.« less

  9. Theory of acoustic radiation pressure for actual fluids

    NASA Astrophysics Data System (ADS)

    Doinikov, Alexander A.

    1996-12-01

    A body irradiated by a sound field is known to experience a steady force that is called the acoustic radiation pressure. This force plays an important role in many physical phenomena, such as cavitation, sonoluminescence, acoustic levitation, etc. The existing theory of acoustic radiation pressure neglects dissipative effects. The present paper develops a theory that takes these effects into account, both dissipative mechanisms, viscous and thermal, being considered. It is shown that, when they are no longer negligible, the dissipative effects drastically change the radiation pressure. As a result, its magnitude and sign become different from those predicted by the ``classical'' theory neglecting losses.

  10. Semicircular Canal Pressure Changes During High-intensity Acoustic Stimulation.

    PubMed

    Maxwell, Anne K; Banakis Hartl, Renee M; Greene, Nathaniel T; Benichoux, Victor; Mattingly, Jameson K; Cass, Stephen P; Tollin, Daniel J

    2017-08-01

    Acoustic stimulation generates measurable sound pressure levels in the semicircular canals. High-intensity acoustic stimuli can cause hearing loss and balance disruptions. To examine the propagation of acoustic stimuli to the vestibular end-organs, we simultaneously measured fluid pressure in the cochlea and semicircular canals during both air- and bone-conducted sound presentation. Five full-cephalic human cadaveric heads were prepared bilaterally with a mastoidectomy and extended facial recess. Vestibular pressures were measured within the superior, lateral, and posterior semicircular canals, and referenced to intracochlear pressure within the scala vestibuli with fiber-optic pressure probes. Pressures were measured concurrently with laser Doppler vibrometry measurements of stapes velocity during stimulation with both air- and bone-conduction. Stimuli were pure tones between 100 Hz and 14 kHz presented with custom closed-field loudspeakers for air-conducted sounds and via commercially available bone-anchored device for bone-conducted sounds. Pressures recorded in the superior, lateral, and posterior semicircular canals in response to sound stimulation were equal to or greater in magnitude than those recorded in the scala vestibuli (up to 20 dB higher). The pressure magnitudes varied across canals in a frequency-dependent manner. High sound pressure levels were recorded in the semicircular canals with sound stimulation, suggesting that similar acoustical energy is transmitted to the semicircular canals and the cochlea. Since these intralabyrinthine pressures exceed intracochlear pressure levels, our results suggest that the vestibular end-organs may also be at risk for injury during exposure to high-intensity acoustic stimuli known to cause trauma in the auditory system.

  11. Influences of a temperature gradient and fluid inertia on acoustic streaming in a standing wave.

    PubMed

    Thompson, Michael W; Atchley, Anthony A; Maccarone, Michael J

    2005-04-01

    Following the experimental method of Thompson and Atchley [J. Acoust. Soc. Am. 117, 1828-1838 (2005)] laser Doppler anemometry (LDA) is used to investigate the influences of a thermoacoustically induced axial temperature gradient and of fluid inertia on the acoustic streaming generated in a cylindrical standing-wave resonator filled with air driven sinusoidally at a frequency of 308 Hz. The axial component of Lagrangian streaming velocity is measured along the resonator axis and across the diameter at acoustic-velocity amplitudes of 2.7, 4.3, 6.1, and 8.6 m/s at the velocity antinodes. The magnitude of the axial temperature gradient along the resonator wall is varied between approximately 0 and 8 K/m by repeating measurements with the resonator either surrounded by a water jacket, suspended within an air-filled tank, or wrapped in foam insulation. A significant correlation is observed between the temperature gradient and the behavior of the streaming: as the magnitude of the temperature gradient increases, the magnitude of the streaming decreases and the shape of the streaming cell becomes increasingly distorted. The observed steady-state streaming velocities are not in agreement with any available theory.

  12. System for Manipulating Drops and Bubbles Using Acoustic Radiation Pressure

    NASA Technical Reports Server (NTRS)

    Oeftering, Richard C. (Inventor)

    1999-01-01

    The manipulation and control of drops of liquid and gas bubbles is achieved using high intensity acoustics in the form of and/or acoustic radiation pressure and acoustic streaming. generated by a controlled wave emission from a transducer. Acoustic radiation pressure is used to deploy or dispense drops into a liquid or a gas or bubbles into a liquid at zero or near zero velocity from the discharge end of a needle such as a syringe needle. Acoustic streaming is useful in manipulating the drop or bubble during or after deployment. Deployment and discharge is achieved by focusing the acoustic radiation pressure on the discharge end of the needle, and passing the acoustic waves through the fluid in the needle. through the needle will itself, or coaxially through the fluid medium surrounding the needle. Alternatively, the acoustic waves can be counter-deployed by focusing on the discharge end of the needle from a transducer axially aligned with the needle, but at a position opposite the needle, to prevent premature deployment of the drop or bubble. The acoustic radiation pressure can also be used for detecting the presence or absence of a drop or a bubble at the tip of a needle or for sensing various physical characteristics of the drop or bubble such as size or density.

  13. Ares I Scale Model Acoustic Test Instrumentation for Acoustic and Pressure Measurements

    NASA Technical Reports Server (NTRS)

    Vargas, Magda B.; Counter, Douglas

    2011-01-01

    Ares I Scale Model Acoustic Test (ASMAT) is a 5% scale model test of the Ares I vehicle, launch pad and support structures conducted at MSFC to verify acoustic and ignition environments and evaluate water suppression systems Test design considerations 5% measurements must be scaled to full scale requiring high frequency measurements Users had different frequencies of interest Acoustics: 200 - 2,000 Hz full scale equals 4,000 - 40,000 Hz model scale Ignition Transient: 0 - 100 Hz full scale equals 0 - 2,000 Hz model scale Environment exposure Weather exposure: heat, humidity, thunderstorms, rain, cold and snow Test environments: Plume impingement heat and pressure, and water deluge impingement Several types of sensors were used to measure the environments Different instrument mounts were used according to the location and exposure to the environment This presentation addresses the observed effects of the selected sensors and mount design on the acoustic and pressure measurements

  14. Apparent Negative Reflection with the Gradient Acoustic Metasurface by Integrating Supercell Periodicity into the Generalized Law of Reflection.

    PubMed

    Liu, Bingyi; Zhao, Wenyu; Jiang, Yongyuan

    2016-12-05

    As the two dimensional version of the functional wavefront manipulation metamaterial, metasurface has become a research hot spot for engineering the wavefront at will with a subwavelength thickness. The wave scattered by the gradient metasurface, which is composed by the periodic supercells, is governed by the generalized Snell's law. However, the critical angle that derived from the generalized Snell's law circles the domain of the incident angles that allow the occurrence of the anomalous reflection and refraction, and no free space scattering waves could exist when the incident angle is beyond the critical angle. Here we theoretically demonstrate that apparent negative reflection can be realized by a gradient acoustic metasurface when the incident angle is beyond the critical angle. The underlying mechanism of the apparent negative reflection is understood as the higher order diffraction arising from the interaction between the local phase modulation and the non-local effects introduced by the supercell periodicity. The apparent negative reflection phenomena has been perfectly verified by the calculated scattered acoustic waves of the reflected gradient acoustic metasurface. This work may provide new freedom in designing functional acoustic signal modulation devices, such as acoustic isolator and acoustic illusion device.

  15. Apparent Negative Reflection with the Gradient Acoustic Metasurface by Integrating Supercell Periodicity into the Generalized Law of Reflection

    PubMed Central

    Liu, Bingyi; Zhao, Wenyu; Jiang, Yongyuan

    2016-01-01

    As the two dimensional version of the functional wavefront manipulation metamaterial, metasurface has become a research hot spot for engineering the wavefront at will with a subwavelength thickness. The wave scattered by the gradient metasurface, which is composed by the periodic supercells, is governed by the generalized Snell’s law. However, the critical angle that derived from the generalized Snell’s law circles the domain of the incident angles that allow the occurrence of the anomalous reflection and refraction, and no free space scattering waves could exist when the incident angle is beyond the critical angle. Here we theoretically demonstrate that apparent negative reflection can be realized by a gradient acoustic metasurface when the incident angle is beyond the critical angle. The underlying mechanism of the apparent negative reflection is understood as the higher order diffraction arising from the interaction between the local phase modulation and the non-local effects introduced by the supercell periodicity. The apparent negative reflection phenomena has been perfectly verified by the calculated scattered acoustic waves of the reflected gradient acoustic metasurface. This work may provide new freedom in designing functional acoustic signal modulation devices, such as acoustic isolator and acoustic illusion device. PMID:27917909

  16. Two-dimensional water acoustic waveguide based on pressure compensation method

    NASA Astrophysics Data System (ADS)

    Zheng, Mingye; Chen, Yi; Liu, Xiaoning; Hu, Gengkai

    2018-02-01

    A two-dimensional (2D) waveguide is a basic facility for experiment measurement due to a much more simplified wave field pattern than that in free space. A waveguide for airborne sound is easily achieved with almost any solid plates. However, the design of a 2D water acoustic waveguide is still challenging because of unavailable solids with a sufficient large impedance difference from water. In this work, a new method of constructing a 2D water acoustic waveguide is proposed based on pressure compensation and has been verified by numerical simulation. A prototype of the water acoustic waveguide is fabricated and complemented by an acoustic pressure scanning system; the measured scattered pressure fields by air and aluminum cylinders both agree quite well with numerical simulations. Most acoustic pressure fields within a frequency range 7 kHz-15 kHz can be measured in this waveguide when the required scanning region is smaller than the aluminum plate area (1800 mm × 800 mm).

  17. Acoustics of the piezo-electric pressure probe

    NASA Technical Reports Server (NTRS)

    Dutt, G. S.

    1974-01-01

    Acoustical properties of a piezoelectric device are reported for measuring the pressure in the plasma flow from an MPD arc. A description and analysis of the acoustical behavior in a piezoelectric probe is presented for impedance matching and damping. The experimental results are presented in a set of oscillographic records.

  18. Pressure gradients fail to predict diffusio-osmosis

    NASA Astrophysics Data System (ADS)

    Liu, Yawei; Ganti, Raman; Frenkel, Daan

    2018-05-01

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

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

    PubMed

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

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

  20. Manipulating Liquids With Acoustic Radiation Pressure Phased Arrays

    NASA Technical Reports Server (NTRS)

    Oeftering, Richard C.

    1999-01-01

    High-intensity ultrasound waves can produce the effects of "Acoustic Radiation Pressure" (ARP) and "acoustic streaming." These effects can be used to propel liquid flows and to apply forces that can be used to move or manipulate floating objects or liquid surfaces. NASA's interest in ARP includes the remote-control agitation of liquids and the manipulation of bubbles and drops in liquid experiments and propellant systems. A high level of flexibility is attained by using a high-power acoustic phased array to generate, steer, and focus a beam of acoustic waves. This is called an Acoustic Radiation Pressure Phased Array, or ARPPA. In this approach, many acoustic transducer elements emit wavelets that converge into a single beam of sound waves. Electronically coordinating the timing, or "phase shift," of the acoustic waves makes it possible to form a beam with a predefined direction and focus. Therefore, a user can direct the ARP force at almost any desired point within a liquid volume. ARPPA lets experimenters manipulate objects anywhere in a test volume. This flexibility allow it to be used for multiple purposes, such as to agitate liquids, deploy and manipulate drops or bubbles, and even suppress sloshing in spacecraft propellant tanks.

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

    PubMed

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

    2018-06-06

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

  2. Numerical Investigations of High Pressure Acoustic Waves in Resonators

    NASA Technical Reports Server (NTRS)

    Athavale, Mahesh; Pindera, Maciej; Daniels, Christopher C.; Steinetz, Bruce M.

    2004-01-01

    This presentation presents work on numerical investigations of nonlinear acoustic phenomena in resonators that can generate high-pressure waves using acoustic forcing of the flow. Time-accurate simulations of the flow in a closed cone resonator were performed at different oscillation frequencies and amplitudes, and the numerical results for the resonance frequency and fluid pressure increase match the GRC experimental data well. Work on cone resonator assembly simulations has started and will involve calculations of the flow through the resonator assembly with and without acoustic excitation. A new technique for direct calculation of resonance frequency of complex shaped resonators is also being investigated. Script-driven command procedures will also be developed for optimization of the resonator shape for maximum pressure increase.

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

    NASA Technical Reports Server (NTRS)

    Ashpis, David E.; Tumin, Anatoli

    2003-01-01

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

  4. Design of Fresnel Lens-Type Multi-Trapping Acoustic Tweezers

    PubMed Central

    Tu, You-Lin; Chen, Shih-Jui; Hwang, Yean-Ren

    2016-01-01

    In this paper, acoustic tweezers which use beam forming performed by a Fresnel zone plate are proposed. The performance has been demonstrated by finite element analysis, including the acoustic intensity, acoustic pressure, acoustic potential energy, gradient force, and particle distribution. The acoustic tweezers use an ultrasound beam produced by a lead zirconate titanate (PZT) transducer operating at 2.4 MHz and 100 Vpeak-to-peak in a water medium. The design of the Fresnel lens (zone plate) is based on air reflection, acoustic impedance matching, and the Fresnel half-wave band (FHWB) theory. This acoustic Fresnel lens can produce gradient force and acoustic potential wells that allow the capture and manipulation of single particles or clusters of particles. Simulation results strongly indicate a good trapping ability, for particles under 150 µm in diameter, in the minimum energy location. This can be useful for cell or microorganism manipulation. PMID:27886050

  5. Broadband gradient impedance matching using an acoustic metamaterial for ultrasonic transducers

    NASA Astrophysics Data System (ADS)

    Li, Zheng; Yang, Dan-Qing; Liu, Shi-Lei; Yu, Si-Yuan; Lu, Ming-Hui; Zhu, Jie; Zhang, Shan-Tao; Zhu, Ming-Wei; Guo, Xia-Sheng; Wu, Hao-Dong; Wang, Xin-Long; Chen, Yan-Feng

    2017-02-01

    High-quality broadband ultrasound transducers yield superior imaging performance in biomedical ultrasonography. However, proper design to perfectly bridge the energy between the active piezoelectric material and the target medium over the operating spectrum is still lacking. Here, we demonstrate a new anisotropic cone-structured acoustic metamaterial matching layer that acts as an inhomogeneous material with gradient acoustic impedance along the ultrasound propagation direction. When sandwiched between the piezoelectric material unit and the target medium, the acoustic metamaterial matching layer provides a broadband window to support extraordinary transmission of ultrasound over a wide frequency range. We fabricated the matching layer by etching the peeled silica optical fibre bundles with hydrofluoric acid solution. The experimental measurement of an ultrasound transducer equipped with this acoustic metamaterial matching layer shows that the corresponding -6 dB bandwidth is able to reach over 100%. This new material fully enables new high-end piezoelectric materials in the construction of high-performance ultrasound transducers and probes, leading to considerably improved resolutions in biomedical ultrasonography and compact harmonic imaging systems.

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

    PubMed

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

    2018-03-02

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

  7. Time dependent inflow-outflow boundary conditions for 2D acoustic systems

    NASA Technical Reports Server (NTRS)

    Watson, Willie R.; Myers, Michael K.

    1989-01-01

    An analysis of the number and form of the required inflow-outflow boundary conditions for the full two-dimensional time-dependent nonlinear acoustic system in subsonic mean flow is performed. The explicit predictor-corrector method of MacCormack (1969) is used. The methodology is tested on both uniform and sheared mean flows with plane and nonplanar sources. Results show that the acoustic system requires three physical boundary conditions on the inflow and one on the outflow boundary. The most natural choice for the inflow boundary conditions is judged to be a specification of the vorticity, the normal acoustic impedance, and a pressure gradient-density gradient relationship normal to the boundary. Specification of the acoustic pressure at the outflow boundary along with these inflow boundary conditions is found to give consistent reliable results. A set of boundary conditions developed earlier, which were intended to be nonreflecting is tested using the current method and is shown to yield unstable results for nonplanar acoustic waves.

  8. Program for the feasibility of developing a high pressure acoustic levitator

    NASA Technical Reports Server (NTRS)

    Rey, Charles A.; Merkley, Dennis R.; Hammarlund, Gregory R.

    1988-01-01

    This is the final report for the program for the feasibility of developing a high-pressure acoustic levitator (HPAL). It includes work performed during the period from February 15, 1987 to October 26, 1987. The program was conducted for NASA under contract number NAS3-25115. The HPAL would be used for containerless processing of materials in the 1-g Earth environment. Results show that the use of increased gas pressure produces higher sound pressure levels. The harmonics produced by the acoustic source are also reduced. This provides an improvement in the capabilities of acoustic levitation in 1-g. The reported processing capabilities are directly limited by the design of the Medium Pressure Acoustic Levitator used for this study. Data show that sufficient acoustic intensities can be obtained to levitate and process a specimen of density 5 g/cu cm at 1500 C. However, it is recommended that a working engineering model of the HPAL be developed. The model would be used to establish the maximum operating parameters of furnace temperature and sample density.

  9. Pressure potential and stability analysis in an acoustical noncontact transportation

    NASA Astrophysics Data System (ADS)

    Li, J.; Liu, C. J.; Zhang, W. J.

    2017-01-01

    Near field acoustic traveling wave is one of the most popular principles in noncontact manipulations and transportations. The stability behavior is a key factor in the industrial applications of acoustical noncontact transportation. We present here an in-depth analysis of the transportation stability of a planar object levitated in near field acoustic traveling waves. To more accurately describe the pressure distributions on the radiation surface, a 3D nonlinear traveling wave model is presented. A closed form solution is derived based on the pressure potential to quantitatively calculate the restoring forces and moments under small disturbances. The physical explanations of the effects of fluid inertia and the effects of non-uniform pressure distributions are provided in detail. It is found that a vibration rail with tapered cross section provides more stable transportation than a rail with rectangular cross section. The present study sheds light on the issue of quantitative evaluation of stability in acoustic traveling waves and proposes three main factors that influence the stability: (a) vibration shape, (b) pressure distribution and (c) restoring force/moment. It helps to provide a better understanding of the physics behind the near field acoustic transportation and provide useful design and optimization tools for industrial applications.

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

    NASA Technical Reports Server (NTRS)

    Ashpis, David E.; Tumin, Anatoli

    2003-01-01

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

  11. Model helicopter rotor high-speed impulsive noise: Measured acoustics and blade pressures

    NASA Technical Reports Server (NTRS)

    Boxwell, D. A.; Schmitz, F. H.; Splettstoesser, W. R.; Schultz, K. J.

    1983-01-01

    A 1/17-scale research model of the AH-1 series helicopter main rotor was tested. Model-rotor acoustic and simultaneous blade pressure data were recorded at high speeds where full-scale helicopter high-speed impulsive noise levels are known to be dominant. Model-rotor measurements of the peak acoustic pressure levels, waveform shapes, and directively patterns are directly compared with full-scale investigations, using an equivalent in-flight technique. Model acoustic data are shown to scale remarkably well in shape and in amplitude with full-scale results. Model rotor-blade pressures are presented for rotor operating conditions both with and without shock-like discontinuities in the radiated acoustic waveform. Acoustically, both model and full-scale measurements support current evidence that above certain high subsonic advancing-tip Mach numbers, local shock waves that exist on the rotor blades ""delocalize'' and radiate to the acoustic far-field.

  12. Echo planar imaging at 4 Tesla with minimum acoustic noise.

    PubMed

    Tomasi, Dardo G; Ernst, Thomas

    2003-07-01

    To minimize the acoustic sound pressure levels of single-shot echo planar imaging (EPI) acquisitions on high magnetic field MRI scanners. The resonance frequencies of gradient coil vibrations, which depend on the coil length and the elastic properties of the materials in the coil assembly, were measured using piezoelectric transducers. The frequency of the EPI-readout train was adjusted to avoid the frequency ranges of mechanical resonances. Our MRI system exhibited two sharp mechanical resonances (at 720 and 1220 Hz) that can increase vibrational amplitudes up to six-fold. A small adjustment of the EPI-readout frequency made it possible to reduce the sound pressure level of EPI-based perfusion and functional MRI scans by 12 dB. Normal vibrational modes of MRI gradient coils can dramatically increase the sound pressure levels during echo planar imaging (EPI) scans. To minimize acoustic noise, the frequency of EPI-readout trains and the resonance frequencies of gradient coil vibrations need to be different. Copyright 2003 Wiley-Liss, Inc.

  13. Accurate pressure gradient calculations in hydrostatic atmospheric models

    NASA Technical Reports Server (NTRS)

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

    1987-01-01

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

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

    NASA Astrophysics Data System (ADS)

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

    2016-04-01

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

  15. Tongue-Palate Contact Pressure, Oral Air Pressure, and Acoustics of Clear Speech

    ERIC Educational Resources Information Center

    Searl, Jeff; Evitts, Paul M.

    2013-01-01

    Purpose: The authors compared articulatory contact pressure (ACP), oral air pressure (Po), and speech acoustics for conversational versus clear speech. They also assessed the relationship of these measures to listener perception. Method: Twelve adults with normal speech produced monosyllables in a phrase using conversational and clear speech.…

  16. Pressure Gradient Effects on Hypersonic Cavity Flow Heating

    NASA Technical Reports Server (NTRS)

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

    2006-01-01

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

  17. Pressure Gradient Effects on Hypersonic Cavity Flow Heating

    NASA Technical Reports Server (NTRS)

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

    2007-01-01

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

  18. Surface acoustic wave oxygen pressure sensor

    NASA Technical Reports Server (NTRS)

    Oglesby, Donald M. (Inventor); Upchurch, Billy T. (Inventor); Leighty, Bradley D. (Inventor)

    1994-01-01

    A transducer for the measurement of absolute gas-state oxygen pressure from pressures of less than 100 Pa to atmospheric pressure (1.01 x 10(exp 5) Pa) is based on a standard surface acoustic wave (SAW) device. The piezoelectric material of the SAW device is coated with a compound which will selectively and reversibly bind oxygen. When oxygen is bound by the coating, the mass of the coating increases by an amount equal to the mass of the bound oxygen. Such an increase in the mass of the coating causes a corresponding decrease in the resonant frequency of the SAW device.

  19. Considerations for acoustic emission monitoring of spherical Kevlar/epoxy composite pressure vessels

    NASA Technical Reports Server (NTRS)

    Hamstad, M. A.; Patterson, R. G.

    1977-01-01

    We are continuing to research the applications of acoustic emission testing for predicting burst pressure of filament-wound Kevlar 49/epoxy pressure vessels. This study has focused on three specific areas. The first area involves development of an experimental technique and the proper instrumentation to measure the energy given off by the acoustic emission transducer per acoustic emission burst. The second area concerns the design of a test fixture in which to mount the composite vessel so that the acoustic emission transducers are held against the outer surface of the composite. Included in this study area is the calibration of the entire test setup including couplant, transducer, electronics, and the instrument measuring the energy per burst. In the third and final area of this study, we consider the number, location, and sensitivity of the acoustic emission transducers used for proof testing composite pressure vessels.

  20. Acoustic pressure wound therapy to facilitate granulation tissue in sacral pressure ulcers in patients with compromised mobility: a case series.

    PubMed

    Schmuckler, Jo

    2008-08-01

    Electrical stimulation and other modalities are recommended for treatment of pressure ulcers in spinal cord injury patients but their use may be limited by clinical contraindications such as necrosis and infection. Acoustic pressure wound therapy can be used to address infection and has no known contraindications related to wound status. A retrospective nonconsecutive study was conducted involving five inpatients with sacral pressure ulcers and compromised mobility (spinal cord injury, ventilator/mobility dependency, or persistent vegetative state) treated with acoustic pressure wound therapy three times per week, 4 to 6 minutes per session, for 5 weeks to 5.5 months. Acoustic pressure wound therapy was administered until necrotic tissue was removed, granulation was complete, drainage resolved to moderate levels, and wound size was compatible with indications for high-voltage electrical stimulation. Within 1 to 4 weeks of starting acoustic pressure wound therapy, four out of five wounds with substantial yellow slough or eschar demonstrated 100% granulation tissue and wound area and volume decreased 71% to 97% and 75% to 99%, respectively. Subsequent treatments included electrical stimulation alone (three patients) or in conjunction with negative pressure wound therapy (one patient), and silver foam (one patient). Acoustic pressure wound therapy was found to be an effective option in preparing wounds for subsequent therapy.

  1. Acoustic emission testing of 12-nickel maraging steel pressure vessels

    NASA Technical Reports Server (NTRS)

    Dunegan, H. L.

    1973-01-01

    Acoustic emission data were obtained from three point bend fracture toughness specimens of 12-nickel maraging steel, and two pressure vessels of the same material. One of the pressure vessels contained a prefabricated flaw which was extended and sharpened by fatigue cycling. It is shown that the flawed vessel had similar characteristics to the fracture specimens, thereby allowing estimates to be made of its nearness to failure during a proof test. Both the flawed and unflawed pressure vessel survived the proof pressure and 5 cycles to the working pressure, but it was apparent from the acoustic emission response during the proof cycle and the 5 cycles to the working pressure that the flawed vessel was very near failure. The flawed vessel did not survive a second cycle to the proof pressure before failure due to flaw extension through the wall (causing a leak).

  2. Pressure gradient induced generation of microbubbles

    NASA Astrophysics Data System (ADS)

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

    2015-11-01

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

  3. Evolution of a Planar Wake in Adverse Pressure Gradient

    NASA Technical Reports Server (NTRS)

    Driver, David M.; Mateer, George G.

    2016-01-01

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

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

    NASA Technical Reports Server (NTRS)

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

    2000-01-01

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

  5. Enhanced acoustic sensing through wave compression and pressure amplification in anisotropic metamaterials.

    PubMed

    Chen, Yongyao; Liu, Haijun; Reilly, Michael; Bae, Hyungdae; Yu, Miao

    2014-10-15

    Acoustic sensors play an important role in many areas, such as homeland security, navigation, communication, health care and industry. However, the fundamental pressure detection limit hinders the performance of current acoustic sensing technologies. Here, through analytical, numerical and experimental studies, we show that anisotropic acoustic metamaterials can be designed to have strong wave compression effect that renders direct amplification of pressure fields in metamaterials. This enables a sensing mechanism that can help overcome the detection limit of conventional acoustic sensing systems. We further demonstrate a metamaterial-enhanced acoustic sensing system that achieves more than 20 dB signal-to-noise enhancement (over an order of magnitude enhancement in detection limit). With this system, weak acoustic pulse signals overwhelmed by the noise are successfully recovered. This work opens up new vistas for the development of metamaterial-based acoustic sensors with improved performance and functionalities that are highly desirable for many applications.

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

    PubMed

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

    2016-01-01

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

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

    NASA Technical Reports Server (NTRS)

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

    1997-01-01

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

  8. Acoustic propagation in rigid ducts with blockage

    NASA Technical Reports Server (NTRS)

    El-Raheb, M.; Wagner, P.

    1982-01-01

    Acoustic levitation has been suggested for moving nonmagnetic material in furnaces for heat processing in space experiments. Basically, acoustic standing waves under resonant conditions are excited in the cavity of the furnace while the material blockage is located at a pressure node and thus at a maximum gradient. The position of the blockage is controlled by displacing the node as a result of frequency change. The present investigation is concerned with the effect of blockage on the longitudinal and transverse resonances of a cylindrical cavity, taking into account the results of a one-dimensional and three-dimensional (3-D) analysis. Based on a Green's function surface element method, 3-D analysis is tested experimentally and proved to be accurate over a wide range of geometric parameters and boundary shapes. The shift in resonance depends on the change in pressure gradient and duct shortening caused by the blockage.

  9. Negative pressure wound therapy combined with acoustic pressure wound therapy for infected post surgery wounds: a case series.

    PubMed

    Howell-Taylor, Melania; Hall, Macy G; Brownlee Iii, William J; Taylor, Mary

    2008-09-01

    Acute infection of surgical incision sites often requires specialized wound care in preparation for surgical closure. Optimal therapy for preparing such wounds for a secondary closure procedure remains uncertain. The authors report wound outcomes after administering acoustic pressure wound therapy in conjunction with negative pressure wound therapy with reticulated open-cell foam dressing changes to assist with bacteria removal from open, infected surgical-incision sites in preparation for secondary surgical closure in three patients. Before incorporating acoustic pressure wound therapy at the authors' facility, the average negative pressure wound therapy with reticulated open-cell foam dressing course prior to secondary surgical closure was 30 days; with its addition, two of three patients underwent successful surgical closure with no postoperative complications after 21 and 14 days, respectively; one patient succumbed to nonwound-related complications before wound closure. Larger, prospective studies are needed to evaluate combining negative pressure wound therapy with reticulated open-cell foam dressing and acoustic pressure wound therapy for infected, acute post surgery wounds.

  10. A Spherically-Shaped PZT Thin Film Ultrasonic Transducer with an Acoustic Impedance Gradient Matching Layer Based on a Micromachined Periodically Structured Flexible Substrate

    PubMed Central

    Feng, Guo-Hua; Liu, Wei-Fan

    2013-01-01

    This paper presents the microfabrication of an acoustic impedance gradient matching layer on a spherically-shaped piezoelectric ultrasonic transducer. The acoustic matching layer can be designed to achieve higher acoustic energy transmission and operating bandwidth. Also included in this paper are a theoretical analysis of the device design and a micromachining technique to produce the novel transducer. Based on a design of a lead titanium zirconium (PZT) micropillar array, the constructed gradient acoustic matching layer has much better acoustic transmission efficiency within a 20–50 MHz operation range compared to a matching layer with a conventional quarter-wavelength thickness Parylene deposition. To construct the transducer, periodic microcavities are built on a flexible copper sheet, and then the sheet forms a designed curvature with a ball shaping. After PZT slurry deposition, the constructed PZT micropillar array is released onto a curved thin PZT layer. Following Parylene conformal coating on the processed PZT micropillars, the PZT micropillars and the surrounding Parylene comprise a matching layer with gradient acoustic impedance. By using the proposed technique, the fabricated transducer achieves a center frequency of 26 MHz and a −6 dB bandwidth of approximately 65%. PMID:24113683

  11. A spherically-shaped PZT thin film ultrasonic transducer with an acoustic impedance gradient matching layer based on a micromachined periodically structured flexible substrate.

    PubMed

    Feng, Guo-Hua; Liu, Wei-Fan

    2013-10-09

    This paper presents the microfabrication of an acoustic impedance gradient matching layer on a spherically-shaped piezoelectric ultrasonic transducer. The acoustic matching layer can be designed to achieve higher acoustic energy transmission and operating bandwidth. Also included in this paper are a theoretical analysis of the device design and a micromachining technique to produce the novel transducer. Based on a design of a lead titanium zirconium (PZT) micropillar array, the constructed gradient acoustic matching layer has much better acoustic transmission efficiency within a 20-50 MHz operation range compared to a matching layer with a conventional quarter-wavelength thickness Parylene deposition. To construct the transducer, periodic microcavities are built on a flexible copper sheet, and then the sheet forms a designed curvature with a ball shaping. After PZT slurry deposition, the constructed PZT micropillar array is released onto a curved thin PZT layer. Following Parylene conformal coating on the processed PZT micropillars, the PZT micropillars and the surrounding Parylene comprise a matching layer with gradient acoustic impedance. By using the proposed technique, the fabricated transducer achieves a center frequency of 26 MHz and a -6 dB bandwidth of approximately 65%.

  12. Acoustic pressure measurement of pulsed ultrasound using acousto-optic diffraction

    NASA Astrophysics Data System (ADS)

    Jia, Lecheng; Chen, Shili; Xue, Bin; Wu, Hanzhong; Zhang, Kai; Yang, Xiaoxia; Zeng, Zhoumo

    2018-01-01

    Compared with continuous ultrasound wave, pulsed ultrasound has been widely used in ultrasound imaging. The aim of this work is to show the applicability of acousto-optic diffraction on pulsed ultrasound transducer. In this paper, acoustic pressure of two ultrasound transducers is measured based on Raman-Nath diffraction. The frequencies of transducers are 5MHz and 10MHz. The pulse-echo method and simulation data are used to evaluate the results. The results show that the proposed method is capable to measure the absolute sound pressure. We get a sectional view of acoustic pressure using a displacement platform as an auxiliary. Compared with the traditional sound pressure measurement methods, the proposed method is non-invasive with high sensitivity and spatial resolution.

  13. Estimation of pressure gradients at renal artery stenoses

    NASA Astrophysics Data System (ADS)

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

    2003-05-01

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

  14. Acoustics and Surface Pressure Measurements from Tandem Cylinder Configurations

    NASA Technical Reports Server (NTRS)

    Hutcheson, Florence V.; Brooks, Thomas F.; Lockard, David P.; Choudhari, Meelan M.; Stead, Daniel J.

    2014-01-01

    Acoustic and unsteady surface pressure measurements from two cylinders in tandem configurations were acquired to study the effect of spacing, surface trip and freestream velocity on the radiated noise. The Reynolds number ranged from 1.15x10(exp 5) to 2.17x10(exp 5), and the cylinder spacing varied between 1.435 and 3.7 cylinder diameters. The acoustic and surface pressure spectral characteristics associated with the different flow regimes produced by the cylinders' wake interference were identified. The dependence of the Strouhal number, peak Sound Pressure Level and spanwise coherence on cylinder spacing and flow velocity was examined. Directivity measurements were performed to determine how well the dipole assumption for the radiation of vortex shedding noise holds for the largest and smallest cylinder spacing tested.

  15. One-dimensional pressure transfer models for acoustic-electric transmission channels

    NASA Astrophysics Data System (ADS)

    Wilt, K. R.; Lawry, T. J.; Scarton, H. A.; Saulnier, G. J.

    2015-09-01

    A method for modeling piezoelectric-based ultrasonic acoustic-electric power and data transmission channels is presented. These channels employ piezoelectric disk transducers to convey signals across a series of physical layers using ultrasonic waves. This model decomposes the mechanical pathway of the signal into individual ultrasonic propagation layers which are generally independent of the layer's adjacent domains. Each layer is represented by a two-by-two traveling pressure wave transfer matrix which relates the forward and reverse pressure waves on one side of the layer to the pressure waves on the opposite face, where each face is assumed to be in contact with a domain of arbitrary reference acoustic impedance. A rigorous implementation of ultrasonic beam spreading is introduced and implemented within applicable domains. Compatible pressure-wave models for piezoelectric transducers are given, which relate the electric voltage and current interface of the transducer to the pressure waves on one mechanical interface while also allowing for passive acoustic loading of the secondary mechanical interface. It is also shown that the piezoelectric model's electrical interface is compatible with transmission line parameters (ABCD-parameters), allowing for connection of electronic components and networks. The model is shown to be capable of reproducing the behavior of realistic physical channels.

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

    NASA Astrophysics Data System (ADS)

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

    2016-11-01

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

  17. High-pressure liquid chromatographic gradient mixer

    DOEpatents

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

    1982-09-08

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

  18. Generation of region 1 current by magnetospheric pressure gradients

    NASA Technical Reports Server (NTRS)

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

    1994-01-01

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

  19. Micropower Mixed-signal VLSI Independent Component Analysis for Gradient Flow Acoustic Source Separation.

    PubMed

    Stanaćević, Milutin; Li, Shuo; Cauwenberghs, Gert

    2016-07-01

    A parallel micro-power mixed-signal VLSI implementation of independent component analysis (ICA) with reconfigurable outer-product learning rules is presented. With the gradient sensing of the acoustic field over a miniature microphone array as a pre-processing method, the proposed ICA implementation can separate and localize up to 3 sources in mild reverberant environment. The ICA processor is implemented in 0.5 µm CMOS technology and occupies 3 mm × 3 mm area. At 16 kHz sampling rate, ASIC consumes 195 µW power from a 3 V supply. The outer-product implementation of natural gradient and Herault-Jutten ICA update rules demonstrates comparable performance to benchmark FastICA algorithm in ideal conditions and more robust performance in noisy and reverberant environment. Experiments demonstrate perceptually clear separation and precise localization over wide range of separation angles of two speech sources presented through speakers positioned at 1.5 m from the array on a conference room table. The presented ASIC leads to a extreme small form factor and low power consumption microsystem for source separation and localization required in applications like intelligent hearing aids and wireless distributed acoustic sensor arrays.

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

    PubMed

    Nath, Saurabh; Boreyko, Jonathan B

    2016-08-23

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

  1. Investigations of High Pressure Acoustic Waves in Resonators with Seal-Like Features

    NASA Technical Reports Server (NTRS)

    Daniels, Christopher C.; Steinetz, Bruce M.; Finkbeiner, Joshua R.; Li, Xiao-Fan; Raman, Ganesh

    2004-01-01

    1) Standing waves with maximum pressures of 188 kPa have been produced in resonators containing ambient pressure air; 2) Addition of structures inside the resonator shifts the fundamental frequency and decreases the amplitude of the generated pressure waves; 3) Addition of holes to the resonator does reduce the magnitude of the acoustic waves produced, but their addition does not prohibit the generation of large magnitude non-linear standing waves; 4) The feasibility of reducing leakage using non-linear acoustics has been confirmed.

  2. Experimental determination of the particle motions associated with the low order acoustic modes in enclosures

    NASA Technical Reports Server (NTRS)

    Byrne, K. P.; Marshall, S. E.

    1983-01-01

    A procedure for experimentally determining, in terms of the particle motions, the shapes of the low order acoustic modes in enclosures is described. The procedure is based on finding differentiable functions which approximate the shape functions of the low order acoustic modes when these modes are defined in terms of the acoustic pressure. The differentiable approximating functions are formed from polynomials which are fitted by a least squares procedure to experimentally determined values which define the shapes of the low order acoustic modes in terms of the acoustic pressure. These experimentally determined values are found by a conventional technique in which the transfer functions, which relate the acoustic pressures at an array of points in the enclosure to the volume velocity of a fixed point source, are measured. The gradient of the function which approximates the shape of a particular mode in terms of the acoustic pressure is evaluated to give the mode shape in terms of the particle motion. The procedure was tested by using it to experimentally determine the shapes of the low order acoustic modes in a small rectangular enclosure.

  3. High pressure liquid chromatographic gradient mixer

    DOEpatents

    Daughton, Christian G.; Sakaji, Richard H.

    1985-01-01

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

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

    NASA Astrophysics Data System (ADS)

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

    2014-07-01

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

  5. Measured wavenumber: frequency spectrum associated with acoustic and aerodynamic wall pressure fluctuations.

    PubMed

    Arguillat, Blandine; Ricot, Denis; Bailly, Christophe; Robert, Gilles

    2010-10-01

    Direct measurements of the wavenumber-frequency spectrum of wall pressure fluctuations beneath a turbulent plane channel flow have been performed in an anechoic wind tunnel. A rotative array has been designed that allows the measurement of a complete map, 63×63 measuring points, of cross-power spectral densities over a large area. An original post-processing has been developed to separate the acoustic and the aerodynamic exciting loadings by transforming space-frequency data into wavenumber-frequency spectra. The acoustic part has also been estimated from a simple Corcos-like model including the contribution of a diffuse sound field. The measured acoustic contribution to the surface pressure fluctuations is 5% of the measured aerodynamic surface pressure fluctuations for a velocity and boundary layer thickness relevant for automotive interior noise applications. This shows that for aerodynamically induced car interior noise, both contributions to the surface pressure fluctuations on car windows have to be taken into account.

  6. Effect of static pressure on acoustic energy radiated by cavitation bubbles in viscous liquids under ultrasound.

    PubMed

    Yasui, Kyuichi; Towata, Atsuya; Tuziuti, Toru; Kozuka, Teruyuki; Kato, Kazumi

    2011-11-01

    The effect of static pressure on acoustic emissions including shock-wave emissions from cavitation bubbles in viscous liquids under ultrasound has been studied by numerical simulations in order to investigate the effect of static pressure on dispersion of nano-particles in liquids by ultrasound. The results of the numerical simulations for bubbles of 5 μm in equilibrium radius at 20 kHz have indicated that the optimal static pressure which maximizes the energy of acoustic waves radiated by a bubble per acoustic cycle increases as the acoustic pressure amplitude increases or the viscosity of the solution decreases. It qualitatively agrees with the experimental results by Sauter et al. [Ultrason. Sonochem. 15, 517 (2008)]. In liquids with relatively high viscosity (∼200 mPa s), a bubble collapses more violently than in pure water when the acoustic pressure amplitude is relatively large (∼20 bar). In a mixture of bubbles of different equilibrium radius (3 and 5 μm), the acoustic energy radiated by a 5 μm bubble is much larger than that by a 3 μm bubble due to the interaction with bubbles of different equilibrium radius. The acoustic energy radiated by a 5 μm bubble is substantially increased by the interaction with 3 μm bubbles.

  7. Investigations of High Pressure Acoustic Waves in Resonators with Seal-like Features

    NASA Technical Reports Server (NTRS)

    Daniels, Christopher; Steinetz, Bruce; Finkbeiner, Joshua

    2003-01-01

    A conical resonator (having a dissonant acoustic design) was tested in four configurations: (1) baseline resonator with closed ends and no blockage, (2) closed resonator with internal blockage, (3) ventilated resonator with no blockage, and (4) ventilated resonator with an applied pressure differential. These tests were conducted to investigate the effects of blockage and ventilation holes on dynamic pressurization. Additionally, the investigation was to determine the ability of acoustic pressurization to impede flow through the resonator. In each of the configurations studied, the entire resonator was oscillated at the gas resonant frequency while dynamic pressure, static pressure, and temperature of the fluid were measured. In the final configuration, flow through the resonator was recorded for three oscillation conditions. Ambient condition air was used as the working fluid.

  8. Acoustic beam control in biomimetic projector via velocity gradient

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

    Gao, Xiaowei; Dong, Erqian; Song, Zhongchang

    A biomimetic projector (BioP) based on computerized tomography of pygmy sperm whale's biosonar system has been designed using gradient-index (GRIN) material. The directivity of this BioP device was investigated as function of frequency and the velocity gradient of the GRIN material. A strong beam control over a broad bandwidth at the subwavelength scale has been achieved. Compared with a bare subwavelength source, the main lobe pressure of the BioP is about five times as high and the angular resolution is one order of magnitude better. Our results indicate that this BioP has excellent application potential in miniaturized underwater sonars.

  9. Acoustic beam control in biomimetic projector via velocity gradient

    NASA Astrophysics Data System (ADS)

    Gao, Xiaowei; Zhang, Yu; Cao, Wenwu; Dong, Erqian; Song, Zhongchang; Li, Songhai; Tang, Liguo; Zhang, Sai

    2016-07-01

    A biomimetic projector (BioP) based on computerized tomography of pygmy sperm whale's biosonar system has been designed using gradient-index (GRIN) material. The directivity of this BioP device was investigated as function of frequency and the velocity gradient of the GRIN material. A strong beam control over a broad bandwidth at the subwavelength scale has been achieved. Compared with a bare subwavelength source, the main lobe pressure of the BioP is about five times as high and the angular resolution is one order of magnitude better. Our results indicate that this BioP has excellent application potential in miniaturized underwater sonars.

  10. Deflecting Rayleigh surface acoustic waves by a meta-ridge with a gradient phase shift

    NASA Astrophysics Data System (ADS)

    Xu, Yanlong; Yang, Zhichun; Cao, Liyun

    2018-05-01

    We propose a non-resonant meta-ridge to deflect Rayleigh surface acoustic waves (RSAWs) according to the generalized Snell’s law with a gradient phase shift. The gradient phase shift is predicted by an analytical formula, which is related to the path length of the traveling wave. The non-resonant meta-ridge is designed based on the characteristics of the RSAW: it only propagates along the interface with a penetration depth, and it is dispersion-free with a constant phase velocity. To guarantee that the characteristics are still valid when RSAWs propagate in a three-dimensional (3D) structure, grooves are employed to construct the supercell of the meta-ridge. The horizontal length, inclined angle, and thickness of the ridge, along with the filling ratio of the groove, are parametrically examined step by step to investigate their influences on the propagation of RSAWs. The final 3D meta-ridges are designed theoretically and their capability of deflecting the incident RSAWs are validated numerically. The study presents a new method to control the trajectory of RSAWs, which will be conducive to developing innovative devices for surface acoustic waves.

  11. Manipulation of Liquids Using Phased Array Generation of Acoustic Radiation Pressure

    NASA Technical Reports Server (NTRS)

    Oeftering, Richard C. (Inventor)

    2000-01-01

    A phased array of piezoelectric transducers is used to control and manipulate contained as well as uncontained fluids in space and earth applications. The transducers in the phased array are individually activated while being commonly controlled to produce acoustic radiation pressure and acoustic streaming. The phased array is activated to produce a single pulse, a pulse burst or a continuous pulse to agitate, segregate or manipulate liquids and gases. The phased array generated acoustic radiation pressure is also useful in manipulating a drop, a bubble or other object immersed in a liquid. The transducers can be arranged in any number of layouts including linear single or multi- dimensional, space curved and annular arrays. The individual transducers in the array are activated by a controller, preferably driven by a computer.

  12. Analyses of Sea Surface Height, Bottom Pressure and Acoustic Travel Time in the Japan/East Sea

    DTIC Science & Technology

    2006-01-01

    ANALYSES OF SEA SURFACE HEIGHT, BOTTOM PRESSURE AND ACOUSTIC TRAVEL TIME IN THE JAPAN/EAST SEA BY YONGSHENG XU A DISSERTATION SUBMITTED IN PARTIAL...COVERED 00-00-2006 to 00-00-2006 4. TITLE AND SUBTITLE Analyses of Sea Surface Height, Bottom Pressure and Acoustic Travel Time in the Japan/East Sea...1999 to July 2001. The PIESs recorded hourly vertical acoustic travel time and pressure, which are respectively good proxies of baroclinic and

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

    PubMed

    Fritz, Brad G; Mackley, Rob D

    2010-01-01

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

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

    NASA Technical Reports Server (NTRS)

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

    1980-01-01

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

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

    NASA Technical Reports Server (NTRS)

    El-Hady, Nabil M.

    1988-01-01

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

  16. Mean Flow Augmented Acoustics in Rocket Systems

    NASA Technical Reports Server (NTRS)

    Fischbach, Sean

    2014-01-01

    Combustion instability in solid rocket motors and liquid engines has long been a subject of concern. Many rockets display violent fluctuations in pressure, velocity, and temperature originating from the complex interactions between the combustion process and gas dynamics. Recent advances in energy based modeling of combustion instabilities require accurate determination of acoustic frequencies and mode shapes. Of particular interest is the acoustic mean flow interactions within the converging section of a rocket nozzle, where gradients of pressure, density, and velocity become large. The expulsion of unsteady energy through the nozzle of a rocket is identified as the predominate source of acoustic damping for most rocket systems. Recently, an approach to address nozzle damping with mean flow effects was implemented by French [1]. This new approach extends the work originated by Sigman and Zinn [2] by solving the acoustic velocity potential equation (AVPE) formulated by perturbing the Euler equations [3]. The present study aims to implement the French model within the COMSOL Multiphysiscs framework and analyzes one of the author's presented test cases.

  17. Inferring Pre-shock Acoustic Field From Post-shock Pitot Pressure Measurement

    NASA Astrophysics Data System (ADS)

    Wang, Jian-Xun; Zhang, Chao; Duan, Lian; Xiao, Heng; Virginia Tech Team; Missouri Univ of Sci; Tech Team

    2017-11-01

    Linear interaction analysis (LIA) and iterative ensemble Kalman method are used to convert post-shock Pitot pressure fluctuations to static pressure fluctuations in front of the shock. The LIA is used as the forward model for the transfer function associated with a homogeneous field of acoustic waves passing through a nominally normal shock wave. The iterative ensemble Kalman method is then employed to infer the spectrum of upstream acoustic waves based on the post-shock Pitot pressure measured at a single point. Several test cases with synthetic and real measurement data are used to demonstrate the merits of the proposed inference scheme. The study provides the basis for measuring tunnel freestream noise with intrusive probes in noisy supersonic wind tunnels.

  18. Modeling of Structural-Acoustic Interaction Using Coupled FE/BE Method and Control of Interior Acoustic Pressure Using Piezoelectric Actuators

    NASA Technical Reports Server (NTRS)

    Mei, Chuh; Shi, Yacheng

    1997-01-01

    A coupled finite element (FE) and boundary element (BE) approach is presented to model full coupled structural/acoustic/piezoelectric systems. The dual reciprocity boundary element method is used so that the natural frequencies and mode shapes of the coupled system can be obtained, and to extend this approach to time dependent problems. The boundary element method is applied to interior acoustic domains, and the results are very accurate when compared with limited exact solutions. Structural-acoustic problems are then analyzed with the coupled finite element/boundary element method, where the finite element method models the structural domain and the boundary element method models the acoustic domain. Results for a system consisting of an isotropic panel and a cubic cavity are in good agreement with exact solutions and experiment data. The response of a composite panel backed cavity is then obtained. The results show that the mass and stiffness of piezoelectric layers have to be considered. The coupled finite element and boundary element equations are transformed into modal coordinates, which is more convenient for transient excitation. Several transient problems are solved based on this formulation. Two control designs, a linear quadratic regulator (LQR) and a feedforward controller, are applied to reduce the acoustic pressure inside the cavity based on the equations in modal coordinates. The results indicate that both controllers can reduce the interior acoustic pressure and the plate deflection.

  19. Sound pressure level gain in an acoustic metamaterial cavity.

    PubMed

    Song, Kyungjun; Kim, Kiwon; Hur, Shin; Kwak, Jun-Hyuk; Park, Jihyun; Yoon, Jong Rak; Kim, Jedo

    2014-12-11

    The inherent attenuation of a homogeneous viscous medium limits radiation propagation, thereby restricting the use of many high-frequency acoustic devices to only short-range applications. Here, we design and experimentally demonstrate an acoustic metamaterial localization cavity which is used for sound pressure level (SPL) gain using double coiled up space like structures thereby increasing the range of detection. This unique behavior occurs within a subwavelength cavity that is 1/10(th) of the wavelength of the incident acoustic wave, which provides up to a 13 dB SPL gain. We show that the amplification results from the Fabry-Perot resonance of the cavity, which has a simultaneously high effective refractive index and effective impedance. We also experimentally verify the SPL amplification in an underwater environment at higher frequencies using a sample with an identical unit cell size. The versatile scalability of the design shows promising applications in many areas, especially in acoustic imaging and underwater communication.

  20. Sound Pressure Level Gain in an Acoustic Metamaterial Cavity

    PubMed Central

    Song, Kyungjun; Kim, Kiwon; Hur, Shin; Kwak, Jun-Hyuk; Park, Jihyun; Yoon, Jong Rak; Kim, Jedo

    2014-01-01

    The inherent attenuation of a homogeneous viscous medium limits radiation propagation, thereby restricting the use of many high-frequency acoustic devices to only short-range applications. Here, we design and experimentally demonstrate an acoustic metamaterial localization cavity which is used for sound pressure level (SPL) gain using double coiled up space like structures thereby increasing the range of detection. This unique behavior occurs within a subwavelength cavity that is 1/10th of the wavelength of the incident acoustic wave, which provides up to a 13 dB SPL gain. We show that the amplification results from the Fabry-Perot resonance of the cavity, which has a simultaneously high effective refractive index and effective impedance. We also experimentally verify the SPL amplification in an underwater environment at higher frequencies using a sample with an identical unit cell size. The versatile scalability of the design shows promising applications in many areas, especially in acoustic imaging and underwater communication. PMID:25502279

  1. Computation of Turbulent Wake Flows in Variable Pressure Gradient

    NASA Technical Reports Server (NTRS)

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

    1999-01-01

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

  2. Artificial acoustic stiffness reduction in fully compressible, direct numerical simulation of combustion

    NASA Astrophysics Data System (ADS)

    Wang, Yi; Trouvé, Arnaud

    2004-09-01

    A pseudo-compressibility method is proposed to modify the acoustic time step restriction found in fully compressible, explicit flow solvers. The method manipulates terms in the governing equations of order Ma2, where Ma is a characteristic flow Mach number. A decrease in the speed of acoustic waves is obtained by adding an extra term in the balance equation for total energy. This term is proportional to flow dilatation and uses a decomposition of the dilatational field into an acoustic component and a component due to heat transfer. The present method is a variation of the pressure gradient scaling (PGS) method proposed in Ramshaw et al (1985 Pressure gradient scaling method for fluid flow with nearly uniform pressure J. Comput. Phys. 58 361-76). It achieves gains in computational efficiencies similar to PGS: at the cost of a slightly more involved right-hand-side computation, the numerical time step increases by a full order of magnitude. It also features the added benefit of preserving the hydrodynamic pressure field. The original and modified PGS methods are implemented into a parallel direct numerical simulation solver developed for applications to turbulent reacting flows with detailed chemical kinetics. The performance of the pseudo-compressibility methods is illustrated in a series of test problems ranging from isothermal sound propagation to laminar premixed flame problems.

  3. The Derivation of the Gradient of the Acoustic Pressure on a Moving Surface for Application to the Fast Scattering Code (FSC)

    NASA Technical Reports Server (NTRS)

    Farassat, F.; Brentner, Kenneth S.

    2005-01-01

    In this paper we develop an analytic expression for calculation of the the acoustic pressure from a rotating blade on a moving surface for application to the Fast Scattering Code (FSC). The analytic result is intended to be used in the helicopter noise prediction code PSU-WOPWOP. One of the goals of the derivation is obtaining a result that will not use any more information than are needed for the prediction of the thickness and loading noise. The result derived here achieves this goal and its incorporation in PSU-WOPWOP is straight forward and attainable.

  4. Acoustic gravity microseismic pressure signal at shallow stations

    NASA Astrophysics Data System (ADS)

    Peureux, Charles; Ardhuin, Fabrice; Royer, Jean-Yves

    2017-04-01

    It has been known for decades that the background permanent seismic noise, the so-called microseimic signal, is generated by the nonlinear interaction of oppositely travelling ocean surface waves [Longuet-Higgins 1951]. It can especially be used to infer the time variability of short ocean waves statistics [Peureux and Ardhuin 2016]. However, better quantitative estimates of the latter are made difficult due to a poor knowledge of the Earth's crust characteristics, whose coupling with acoustic modes can affect large uncertainties to the frequency response at the bottom of the ocean. The pressure field at depths less than an acoustic wave length to the surface is made of evanescent acoustic-gravity modes [Cox and Jacobs 1989]. For this reason, they are less affected by the ocean bottom composition. This near field is recorded and analyzed in the frequency range 0.1 to 0.5 Hz approximately, at two locations : at a shallow site in the North-East Atlantic continental shelf and a deep water site in the Southern Indian ocean, at the ocean bottom and 100 m below sea-surface and in the upper part of the water column respectively. Evanescent and propagating Rayleigh modes are compared against theoretical predictions. Comparisons against surface waves hindcast based on WAVEWATCH(R) III modelling framework help assessing its performances and can be used to help future model improvements. References Longuet-Higgins, M. S., A Theory of the Origin of Microseisms, Philos. Trans. Royal Soc. A, The Royal Society, 1950, 243, 1-3. Peureux, C. and Ardhuin, F., Ocean bottom pressure records from the Cascadia array and short surface gravity waves, J. Geophys. Res. Oceans, 2016, 121, 2862-2873. Cox, C. S. & Jacobs, D. C., Cartesian diver observations of double frequency pressure fluctuations in the upper levels of the ocean, Geophys. Res. Lett., 1989, 16, 807-810.

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

    NASA Astrophysics Data System (ADS)

    Semenov, Semen; Schimpf, Martin

    2004-01-01

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

  6. Acoustic calibration apparatus for calibrating plethysmographic acoustic pressure sensors

    NASA Technical Reports Server (NTRS)

    Zuckerwar, Allan J. (Inventor); Davis, David C. (Inventor)

    1995-01-01

    An apparatus for calibrating an acoustic sensor is described. The apparatus includes a transmission material having an acoustic impedance approximately matching the acoustic impedance of the actual acoustic medium existing when the acoustic sensor is applied in actual in-service conditions. An elastic container holds the transmission material. A first sensor is coupled to the container at a first location on the container and a second sensor coupled to the container at a second location on the container, the second location being different from the first location. A sound producing device is coupled to the container and transmits acoustic signals inside the container.

  7. Acoustic calibration apparatus for calibrating plethysmographic acoustic pressure sensors

    NASA Technical Reports Server (NTRS)

    Zuckerwar, Allan J. (Inventor); Davis, David C. (Inventor)

    1994-01-01

    An apparatus for calibrating an acoustic sensor is described. The apparatus includes a transmission material having an acoustic impedance approximately matching the acoustic impedance of the actual acoustic medium existing when the acoustic sensor is applied in actual in-service conditions. An elastic container holds the transmission material. A first sensor is coupled to the container at a first location on the container and a second sensor coupled to the container at a second location on the container, the second location being different from the first location. A sound producing device is coupled to the container and transmits acoustic signals inside the container.

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

    NASA Astrophysics Data System (ADS)

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

    2017-06-01

    Horizontal and vertical pressure gradients may be important physical mechanisms contributing to onshore sediment transport beneath steep, near-breaking waves in the surf zone. A barred beach was constructed in a large-scale laboratory wave flume with a fixed profile containing a mobile sediment layer on the crest of the sandbar. Horizontal and vertical pore pressure gradients were obtained by finite differences of measurements from an array of pressure transducers buried within the upper several centimeters of the bed. Colocated observations of erosion depth were made during asymmetric wave trials with wave heights between 0.10 and 0.98 m, consistently resulting in onshore sheet flow sediment transport. The pore pressure gradient vector within the bed exhibited temporal rotations during each wave cycle, directed predominantly upward under the trough and then rapidly rotating onshore and downward as the wavefront passed. The magnitude of the pore pressure gradient during each phase of rotation was correlated with local wave steepness and relative depth. Momentary bed failures as deep as 20 grain diameters were coincident with sharp increases in the onshore-directed pore pressure gradients, but occurred at horizontal pressure gradients less than theoretical critical values for initiation of the motion for compact beds. An expression combining the effects of both horizontal and vertical pore pressure gradients with bed shear stress and soil stability is used to determine that failure of the bed is initiated at nonnegligible values of both forces.Plain Language SummaryThe <span class="hlt">pressure</span> <span class="hlt">gradient</span> present within the seabed beneath breaking waves may be an important physical mechanism transporting sediment. A large-scale laboratory was used to replicate realistic surfzone conditions in controlled tests, allowing for horizontal and vertical <span class="hlt">pressure</span> <span class="hlt">gradient</span> magnitudes and the resulting sediment bed response to be observed with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160007487','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160007487"><span>Receptivity of Hypersonic Boundary Layers to <span class="hlt">Acoustic</span> and Vortical Disturbances (Invited)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Balakumar, P.</p> <p>2015-01-01</p> <p>Boundary-layer receptivity to two-dimensional <span class="hlt">acoustic</span> and vortical disturbances for hypersonic flows over two-dimensional and axi-symmetric geometries were numerically investigated. The role of bluntness, wall cooling, and <span class="hlt">pressure</span> <span class="hlt">gradients</span> on the receptivity and stability were analyzed and compared with the sharp nose cases. It was found that for flows over sharp nose geometries in adiabatic wall conditions the instability waves are generated in the leading-edge region and that the boundary layer is much more receptive to slow <span class="hlt">acoustic</span> waves as compared to the fast waves. The computations confirmed the stabilizing effect of nose bluntness and the role of the entropy layer in the delay of boundary layer transition. The receptivity coefficients in flows over blunt bodies are orders of magnitude smaller than that for the sharp cone cases. Wall cooling stabilizes the first mode strongly and destabilizes the second mode. However, the receptivity coefficients are also much smaller compared to the adiabatic case. The adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> increased the unstable second mode regions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/8160828','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/8160828"><span>Intramyocardial <span class="hlt">pressure</span> <span class="hlt">gradients</span> in working and nonworking isolated cat hearts.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mihailescu, L S; Abel, F L</p> <p>1994-03-01</p> <p>This study presents an improved method for the measurement of intramyocardial <span class="hlt">pressure</span> (IMP) using the servo-nulling mechanism. Glass micropipettes (20-24 microns OD) were used as transducers, coated to increase their mechanical resistance to breakage, and placed inside the left ventricular wall with a micropipette holder and manipulator. IMP was measured at the base of the left ventricle in working and nonworking isolated cat hearts that were perfused with Krebs-Henseleit buffer. In working hearts a transmural <span class="hlt">gradient</span> of systolic IMP oriented from endocardium toward the epicardium was found; the endocardial values for systolic IMP were slightly higher than systolic left ventricular <span class="hlt">pressure</span> (LVP), by 11-18%. Increases in afterload induced increases in IMP, without changing the systolic IMP-to-LVP ratio. In nonworking hearts with drained left ventricles, the systolic transmural <span class="hlt">gradient</span> for IMP described for working hearts persisted, but at lower values, and was directly dependent on coronary perfusion <span class="hlt">pressure</span>. Systolic IMP-to-LVP ratios were always > 1. The diastolic IMP of both working and nonworking hearts exhibited irregular transmural <span class="hlt">gradients</span>. Our results support the view that generated systolic IMP is largely independent of LVP development.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020051552&hterms=DURAND&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D30%26Ntt%3DDURAND','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020051552&hterms=DURAND&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D30%26Ntt%3DDURAND"><span>Fundamentals of <span class="hlt">Acoustics</span>. Psychoacoustics and Hearing. <span class="hlt">Acoustical</span> Measurements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Begault, Durand R.; Ahumada, Al (Technical Monitor)</p> <p>1997-01-01</p> <p>These are 3 chapters that will appear in a book titled "Building <span class="hlt">Acoustical</span> Design", edited by Charles Salter. They are designed to introduce the reader to fundamental concepts of <span class="hlt">acoustics</span>, particularly as they relate to the built environment. "Fundamentals of <span class="hlt">Acoustics</span>" reviews basic concepts of sound waveform frequency, <span class="hlt">pressure</span>, and phase. "Psychoacoustics and Hearing" discusses the human interpretation sound <span class="hlt">pressure</span> as loudness, particularly as a function of frequency. "<span class="hlt">Acoustic</span> Measurements" gives a simple overview of the time and frequency weightings for sound <span class="hlt">pressure</span> measurements that are used in <span class="hlt">acoustical</span> work.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19760018239','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19760018239"><span>Response of space shuttle insulation panels to <span class="hlt">acoustic</span> noise <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>Vaicaitis, R.</p> <p>1976-01-01</p> <p>The response of reusable space shuttle insulation panels to random <span class="hlt">acoustic</span> <span class="hlt">pressure</span> fields are studied. The basic analytical approach in formulating the governing equations of motion uses a Rayleigh-Ritz technique. The input <span class="hlt">pressure</span> field is modeled as a stationary Gaussian random process for which the cross-spectral density function is known empirically from experimental measurements. The response calculations are performed in both frequency and time domain.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..DFDL22008C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..DFDL22008C"><span>Assessment of fluctuating <span class="hlt">pressure</span> <span class="hlt">gradient</span> using acceleration spectra in near wall flows</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cadel, Daniel; Lowe, K. Todd</p> <p>2015-11-01</p> <p>Separation of contributions to the fluctuating acceleration from <span class="hlt">pressure</span> <span class="hlt">gradient</span> fluctuations and viscous shear fluctuations in the frequency domain is examined in a turbulent boundary layer. Past work leveraging turbulent accelerations for <span class="hlt">pressure</span> <span class="hlt">gradient</span> measurements has neglected the viscous shear term from the momentum equation--an invalid assumption in the case of near wall flows. The present study seeks to account for the influence of the viscous shear term and spectrally reject its contribution, which is thought to be concentrated at higher frequencies. Spectra of velocity and acceleration fluctuations in a flat plate, zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> turbulent boundary layer at a momentum thickness Reynolds number of 7500 are measured using a spatially resolving three-component laser Doppler velocimeter. This canonical case data is applied for validation of the spectral approach for future application in more complex aerodynamic flows.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013APS..DFDA25002K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013APS..DFDA25002K"><span>Plasma Streamwise Vortex Generators in an Adverse <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kelley, Christopher; Corke, Thomas; Thomas, Flint</p> <p>2013-11-01</p> <p>A wind tunnel experiment was conducted to compare plasma streamwise vortex generators (PSVGs) and passive vortex generators (VGs). These devices were installed on a wing section by which the angle of attack could be used to vary the streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The experiment was performed for freestream Mach numbers 0.1-0.2. Three-dimensional velocity components were measured using a 5-hole Pitot probe in the boundary layer. These measurements were used to quantify the production of streamwise vorticity and the magnitude of the reorientation term from the vorticity transport equation. The effect of Mach number, <span class="hlt">pressure</span> <span class="hlt">gradient</span>, operating voltage, and electrode length was then investigated for the PSVGs. The results indicate that the PSVGs could easily outperform the passive VGs and provide a suitable alternative for flow control.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhSen...7..253L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhSen...7..253L"><span>Development of high sensitivity eight-element multiplexed fiber laser <span class="hlt">acoustic</span> <span class="hlt">pressure</span> hydrophone array and interrogation system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Ming; Sun, Zhihui; Zhang, Xiaolei; Li, Shujuan; Song, Zhiqiang; Wang, Meng; Guo, Jian; Ni, Jiasheng; Wang, Chang; Peng, Gangding; Xu, Xiangang</p> <p>2017-09-01</p> <p>Fiber laser hydrophones have got widespread concerns due to the unique advantages and broad application prospects. In this paper, the research results of the eight-element multiplexed fiber laser <span class="hlt">acoustic</span> <span class="hlt">pressure</span> array and the interrogation system are introduced, containing low-noise distributed feedback fiber laser (DFB-FL) fabrication, sensitivity enhancement packaging, and interferometric signal demodulation. The frequency response range of the system is 10Hz-10kHz, the laser frequency <span class="hlt">acoustic</span> <span class="hlt">pressure</span> sensitivity reaches 115 dB re Hz/Pa, and the equivalent noise <span class="hlt">acoustic</span> <span class="hlt">pressure</span> is less than 60μPa/Hz1/2. The dynamic range of the system is greater than 120 dB.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24861781','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24861781"><span>Constant <span class="hlt">pressure</span> mode extended simple <span class="hlt">gradient</span> liquid chromatography system for micro and nanocolumns.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Šesták, Jozef; Kahle, Vladislav</p> <p>2014-07-11</p> <p>Performing <span class="hlt">gradient</span> liquid chromatography at constant <span class="hlt">pressure</span> instead of constant flow rate has serious potential for shortening the analysis time and increasing the productivity of HPLC instruments that use <span class="hlt">gradient</span> methods. However, in the constant <span class="hlt">pressure</span> mode the decreasing column permeability during a long period of time negatively affects the repeatability of retention time. Thus a volume-based approach, in which the detector signal is plotted as a function of retention volume, must be taken into consideration. Traditional HPLC equipment, however, requires quite complex hardware and software modifications in order to work at constant <span class="hlt">pressure</span> and in the volume-based mode. In this short communication, a low cost and easily feasible <span class="hlt">pressure</span>-controlled extension of the previously described simple <span class="hlt">gradient</span> liquid chromatography platform is proposed. A test mixture of four nitro esters was separated by 10-60% (v/v) acetone/water <span class="hlt">gradient</span> and a high repeatability of retention volumes at 20MPa (RSD less than 0.45%) was realized. Separations were also performed at different values of <span class="hlt">pressure</span> (20, 25, and 31MPa), and only small variations of the retention volumes (up to 0.8%) were observed. In this particular case, the gain in the analysis speed of 7% compared to the constant flow mode was realized at a constant <span class="hlt">pressure</span>. Copyright © 2014 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=sound+AND+pressure+AND+level&pg=5&id=EJ427099','ERIC'); return false;" href="https://eric.ed.gov/?q=sound+AND+pressure+AND+level&pg=5&id=EJ427099"><span>Intelligibility of Telephone Speech for the Hearing Impaired When Various Microphones Are Used for <span class="hlt">Acoustic</span> Coupling.</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>Janota, Claus P.; Janota, Jeanette Olach</p> <p>1991-01-01</p> <p>Various candidate microphones were evaluated for <span class="hlt">acoustic</span> coupling of hearing aids to a telephone receiver. Results from testing by 9 hearing-impaired adults found comparable listening performance with a <span class="hlt">pressure</span> <span class="hlt">gradient</span> microphone at a 10 decibel higher level of interfering noise than with a normal <span class="hlt">pressure</span>-sensitive microphone. (Author/PB)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28296135','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28296135"><span>Assessment of trans-aortic <span class="hlt">pressure</span> <span class="hlt">gradient</span> using a coronary <span class="hlt">pressure</span> wire in patients with mechanical aortic and mitral valve prostheses.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kherada, Nisharahmed; Brenes, Juan Carlos; Kini, Annapoorna S; Dangas, George D</p> <p>2017-03-15</p> <p>Accurate evaluation of trans-aortic valvular <span class="hlt">pressure</span> <span class="hlt">gradients</span> is challenging in cases where dual mechanical aortic and mitral valve prostheses are present. Non-invasive Doppler echocardiographic imaging has its limitations due to multiple geometric assumptions. Invasive measurement of trans-valvular <span class="hlt">gradients</span> with cardiac catheterization can provide further information in patients with two mechanical valves, where simultaneous <span class="hlt">pressure</span> measurements in the left ventricle and ascending aorta must be obtained. Obtaining access to the left ventricle via the mitral valve after a trans-septal puncture is not feasible in the case of a concomitant mechanical mitral valve, whereas left ventricular apical puncture technique is associated with high procedural risks. Retrograde crossing of a bileaflet mechanical aortic prosthesis with standard catheters is associated with the risk of catheter entrapment and acute valvular regurgitation. In these cases, the assessment of trans-valvular <span class="hlt">gradients</span> using a 0.014˝ diameter coronary <span class="hlt">pressure</span> wire technique has been described in a few case reports. We present the case of a 76-year-old female with rheumatic valvular heart disease who underwent mechanical aortic and mitral valve replacement in the past. She presented with decompensated heart failure and echocardiographic findings suggestive of elevated <span class="hlt">pressure</span> <span class="hlt">gradient</span> across the mechanical aortic valve prosthesis. The use of a high-fidelity 0.014˝ diameter coronary <span class="hlt">pressure</span> guidewire resulted in the detection of a normal trans-valvular <span class="hlt">pressure</span> <span class="hlt">gradient</span> across the mechanical aortic valve. This avoided a high-risk third redo valve surgery in our patient. © 2017 Wiley Periodicals, Inc. © 2017 Wiley Periodicals, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1015062','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1015062"><span>Cryogenic Impinging Jets Subjected to High Frequency Transverse <span class="hlt">Acoustic</span> Forcing in a High <span class="hlt">Pressure</span> Environment</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2016-07-27</p> <p>Transverse <span class="hlt">Acoustic</span> Forcing in a High <span class="hlt">Pressure</span> Environment 5a. CONTRACT NUMBER 5b. GRANT NUMBER 5c. PROGRAM ELEMENT NUMBER 6. AUTHOR(S) Mario ...<span class="hlt">Acoustic</span> Forcing in a High <span class="hlt">Pressure</span> Environment Mario Roa, Sierra Lobo, Inc. Alex Schumaker, AFRL Doug Talley, AFRL 24-27 July 2016 Joint Propulsion...Distribution A: Approved for Public Release; Distribution Unlimited. PA# 16333 9 Parametric Sweep Super -Critical Results Differences between</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70179130','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70179130"><span>Barrier island breach evolution: Alongshore transport and bay-ocean <span class="hlt">pressure</span> <span class="hlt">gradient</span> interactions</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Safak, Ilgar; Warner, John C.; List, Jeffrey</p> <p>2016-01-01</p> <p>Physical processes controlling repeated openings and closures of a barrier island breach between a bay and the open ocean are studied using aerial photographs and atmospheric and hydrodynamic observations. The breach site is located on Pea Island along the Outer Banks, separating Pamlico Sound from the Atlantic Ocean. Wind direction was a major control on the <span class="hlt">pressure</span> <span class="hlt">gradients</span> between the bay and the ocean to drive flows that initiate or maintain the breach opening. Alongshore sediment flux was found to be a major contributor to breach closure. During the analysis period from 2011 to 2016, three hurricanes had major impacts on the breach. First, Hurricane Irene opened the breach with wind-driven flow from bay to ocean in August 2011. Hurricane Sandy in October 2012 quadrupled the channel width from <span class="hlt">pressure</span> <span class="hlt">gradient</span> flows due to water levels that were first higher on the ocean side and then higher on the bay side. The breach closed sometime in Spring 2013, most likely due to an event associated with strong alongshore sediment flux but minimal ocean-bay <span class="hlt">pressure</span> <span class="hlt">gradients</span>. Then, in July 2014, Hurricane Arthur briefly opened the breach again from the bay side, in a similar fashion to Irene. In summary, opening and closure of breaches are shown to follow a dynamic and episodic balance between along-channel <span class="hlt">pressure</span> <span class="hlt">gradient</span> driven flows and alongshore sediment fluxes.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li class="active"><span>6</span></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_6 --> <div id="page_7" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="121"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=38315&Lab=ORD&keyword=Sound+AND+reflection+AND+Wall&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50','EPA-EIMS'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=38315&Lab=ORD&keyword=Sound+AND+reflection+AND+Wall&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50"><span><span class="hlt">ACOUSTIC</span> LOCATION OF LEAKS IN <span class="hlt">PRESSURIZED</span> UNDERGROUND PETROLEUM PIPELINES</span></a></p> <p><a target="_blank" href="http://oaspub.epa.gov/eims/query.page">EPA Science Inventory</a></p> <p></p> <p></p> <p>Experiments were conducted at the UST Test Apparatus Pipeline in which three <span class="hlt">acoustic</span> sensors separated by a maximum distance of 38 m (125-ft) were used to monitor signals produced by 3.0-, 1.5-, and 1.0-gal/h leaks in the wall of a 2-in.-diameter <span class="hlt">pressurized</span> petroleum pipeline. ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940009275','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940009275"><span>Study of bubble behavior in weightlessness (effects of thermal <span class="hlt">gradient</span> and <span class="hlt">acoustic</span> stationary wave) (M-16)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Azuma, H.</p> <p>1993-01-01</p> <p>The aim of this experiment is to understand how bubbles behave in a thermal <span class="hlt">gradient</span> and <span class="hlt">acoustic</span> stationary wave under microgravity. In microgravity, bubble or bubbles in a liquid will not rise upward as they do on Earth but will rest where they are formed because there exists no gravity-induced buoyancy. We are interested in how bubbles move and in the mechanisms which support the movement. We will try two ways to make bubbles migrate. The first experiment concerns behavior of bubbles in a thermal <span class="hlt">gradient</span>. It is well known than an effect of surface tension which is masked by gravity on the ground becomes dominant in microgravity. The surface tension on the side of the bubble at a lower temperature is stronger than at a higher temperature. The bubble migrates toward the higher temperature side due to the surface tension difference. The migration speed depends on the so-called Marangoni number, which is a function of the temperature difference, the bubble diameter, liquid viscosity, and thermal diffusivity. At present, some experimental data about migration speeds in liquids with very small Marangoni numbers were obtained in space experiments, but cases of large Marangoni number are rarely obtained. In our experiment a couple of bubbles are to be injected into a cell filled with silicon oil, and the temperature <span class="hlt">gradient</span> is to be made gradually in the cell by a heater and a cooler. We will be able to determine migration speeds in a very wide range of Marangoni numbers, as well as study interactions between the bubbles. We will observe bubble movements affected by hydrodynamical and thermal interactions, the two kinds of interactions which occur simultaneously. These observation data will be useful for analyzing the interactions as well as understanding the behavior of particles or drops in materials processing. The second experiment concerns bubble movement in an <span class="hlt">acoustic</span> stationary wave. It is known that a bubble in a stationary wave moves toward the node or the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20060050051','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20060050051"><span><span class="hlt">Acoustic</span> Seal</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Steinetz, Bruce M. (Inventor)</p> <p>2006-01-01</p> <p>The invention relates to a sealing device having an <span class="hlt">acoustic</span> resonator. The <span class="hlt">acoustic</span> resonator is adapted to create <span class="hlt">acoustic</span> waveforms to generate a sealing <span class="hlt">pressure</span> barrier blocking fluid flow from a high <span class="hlt">pressure</span> area to a lower <span class="hlt">pressure</span> area. The sealing device permits noncontacting sealing operation. The sealing device may include a resonant-macrosonic-synthesis (RMS) resonator.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080008646','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080008646"><span><span class="hlt">Acoustic</span> seal</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Steinetz, Bruce M. (Inventor)</p> <p>2006-01-01</p> <p>The invention relates to a sealing device having an <span class="hlt">acoustic</span> resonator. The <span class="hlt">acoustic</span> resonator is adapted to create <span class="hlt">acoustic</span> waveforms to generate a sealing <span class="hlt">pressure</span> barrier blocking fluid flow from a high <span class="hlt">pressure</span> area to a lower <span class="hlt">pressure</span> area. The sealing device permits noncontacting sealing operation. The sealing device may include a resonant-macrosonic-synthesis (RMS) resonator.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21218872','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21218872"><span>The effects of external <span class="hlt">acoustic</span> <span class="hlt">pressure</span> fields on a free-running supercavitating projectile.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cameron, Peter J K; Rogers, Peter H; Doane, John W</p> <p>2010-12-01</p> <p>Proliferation of supercavitating torpedoes has motivated research on countermeasures against them as well as on the fluid phenomenon which makes them possible. The goal of this research was to investigate an envisaged countermeasure, an <span class="hlt">acoustic</span> field capable of slowing or diverting the weapon by disrupting the cavitation envelope. The research focused on the interactions between high <span class="hlt">pressure</span> amplitude sound waves and a supercavity produced by a small free-flying projectile. The flight dynamics and cavity geometry measurements were compared to control experiments and theoretical considerations were made for evaluating the effects. Corrugations on the cavity/water interface caused by the <span class="hlt">pressure</span> signal have been observed and characterized. Results also show that the accuracy of a supercavitating projectile can be adversely affected by the sound signal. This research concludes with results that indicate that it is <span class="hlt">acoustic</span> cavitation in the medium surrounding the supercavity, caused by the high <span class="hlt">pressure</span> amplitude sound, that is responsible for the reduced accuracy. A hypothesis has been presented addressing the means by which the <span class="hlt">acoustic</span> cavitation could cause this effect.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070022262','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070022262"><span>Aero-<span class="hlt">acoustics</span> of Drag Generating Swirling Exhaust Flows</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shah, P. N.; Mobed, D.; Spakovszky, Z. S.; Brooks, T. F.; Humphreys, W. M. Jr.</p> <p>2007-01-01</p> <p>Aircraft on approach in high-drag and high-lift configuration create unsteady flow structures which inherently generate noise. For devices such as flaps, spoilers and the undercarriage there is a strong correlation between overall noise and drag such that, in the quest for quieter aircraft, one challenge is to generate drag at low noise levels. This paper presents a rigorous aero-<span class="hlt">acoustic</span> assessment of a novel drag concept. The idea is that a swirling exhaust flow can yield a steady, and thus relatively quiet, streamwise vortex which is supported by a radial <span class="hlt">pressure</span> <span class="hlt">gradient</span> responsible for <span class="hlt">pressure</span> drag. Flows with swirl are naturally limited by instabilities such as vortex breakdown. The paper presents a first aero-<span class="hlt">acoustic</span> assessment of ram <span class="hlt">pressure</span> driven swirling exhaust flows and their associated instabilities. The technical approach combines an in-depth aerodynamic analysis, plausibility arguments to qualitatively describe the nature of <span class="hlt">acoustic</span> sources, and detailed, quantitative <span class="hlt">acoustic</span> measurements using a medium aperture directional microphone array in combination with a previously established Deconvolution Approach for Mapping of <span class="hlt">Acoustic</span> Sources (DAMAS). A model scale engine nacelle with stationary swirl vanes was designed and tested in the NASA Langley Quiet Flow Facility at a full-scale approach Mach number of 0.17. The analysis shows that the <span class="hlt">acoustic</span> signature is comprised of quadrupole-type turbulent mixing noise of the swirling core flow and scattering noise from vane boundary layers and turbulent eddies of the burst vortex structure near sharp edges. The exposed edges are the nacelle and pylon trailing edge and the centerbody supporting the vanes. For the highest stable swirl angle setting a nacelle area based drag coefficient of 0.8 was achieved with a full-scale Overall Sound <span class="hlt">Pressure</span> Level (OASPL) of about 40dBA at the ICAO approach certification point.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040110388','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040110388"><span>A Comparison of Measured and Predicted XV-15 Tiltrotor Surface <span class="hlt">Acoustic</span> <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>Lyle, Karen H.; Burley, Casey L.; Prichard, Devon S.</p> <p>1997-01-01</p> <p>Predicted XV-15 exterior surface <span class="hlt">acoustic</span> <span class="hlt">pressures</span> are compared with previously published experimental data. Surface <span class="hlt">acoustic</span> <span class="hlt">pressure</span> transducers were concentrated near the tip-path-plane of the rotor in airplane mode. The comparison emphasized cruise conditions which are of interest for tiltrotor interior noise - level flight for speeds ranging from 72 m/s to 113 m/s. The predictions were produced by components of the NASA Langley Tiltrotor Aeroacoustic Code (TRAC) system of computer codes. Comparisons between measurements and predictions were made in both the time and frequency domains, as well as overall sound <span class="hlt">pressure</span> levels. In general, the predictions replicated the measured data well. Discrepancies between measurements and predictions were noted. Some of the discrepancies were due to poor correlation of the measured data with the rotor tach signal. In other cases limitations of the predictive methodology have been indicated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29770413','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29770413"><span>Effect of <span class="hlt">pressure</span> <span class="hlt">gradient</span> and new phases for 1,3,5-trinitrohexahydro-s-triazine (RDX) under high <span class="hlt">pressures</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gao, Chan; Zhang, Xueyong; Zhang, Chuanchao; Sui, Zhilei; Hou, Meng; Dai, Rucheng; Wang, Zhongping; Zheng, Xianxu; Zhang, Zengming</p> <p>2018-05-17</p> <p>Herein, <span class="hlt">pressure</span>-induced phase transitions of RDX up to 50 GPa were systematically studied under different compression conditions. Precise phase transition points were obtained based on high-quality Raman spectra with small <span class="hlt">pressure</span> intervals. This favors the correctness of the theoretical formula for detonation and the design of a precision weapon. The experimental results indicated that α-RDX immediately transformed to γ-RDX at 3.5 GPa due to hydrostatic conditions and possible interaction between the penetrating helium and RDX, with helium gas as the <span class="hlt">pressure</span>-transmitting medium (PTM). Mapping of <span class="hlt">pressure</span> distribution in samples demonstrates that the <span class="hlt">pressure</span> <span class="hlt">gradient</span> is generated in the chamber and independent of other PTMs. The <span class="hlt">gradient</span> induced the first phase transition starts at 2.3 GPa and completed at 4.1 GPa. The larger <span class="hlt">pressure</span> <span class="hlt">gradient</span> promoted phase transition in advance under higher <span class="hlt">pressures</span>. Experimental results supported that there existed two conformers of AAI and AAE for γ-RDX, as proposed by another group. δ-RDX was considered to only occur in a hydrostatic environment around 18 GPa using helium as the PTM. This study confirms that δ-RDX is independent of PTM and exists under non-hydrostatic conditions. Evidence for a new phase (ζ) was found at about 28 GPa. These 4 phases have also been verified via XRD under high <span class="hlt">pressures</span>. In addition to this, another new phase (η) may exist above 38 GPa, and it needs to be further confirmed in the future. Moreover, all the phase transitions were reversible after the <span class="hlt">pressure</span> was released, and original α-RDX was always obtained at ambient <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790033600&hterms=acoustic+emission+testing&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dacoustic%2Bemission%2Btesting','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790033600&hterms=acoustic+emission+testing&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dacoustic%2Bemission%2Btesting"><span>Variabilities detected by <span class="hlt">acoustic</span> emission from filament-wound Aramid fiber/epoxy composite <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>Hamstad, M. A.</p> <p>1978-01-01</p> <p>Two hundred and fifty Aramid fiber/epoxy <span class="hlt">pressure</span> vessels were filament-wound over spherical aluminum mandrels under controlled conditions typical for advanced filament-winding. A random set of 30 vessels was proof-tested to 74% of the expected burst <span class="hlt">pressure</span>; <span class="hlt">acoustic</span> emission data were obtained during the proof test. A specially designed fixture was used to permit in situ calibration of the <span class="hlt">acoustic</span> emission system for each vessel by the fracture of a 4-mm length of pencil lead (0.3 mm in diameter) which was in contact with the vessel. <span class="hlt">Acoustic</span> emission signatures obtained during testing showed larger than expected variabilities in the mechanical damage done during the proof tests. To date, identification of the cause of these variabilities has not been determined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1018318','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1018318"><span>Systems and methods of monitoring <span class="hlt">acoustic</span> <span class="hlt">pressure</span> to detect a flame condition in a gas turbine</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Ziminsky, Willy Steve [Simpsonville, SC; Krull, Anthony Wayne [Anderson, SC; Healy, Timothy Andrew , Yilmaz, Ertan</p> <p>2011-05-17</p> <p>A method may detect a flashback condition in a fuel nozzle of a combustor. The method may include obtaining a current <span class="hlt">acoustic</span> <span class="hlt">pressure</span> signal from the combustor, analyzing the current <span class="hlt">acoustic</span> <span class="hlt">pressure</span> signal to determine current operating frequency information for the combustor, and indicating that the flashback condition exists based at least in part on the current operating frequency information.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29843947','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29843947"><span>Intracochlear <span class="hlt">pressure</span> measurements during <span class="hlt">acoustic</span> shock wave exposure.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Greene, Nathaniel T; Alhussaini, Mohamed A; Easter, James R; Argo, Theodore F; Walilko, Tim; Tollin, Daniel J</p> <p>2018-05-19</p> <p>Injuries to the peripheral auditory system are among the most common results of high intensity impulsive <span class="hlt">acoustic</span> exposure. Prior studies of high intensity sound transmission by the ossicular chain have relied upon measurements in animal models, measurements at more moderate sound levels (i.e. < 130 dB SPL), and/or measured responses to steady-state noise. Here, we directly measure intracochlear <span class="hlt">pressure</span> in human cadaveric temporal bones, with fiber optic <span class="hlt">pressure</span> sensors placed in scala vestibuli (SV) and tympani (ST), during exposure to shock waves with peak positive <span class="hlt">pressures</span> between ∼7 and 83 kPa. Eight full-cephalic human cadaver heads were exposed, face-on, to <span class="hlt">acoustic</span> shock waves in a 45 cm diameter shock tube. Specimens were exposed to impulses with nominal peak overpressures of 7, 28, 55, & 83 kPa (171, 183, 189, & 192 dB pSPL), measured in the free field adjacent to the forehead. Specimens were prepared bilaterally by mastoidectomy and extended facial recess to expose the ossicular chain. Ear canal (EAC), middle ear, and intracochlear sound <span class="hlt">pressure</span> levels were measured with fiber-optic <span class="hlt">pressure</span> sensors. Surface-mounted sensors measured SPL and skull strain near the opening of each EAC and at the forehead. Measurements on the forehead showed incident peak <span class="hlt">pressures</span> approximately twice that measured by adjacent free-field and EAC entrance sensors, as expected based on the sensor orientation (normal vs tangential to the shock wave propagation). At 7 kPa, EAC <span class="hlt">pressure</span> showed gain, calculated from the frequency spectra, consistent with the ear canal resonance, and gain in the intracochlear <span class="hlt">pressures</span> (normalized to the EAC <span class="hlt">pressure</span>) were consistent with (though somewhat lower than) previously reported middle ear transfer functions. Responses to higher intensity impulses tended to show lower intracochlear gain relative to EAC, suggesting sound transmission efficiency along the ossicular chain is reduced at high intensities. Tympanic membrane</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110022626','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110022626"><span>A Study of Standing <span class="hlt">Pressure</span> Waves Within Open and Closed <span class="hlt">Acoustic</span> Resonators</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Daniels, C.; Steinetz, B.; Finkbeiner, J.; Raman, G.; Li, X.</p> <p>2002-01-01</p> <p>The first section of the results presented herein was conducted on an axisymmetric resonator configured with open ventilation ports on either end of the resonator, but otherwise closed and free from obstruction. The remaining section presents the results of a similar resonator shape that was closed, but contained an axisymmetric blockage centrally located through the axis of the resonator. Ambient air was used as the working fluid. In each of the studies, the resonator was oscillated at the resonant frequency of the fluid contained within the cavity while the dynamic <span class="hlt">pressure</span>, static <span class="hlt">pressure</span>, and temperature of the fluid were recorded at both ends of the resonator. The baseline results showed a marked reduction in the amplitude of the dynamic <span class="hlt">pressure</span> waveforms over previous studies due to the use of air instead of refrigerant as the working fluid. A sharp reduction in the amplitude of the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> waves was expected and recorded when the configuration of the resonators was modified from closed to open. A change in the resonant frequency was recorded when blockages of differing geometries were used in the closed resonator, while <span class="hlt">acoustic</span> <span class="hlt">pressure</span> amplitudes varied little from baseline measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014RScI...85a5110S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014RScI...85a5110S"><span>Experimental and numerical characterization of the sound <span class="hlt">pressure</span> in standing wave <span class="hlt">acoustic</span> levitators</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stindt, A.; Andrade, M. A. B.; Albrecht, M.; Adamowski, J. C.; Panne, U.; Riedel, J.</p> <p>2014-01-01</p> <p>A novel method for predictions of the sound <span class="hlt">pressure</span> distribution in <span class="hlt">acoustic</span> levitators is based on a matrix representation of the Rayleigh integral. This method allows for a fast calculation of the <span class="hlt">acoustic</span> field within the resonator. To make sure that the underlying assumptions and simplifications are justified, this approach was tested by a direct comparison to experimental data. The experimental sound <span class="hlt">pressure</span> distributions were recorded by high spatially resolved frequency selective microphone scanning. To emphasize the general applicability of the two approaches, the comparative studies were conducted for four different resonator geometries. In all cases, the results show an excellent agreement, demonstrating the accuracy of the matrix method.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18794959','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18794959"><span>High-speed varifocal imaging with a tunable <span class="hlt">acoustic</span> <span class="hlt">gradient</span> index of refraction lens.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mermillod-Blondin, Alexandre; McLeod, Euan; Arnold, Craig B</p> <p>2008-09-15</p> <p>Fluidic lenses allow for varifocal optical elements, but current approaches are limited by the speed at which focal length can be changed. Here we demonstrate the use of a tunable <span class="hlt">acoustic</span> <span class="hlt">gradient</span> (TAG) index of refraction lens as a fast varifocal element. The optical power of the TAG lens varies continuously, allowing for rapid selection and modification of the effective focal length at time scales of 1 mus and shorter. The wavefront curvature applied to the incident light is experimentally quantified as a function of time, and single-frame imaging is demonstrated. Results indicate that the TAG lens can successfully be employed to perform high-rate imaging at multiple locations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhCS1001a2020S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS1001a2020S"><span>Characterisation of minimal-span plane Couette turbulence with <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sekimoto, Atsushi; Atkinson, Callum; Soria, Julio</p> <p>2018-04-01</p> <p>The turbulence statistics and dynamics in the spanwise-minimal plane Couette flow with <span class="hlt">pressure</span> <span class="hlt">gradients</span>, so-called, Couette-Poiseuille (C-P) flow, are investigated using direct numerical simulation. The large-scale motion is limited in the spanwise box dimension as in the minimal-span channel turbulence of Flores & Jiménez (Phys. Fluids, vol. 22, 2010, 071704). The effect of the top wall, where normal <span class="hlt">pressure</span>-driven Poiseuille flow is realised, is distinguished from the events on the bottom wall, where the <span class="hlt">pressure</span> <span class="hlt">gradient</span> results in mild or almost-zero wall-shear stress. A proper scaling of turbulence statistics in minimal-span C-P flows is presented. Also the ‘shear-less’ wall-bounded turbulence, where the Corrsin shear parameter is very weak compared to normal wall-bounded turbulence, represents local separation, which is also observed as spanwise streaks of reversed flow in full-size plane C-P turbulence. The local separation is a multi-scale event, which grows up to the order of the channel height even in the minimal-span geometry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22492624-sound-beam-manipulation-based-temperature-gradients','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22492624-sound-beam-manipulation-based-temperature-gradients"><span>Sound beam manipulation based on temperature <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Qian, Feng; School of Physics & Electronic Engineering, Changshu Institute of Technology, Changshu 215500; Quan, Li</p> <p></p> <p>Previous research with temperature <span class="hlt">gradients</span> has shown the feasibility of controlling airborne sound propagation. Here, we present a temperature <span class="hlt">gradients</span> based airborne sound manipulation schemes: a cylindrical <span class="hlt">acoustic</span> omnidirectional absorber (AOA). The proposed AOA has high absorption performance which can almost completely absorb the incident wave. Geometric <span class="hlt">acoustics</span> is used to obtain the refractive index distributions with different radii, which is then utilized to deduce the desired temperature <span class="hlt">gradients</span>. Since resonant units are not applied in the scheme, its working bandwidth is expected to be broadband. The scheme is temperature-tuned and easy to realize, which is of potential interest tomore » fields such as noise control or <span class="hlt">acoustic</span> cloaking.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AIPC.1770c0120F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AIPC.1770c0120F"><span>Numerical simulation of the processes in the normal incidence tube for high <span class="hlt">acoustic</span> <span class="hlt">pressure</span> levels</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fedotov, E. S.; Khramtsov, I. V.; Kustov, O. Yu.</p> <p>2016-10-01</p> <p>Numerical simulation of the <span class="hlt">acoustic</span> processes in an impedance tube at high levels of <span class="hlt">acoustic</span> <span class="hlt">pressure</span> is a way to solve a problem of noise suppressing by liners. These studies used liner specimen that is one cylindrical Helmholtz resonator. The evaluation of the real and imaginary parts of the liner <span class="hlt">acoustic</span> impedance and sound absorption coefficient was performed for sound <span class="hlt">pressure</span> levels of 130, 140 and 150 dB. The numerical simulation used experimental data having been obtained on the impedance tube with normal incidence waves. At the first stage of the numerical simulation it was used the linearized Navier-Stokes equations, which describe well the imaginary part of the liner impedance whatever the sound <span class="hlt">pressure</span> level. These equations were solved by finite element method in COMSOL Multiphysics program in axisymmetric formulation. At the second stage, the complete Navier-Stokes equations were solved by direct numerical simulation in ANSYS CFX in axisymmetric formulation. As the result, the acceptable agreement between numerical simulation and experiment was obtained.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDA24008M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDA24008M"><span>Evaluation of the accuracy of the Rotating Parallel Ray Omnidirectional Integration for instantaneous <span class="hlt">pressure</span> reconstruction from the measured <span class="hlt">pressure</span> <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moreto, Jose; Liu, Xiaofeng</p> <p>2017-11-01</p> <p>The accuracy of the Rotating Parallel Ray omnidirectional integration for <span class="hlt">pressure</span> reconstruction from the measured <span class="hlt">pressure</span> <span class="hlt">gradient</span> (Liu et al., AIAA paper 2016-1049) is evaluated against both the Circular Virtual Boundary omnidirectional integration (Liu and Katz, 2006 and 2013) and the conventional Poisson equation approach. Dirichlet condition at one boundary point and Neumann condition at all other boundary points are applied to the Poisson solver. A direct numerical simulation database of isotropic turbulence flow (JHTDB), with a homogeneously distributed random noise added to the entire field of DNS <span class="hlt">pressure</span> <span class="hlt">gradient</span>, is used to assess the performance of the methods. The random noise, generated by the Matlab function Rand, has a magnitude varying randomly within the range of +/-40% of the maximum DNS <span class="hlt">pressure</span> <span class="hlt">gradient</span>. To account for the effect of the noise distribution pattern on the reconstructed <span class="hlt">pressure</span> accuracy, a total of 1000 different noise distributions achieved by using different random number seeds are involved in the evaluation. Final results after averaging the 1000 realizations show that the error of the reconstructed <span class="hlt">pressure</span> normalized by the DNS <span class="hlt">pressure</span> variation range is 0.15 +/-0.07 for the Poisson equation approach, 0.028 +/-0.003 for the Circular Virtual Boundary method and 0.027 +/-0.003 for the Rotating Parallel Ray method, indicating the robustness of the Rotating Parallel Ray method in <span class="hlt">pressure</span> reconstruction. Sponsor: The San Diego State University UGP program.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002ASAJ..111..447F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002ASAJ..111..447F"><span>Low-frequency <span class="hlt">acoustic</span> <span class="hlt">pressure</span>, velocity, and intensity thresholds in a bottlenose dolphin (Tursiops truncatus) and white whale (Delphinapterus leucas)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Finneran, James J.; Carder, Donald A.; Ridgway, Sam H.</p> <p>2002-01-01</p> <p>The relative contributions of <span class="hlt">acoustic</span> <span class="hlt">pressure</span> and particle velocity to the low-frequency, underwater hearing abilities of the bottlenose dolphin (Tursiops truncatus) and white whale (Delphinapterus leucas) were investigated by measuring (masked) hearing thresholds while manipulating the relationship between the <span class="hlt">pressure</span> and velocity. This was accomplished by varying the distance within the near field of a single underwater sound projector (experiment I) and using two underwater sound projectors and an active sound control system (experiment II). The results of experiment I showed no significant change in <span class="hlt">pressure</span> thresholds as the distance between the subject and the sound source was changed. In contrast, velocity thresholds tended to increase and intensity thresholds tended to decrease as the source distance decreased. These data suggest that <span class="hlt">acoustic</span> <span class="hlt">pressure</span> is a better indicator of threshold, compared to particle velocity or mean active intensity, in the subjects tested. Interpretation of the results of experiment II (the active sound control system) was difficult because of complex <span class="hlt">acoustic</span> conditions and the unknown effects of the subject on the generated <span class="hlt">acoustic</span> field; however, these data also tend to support the results of experiment I and suggest that odontocete thresholds should be reported in units of <span class="hlt">acoustic</span> <span class="hlt">pressure</span>, rather than intensity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1433222','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1433222"><span>Effect of Valsalva's manoeuvre and hyoscinbutylbromide on the <span class="hlt">pressure</span> <span class="hlt">gradient</span> across the wall of oesophageal varices.</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Hosking, S W; Robinson, P; Johnson, A G</p> <p>1987-01-01</p> <p>To assess whether Valsalva's manoeuvre might cause variceal bleeding, 22 patients with oesophageal varices were studied. In 12 patients who received no previous treatment to their varices the median <span class="hlt">pressure</span> <span class="hlt">gradient</span> across the varix wall at rest was 19 (6-36) mmHg, and in 10 patients whose varices were thrombosed at their distal end the median <span class="hlt">pressure</span> <span class="hlt">gradient</span> in the proximal patent varix was 8 (1-6) mmHg. In untreated patients groups, the <span class="hlt">pressure</span> <span class="hlt">gradient</span> rose by 6-12 mmHg during Valsalva's manoeuvre in four patients, fell by 4-11 mmHg in five patients and was virtually unchanged in the remainder. These changes seem unlikely to cause variceal bleeding. Patients who repeated Valsalva's manoeuvre showed similar changes on each occasion. Six patients in the untreated group also received hyoscinbutylbromide 20 mg iv. No change was seen in the <span class="hlt">pressure</span> <span class="hlt">gradient</span> in five patients, suggesting that it is of little value in preventing variceal bleeding. PMID:3500098</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_7 --> <div id="page_8" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="141"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930070363&hterms=sensors+pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dsensors%2Bpressure','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930070363&hterms=sensors+pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dsensors%2Bpressure"><span>An oxygen <span class="hlt">pressure</span> sensor using surface <span class="hlt">acoustic</span> wave devices</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Leighty, Bradley D.; Upchurch, Billy T.; Oglesby, Donald M.</p> <p>1993-01-01</p> <p>Surface <span class="hlt">acoustic</span> wave (SAW) piezoelectric devices are finding widespread applications in many arenas, particularly in the area of chemical sensing. We have developed an oxygen <span class="hlt">pressure</span> sensor based on coating a SAW device with an oxygen binding agent which can be tailored to provide variable sensitivity. The coating is prepared by dissolving an oxygen binding agent in a toluene solution of a copolymer which is then sprayed onto the surface of the SAW device. Experimental data shows the feasibility of tailoring sensors to measure the partial <span class="hlt">pressure</span> of oxygen from 2.6 to 67 KPa (20 to 500 torr). Potential applications of this technology are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890005997','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890005997"><span>The influence of free-stream turbulence on turbulent boundary layers with mild adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hoffmann, Jon A.</p> <p>1988-01-01</p> <p>The influence of near isotropic free-stream turbulence on the shape factors and skin friction coefficients of turbulent bounday layers is presented for the cases of zero and mild adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span>. With free-stream turbulence, improved fluid mixing occurs in boundary layers with adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> relative to the zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> condition, with the same free-stream turbulence intensity and length scale. Stronger boundary layers with lower shape factors occur as a result of a lower ratio of the integral scale of turbulence to the boundary layer thickness, and to vortex stretching of the turbulent eddies in the free stream, both of which act to improve the transmission of momentum from the free stream to the boundary layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890012674','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890012674"><span>The influence of free-stream turbulence on turbulent boundary layers with mild adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hoffmann, J. A.; Kassir, S. M.; Larwood, S. M.</p> <p>1989-01-01</p> <p>The influence of near isotropic free-stream turbulence on the shape factors and skin friction coefficients of turbulent boundary layers is presented for the cases of zero and mild adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span>. With free-stream turbulence, improved fluid mixing occurs in boundary layers with adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> relative to the zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> condition, with the same free-stream turbulence intensity and length scale. Stronger boundary layers with lower shape factors occur as a result of a lower ratio of the integral scale of turbulence to the boundary layer thickness, and to vortex stretching of the turbulent eddies in the free-stream, both of which act to improve the transmission of momentum from the free-stream to the boundary layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26774257','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26774257"><span>Severity assessment of intracranial large artery stenosis by <span class="hlt">pressure</span> <span class="hlt">gradient</span> measurements: A feasibility study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Han, Yun-Fei; Liu, Wen-Hua; Chen, Xiang-Liang; Xiong, Yun-Yun; Yin, Qin-; Xu, Ge-Lin; Zhu, Wu-Sheng; Zhang, Ren-Liang; Ma, Min-Min; Li, Min-; Dai, Qi-Liang; Sun, Wen-; Liu, De-Zhi; Duan, Li-Hui; Liu, Xin-Feng</p> <p>2016-08-01</p> <p>Fractional flow reserve (FFR)-guided revascularization strategy is popular in coronary intervention. However, the feasibility of assessing stenotic severity in intracranial large arteries using <span class="hlt">pressure</span> <span class="hlt">gradient</span> measurements still remains unclear. Between March 2013 and May 2014, 12 consecutive patients with intracranial large artery stenosis (including intracranial internal carotid artery, middle cerebral M1 segment, intracranial vertebral artery, and basilar artery) were enrolled in this study. The trans-stenotic <span class="hlt">pressure</span> <span class="hlt">gradient</span> was measured before and/or after percutaneous transluminal angioplasty and stenting (PTAS), and was then compared with percent diameter stenosis. A Pd /Pa cut-off of ≤0.70 was used to guide stenting of hemodynamically significant stenoses. The device-related and procedure-related serious adverse events and recurrent cerebral ischemic events were recorded. The target vessel could be reached in all cases. No technical complications occurred due to the specific study protocol. Excellent <span class="hlt">pressure</span> signals were obtained in all patients. For seven patients who performed PTAS, the mean pre-procedural <span class="hlt">pressure</span> <span class="hlt">gradient</span> decreased from 59.0 ± 17.2 to 13.3 ± 13.6 mm Hg after the procedure (P < 0.01). Only one patient who refused stenting experienced a TIA event in the ipsilateral MCA territory. No recurrent ischemic event was observed in other patients. Mean trans-stenotic <span class="hlt">pressure</span> <span class="hlt">gradients</span> can be safely and easily measured with a 0.014-inch fluid-filled guide wire in intracranial large arteries. © 2016 Wiley Periodicals, Inc. © 2016 Wiley Periodicals, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130013453','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130013453"><span>Evaluation of <span class="hlt">Acoustic</span> Emission SHM of PRSEUS Composite <span class="hlt">Pressure</span> Cube Tests</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Horne, Michael R.; Madaras, Eric I.</p> <p>2013-01-01</p> <p>A series of tests of the Pultruded Rod Stitched Efficient Unitized Structure (PRSEUS) <span class="hlt">pressure</span> cube were conducted during third quarter 2011 at NASA Langley Research Center (LaRC) in the Combined Loads Test facility (COLTS). This is a report of the analysis of the <span class="hlt">Acoustic</span> Emission (AE) data collected during those tests. The AE signals of the later tests are consistent with the final failure progression through two of the <span class="hlt">pressure</span> cube panels. Calibration tests and damage precursor AE indications, from preliminary checkout <span class="hlt">pressurizations</span>, indicated areas of concern that eventually failed. Hence those tests have potential for vehicle health monitoring.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JAP...120a4902W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JAP...120a4902W"><span>Broadband unidirectional <span class="hlt">acoustic</span> cloak based on phase <span class="hlt">gradient</span> metasurfaces with two flat <span class="hlt">acoustic</span> lenses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Xiao-Peng; Wan, Le-Le; Chen, Tian-Ning; Song, Ai-Ling; Wang, Fang</p> <p>2016-07-01</p> <p>Narrow bandwidth and bulky configuration are the main obstacles for the realization and application of invisible cloaks. In this paper, we present an effective method to achieve broadband and thin <span class="hlt">acoustic</span> cloak by using an <span class="hlt">acoustic</span> metasurface (AMS). In order to realize this cloak, we use slitted unit cells to design the AMS due to the advantage of less energy loss, broad operation bandwidth, and subwavelength thickness. According to the hyperboloidal phase profile along the AMS, the incident plane waves can be focused at a designed focal spot by the flat lens. Furthermore, broadband <span class="hlt">acoustic</span> cloak is obtained by combining two identical flat lenses. The incident plane waves are focused at the center point in between of the two lenses by passing through one lens, and then recovered by passing through the other one. However, they cannot reach the cloaked regions in between of the two lenses. The simulation results can verify the non-detectability effect of the <span class="hlt">acoustic</span> cloak. Our study results provide an available and simple approach to experimentally achieve the <span class="hlt">acoustic</span> cloak, which can be used in <span class="hlt">acoustic</span> non-detectability for large objects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930004490','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930004490"><span>The trade-off characteristics of <span class="hlt">acoustic</span> and <span class="hlt">pressure</span> sensors for the NASP</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Winkler, Martin; Bush, Chuck</p> <p>1992-01-01</p> <p>Results of a trade study for the development of <span class="hlt">pressure</span> and <span class="hlt">acoustic</span> sensors for use on the National Aerospace Plane (NASP) are summarized. <span class="hlt">Pressure</span> sensors are needed to operate to 100 psia; <span class="hlt">acoustic</span> sensors are needed that can give meaningful information about a 200 dB sound <span class="hlt">pressure</span> level (SPL) environment. Both sensors will have to operate from a high temperature of 2000 F down to absolute zero. The main conclusions of the study are the following: (1) Diaphragm materials limit minimum size and maximum frequency response attainable. (2) No transduction is available to meet all the NASP requirements with existing technology. (3) Capacitive sensors are large relative to the requirement, have limited resolution and frequency response due to noise, and cable length is limited to approximately 20 feet. (4) Eddy current sensors are large relative to the requirement and have limited cable lengths. (5) Fiber optic sensors provide the possibility for a small sensor, even though present developments do not exhibit that characteristic. The need to use sapphire at high temperature complicates the design. Present high temperature research sensors suffer from poor resolution. A significant development effort will be required to realize the potential of fiber optics. (6) Short-term development seems to favor eddy current techniques with the penalty of larger size and reduced dynamic range for <span class="hlt">acoustic</span> sensors. (7) Long-term development may favor fiber optics with the penalties of cost, schedule, and uncertainty.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28339204','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28339204"><span>Liquid Marble Coalescence and Triggered Microreaction Driven by <span class="hlt">Acoustic</span> Levitation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Zhen; Zang, Duyang; Zhao, Liang; Qu, Mengfei; Li, Xu; Li, Xiaoguang; Li, Lixin; Geng, Xingguo</p> <p>2017-06-27</p> <p>Liquid marbles show promising potential for application in the microreactor field. Control of the coalescence between two or among multiple liquid marbles is critical; however, the successful merging of two isolated marbles is difficult because of their mechanically robust particle shells. In this work, the coalescence of multiple liquid marbles was achieved via <span class="hlt">acoustic</span> levitation. The dynamic behaviors of the liquid marbles were monitored by a high-speed camera. Driven by the sound field, the liquid marbles moved toward each other, collided, and eventually coalesced into a larger single marble. The underlying mechanisms of this process were probed via sound field simulation and <span class="hlt">acoustic</span> radiation <span class="hlt">pressure</span> calculation. The results indicated that the <span class="hlt">pressure</span> <span class="hlt">gradient</span> on the liquid marble surface favors the formation of a liquid bridge between the liquid marbles, resulting in their coalescence. A preliminary indicator reaction was induced by the coalescence of dual liquid marbles, which suggests that expected chemical reactions can be successfully triggered with multiple reagents contained in isolated liquid marbles via <span class="hlt">acoustic</span> levitation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23363099','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23363099"><span>Panel <span class="hlt">acoustic</span> contribution analysis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wu, Sean F; Natarajan, Logesh Kumar</p> <p>2013-02-01</p> <p>Formulations are derived to analyze the relative panel <span class="hlt">acoustic</span> contributions of a vibrating structure. The essence of this analysis is to correlate the <span class="hlt">acoustic</span> power flow from each panel to the radiated <span class="hlt">acoustic</span> <span class="hlt">pressure</span> at any field point. The <span class="hlt">acoustic</span> power is obtained by integrating the normal component of the surface <span class="hlt">acoustic</span> intensity, which is the product of the surface <span class="hlt">acoustic</span> <span class="hlt">pressure</span> and normal surface velocity reconstructed by using the Helmholtz equation least squares based nearfield <span class="hlt">acoustical</span> holography, over each panel. The significance of this methodology is that it enables one to analyze and rank relative <span class="hlt">acoustic</span> contributions of individual panels of a complex vibrating structure to <span class="hlt">acoustic</span> radiation anywhere in the field based on a single set of the <span class="hlt">acoustic</span> <span class="hlt">pressures</span> measured in the near field. Moreover, this approach is valid for both interior and exterior regions. Examples of using this method to analyze and rank the relative <span class="hlt">acoustic</span> contributions of a scaled vehicle cabin are demonstrated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28029367','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28029367"><span>On the feasibility to conduct <span class="hlt">gradient</span> liquid chromatography separations in narrow-bore columns at <span class="hlt">pressures</span> up to 2000bar.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>De Pauw, Ruben; Swier, Tim; Degreef, Bart; Desmet, Gert; Broeckhoven, Ken</p> <p>2016-11-18</p> <p>The limits in operating <span class="hlt">pressures</span> are extended for narrow-bore columns in <span class="hlt">gradient</span> elution up to 2000bar. As the required pumps for these <span class="hlt">pressures</span> are incompatible with common chromatographic solvents and are not suitable to apply a mobile phase composition <span class="hlt">gradient</span>, a mobile phase delivery and injection system is described and experimentally validated which allows to use any possible chromatographic solvent in isocratic and <span class="hlt">gradient</span> elution. The mobile phase delivery and injection system also allows to perform multiple separations without the need to depressurize the column. This system consists out of 5 dual on/off valves and two large volume loops in which the <span class="hlt">gradient</span> and equilibration volume of initial mobile phase are loaded by a commercial liquid chromatography pump. The loops are then flushed toward the column at extreme <span class="hlt">pressures</span>. The mobile phase delivery and injection system is first evaluated in isocratic elution and shows a comparable performance to a state-of-the-art commercial flow-through-needle injector but with twice the <span class="hlt">pressure</span> rating. Distortion of the loaded <span class="hlt">gradient</span> by dispersion in the <span class="hlt">gradient</span> storage loop is studied. The effect of the most important parameters (such as flow rate, <span class="hlt">pressure</span> and <span class="hlt">gradient</span> steepness) is experimentally investigated. Different <span class="hlt">gradient</span> steepnesses and volumes can be applied at different flow rates and operating <span class="hlt">pressures</span> with a good repeatability. Due to the isobaric operation of the pumps, the <span class="hlt">gradient</span> is monitored in real-time by a mass flow meter installed at the detector outlet. The chromatograms are then converted from time to volume-base. A separation of a 19-compound sample is performed on a 300×2.1mm column at 1000bar and on a 600×2.1mm column at 2000bar. The peak capacity was found to increase from 141 to 199 and thus scales with L as is predicted by theory. This allows to conclude that the inlet <span class="hlt">pressure</span> for narrow-bore columns in <span class="hlt">gradient</span> elution can be increased up to 2000bar without fundamental</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980008514','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980008514"><span>Neural Network Burst <span class="hlt">Pressure</span> Prediction in Graphite/Epoxy <span class="hlt">Pressure</span> Vessels from <span class="hlt">Acoustic</span> Emission Amplitude Data</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hill, Eric v. K.; Walker, James L., II; Rowell, Ginger H.</p> <p>1995-01-01</p> <p><span class="hlt">Acoustic</span> emission (AE) data were taken during hydroproof for three sets of ASTM standard 5.75 inch diameter filament wound graphite/epoxy bottles. All three sets of bottles had the same design and were wound from the same graphite fiber; the only difference was in the epoxies used. Two of the epoxies had similar mechanical properties, and because the <span class="hlt">acoustic</span> properties of materials are a function of their stiffnesses, it was thought that the AE data from the two sets might also be similar; however, this was not the case. Therefore, the three resin types were categorized using dummy variables, which allowed the prediction of burst <span class="hlt">pressures</span> all three sets of bottles using a single neural network. Three bottles from each set were used to train the network. The resin category, the AE amplitude distribution data taken up to 25 % of the expected burst <span class="hlt">pressure</span>, and the actual burst <span class="hlt">pressures</span> were used as inputs. Architecturally, the network consisted of a forty-three neuron input layer (a single categorical variable defining the resin type plus forty-two continuous variables for the AE amplitude frequencies), a fifteen neuron hidden layer for mapping, and a single output neuron for burst <span class="hlt">pressure</span> prediction. The network trained on all three bottle sets was able to predict burst <span class="hlt">pressures</span> in the remaining bottles with a worst case error of + 6.59%, slightly greater than the desired goal of + 5%. This larger than desired error was due to poor resolution in the amplitude data for the third bottle set. When the third set of bottles was eliminated from consideration, only four hidden layer neurons were necessary to generate a worst case prediction error of - 3.43%, well within the desired goal.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5479527','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5479527"><span>Hemodynamic and metabolic characteristics associated with development of a right ventricular outflow tract <span class="hlt">pressure</span> <span class="hlt">gradient</span> during upright exercise</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>van Riel, Annelieke C. M. J.; Systrom, David M.; Oliveira, Rudolf K. F.; Landzberg, Michael J.; Mulder, Barbara J. M.; Bouma, Berto J.; Maron, Bradley A.; Shah, Amil M.; Waxman, Aaron B.</p> <p>2017-01-01</p> <p>Background We recently reported a novel observation that many patients with equal resting supine right ventricular(RV) and pulmonary artery(PA) systolic <span class="hlt">pressures</span> develop an RV outflow tract(RVOT) <span class="hlt">pressure</span> <span class="hlt">gradient</span> during upright exercise. The current work details the characteristics of patients who develop such an RVOT <span class="hlt">gradient</span>. Methods We studied 294 patients (59.7±15.5 years-old, 49% male) referred for clinical invasive cardiopulmonary exercise testing, who did not have a resting RVOT <span class="hlt">pressure</span> <span class="hlt">gradient</span> defined by the simultaneously measured peak-to-peak difference between RV and PA systolic <span class="hlt">pressures</span>. Results The magnitude of RVOT <span class="hlt">gradient</span> did not correspond to clinical or hemodynamic findings suggestive of right heart failure; rather, higher <span class="hlt">gradients</span> were associated with favorable exercise findings. The presence of a high peak RVOT <span class="hlt">gradient</span> (90th percentile, ≥33mmHg) was associated with male sex (70 vs. 46%, p = 0.01), younger age (43.6±17.7 vs. 61.8±13.9 years, p<0.001), lower peak right atrial <span class="hlt">pressure</span> (5 [3–7] vs. 8 [4–12]mmHg, p<0.001), higher peak heart rate (159±19 vs. 124±26 beats per minute, p<0.001), and higher peak cardiac index (8.3±2.3 vs. 5.7±1.9 L/min/m2, p<0.001). These associations persisted when treating peak RVOT as a continuous variable and after age and sex adjustment. At peak exercise, patients with a high exercise RVOT <span class="hlt">gradient</span> had both higher RV systolic <span class="hlt">pressure</span> (78±11 vs. 66±17 mmHg, p<0.001) and lower PA systolic <span class="hlt">pressure</span> (34±8 vs. 50±19 mmHg, p<0.001). Conclusions Development of a systolic RV-PA <span class="hlt">pressure</span> <span class="hlt">gradient</span> during upright exercise is not associated with an adverse hemodynamic exercise response and may represent a normal physiologic finding in aerobically fit young people. PMID:28636647</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20220368','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20220368"><span><span class="hlt">Acoustic</span> <span class="hlt">pressure</span> waves induced in human heads by RF pulses from high-field MRI scanners.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lin, James C; Wang, Zhangwei</p> <p>2010-04-01</p> <p>The current evolution toward greater image resolution from magnetic resonance image (MRI) scanners has prompted the exploration of higher strength magnetic fields and use of higher levels of radio frequencies (RFs). Auditory perception of RF pulses by humans has been reported during MRI with head coils. It has shown that the mechanism of interaction for the auditory effect is caused by an RF pulse-induced thermoelastic <span class="hlt">pressure</span> wave inside the head. We report a computational study of the intensity and frequency of thermoelastic <span class="hlt">pressure</span> waves generated by RF pulses in the human head inside high-field MRI and clinical scanners. The U.S. Food and Drug Administration (U.S. FDA) guides limit the local specific absorption rate (SAR) in the body-including the head-to 8 W kg(-1). We present results as functions of SAR and show that for a given SAR the peak <span class="hlt">acoustic</span> <span class="hlt">pressures</span> generated in the anatomic head model were essentially the same at 64, 300, and 400 MHz (1.5, 7.0, and 9.4 T). <span class="hlt">Pressures</span> generated in the anatomic head are comparable to the threshold <span class="hlt">pressure</span> of 20 mPa for sound perception by humans at the cochlea for 4 W kg(-1). Moreover, results indicate that the peak <span class="hlt">acoustic</span> <span class="hlt">pressure</span> in the brain is only 2 to 3 times the auditory threshold at the U.S. FDA guideline of 8 W kg(-1). Even at a high SAR of 20 W kg(-1), where the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> in the brain could be more than 7 times the auditory threshold, the sound <span class="hlt">pressure</span> levels would not be more than 17 db above threshold of perception at the cochlea.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29753461','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29753461"><span>Hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> after portal vein embolization: An accurate predictor of future liver remnant hypertrophy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mohkam, Kayvan; Rode, Agnès; Darnis, Benjamin; Manichon, Anne-Frédérique; Boussel, Loïc; Ducerf, Christian; Merle, Philippe; Lesurtel, Mickaël; Mabrut, Jean-Yves</p> <p>2018-05-09</p> <p>The impact of portal hemodynamic variations after portal vein embolization on liver regeneration remains unknown. We studied the correlation between the parameters of hepatic venous <span class="hlt">pressure</span> measured before and after portal vein embolization and future hypertrophy of the liver remnant after portal vein embolization. Between 2014 and 2017, we reviewed patients who were eligible for major hepatectomy and who had portal vein embolization. Patients had undergone simultaneous measurement of portal venous <span class="hlt">pressure</span> and hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> before and after portal vein embolization by direct puncture of portal vein and inferior vena cava. We assessed these parameters to predict future liver remnant hypertrophy. Twenty-six patients were included. After portal vein embolization, median portal venous <span class="hlt">pressure</span> (range) increased from 15 (9-24) to 19 (10-27) mm Hg and hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> increased from 5 (0-12) to 8 (0-14) mm Hg. Median future liver remnant volume (range) was 513 (299-933) mL before portal vein embolization versus 724 (499-1279) mL 3 weeks after portal vein embolization, representing a 35% (7.4-83.6) median hypertrophy. Post-portal vein embolization hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> was the most accurate parameter to predict failure of future liver remnant to reach a 30% hypertrophy (c-statistic: 0.882 [95% CI: 0.727-1.000], P < 0.001). A cut-off value of post-portal vein embolization hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> of 8 mm Hg showed a sensitivity of 91% (95% CI: 57%-99%), specificity of 80% (95% CI: 52%-96%), positive predictive value of 77% (95% CI: 46%-95%) and negative predictive value of 92.3% (95% CI: 64.0%-99.8%). On multivariate analysis, post-portal vein embolization hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> and previous chemotherapy were identified as predictors of impaired future liver remnant hypertrophy. Post-portal vein embolization hepatic venous <span class="hlt">pressure</span> <span class="hlt">gradient</span> is a simple and reproducible tool which accurately predicts future</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12398441','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12398441"><span>Coupled dynamics of translation and collapse of <span class="hlt">acoustically</span> driven microbubbles.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Reddy, Anil J; Szeri, Andrew J</p> <p>2002-10-01</p> <p><span class="hlt">Pressure</span> <span class="hlt">gradients</span> drive the motion of microbubbles relative to liquids in which they are suspended. Examples include the hydrostatic <span class="hlt">pressure</span> due to a gravitational field, and the <span class="hlt">pressure</span> <span class="hlt">gradients</span> in a sound field, useful for <span class="hlt">acoustic</span> levitation. In this paper, the equations describing the coupled dynamics of radial oscillation and translation of a microbubble are given. The formulation is based on a recently derived expression for the hydrodynamic force on a bubble of changing size in an incompressible liquid [J. Magnaudet and D. Legendre, Phys. Fluids 10, 550-556 (1998)]. The complex interaction between radial and translation dynamics is best understood by examination of the added momentum associated with the liquid motion caused by the moving bubble. Translation is maximized when the bubble collapses violently. The new theory for coupled collapse and translation dynamics is compared to past experiments and to previous theories for decoupled translation dynamics. Special attention is paid to bubbles of relevance in biomedical applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009EGUGA..1111202M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009EGUGA..1111202M"><span>PACT - a bottom <span class="hlt">pressure</span> based, compact deep-ocean tsunameter with <span class="hlt">acoustic</span> surface coupling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Macrander, A.; Gouretski, V.; Boebel, O.</p> <p>2009-04-01</p> <p>The German-Indonsian Tsunami Early Warning System (GITEWS) processes a multitude of information to comprehensively and accurately evaluate the possible risks inherent to seismic events around Indonesia. Within just a few minutes, measurements of the vibration and horizontal movements off the coastal regions of Indonesia provide a clear picture of the location and intensity of a seaquake. However, not every seaquake causes a tsunami, nor is every tsunami caused by a seaquake. To avoid nerve-wrecking and costly false alarms and to protect against tsunamis caused by landslides, the oceanic sea-level must be measured directly. This goal is pursued in the GITEWS work package "ocean instrumentation", aiming at a a highest reliability and redundancy by developing a set of independent instruments, which measure the sea-level both offshore in the deep ocean and at the coast on the islands off Indonesia. Deep ocean sea-level changes less than a centimetre can be detected by <span class="hlt">pressure</span> gauges deployed at the sea floor. Based on some of the concepts developed as part of the US DART system, a bottom <span class="hlt">pressure</span> based, <span class="hlt">acoustically</span> coupled tsunami detector (PACT) was developed under the auspices of the AWI in collaboration with two German SME and with support of University of Bremen and University of Rhode Island. The PACT system records ocean bottom <span class="hlt">pressure</span>, performs on-board tsunami detection and <span class="hlt">acoustically</span> relays the data to the surface buoy. However, employing computational powers and communication technologies of the new millennium, PACT integrates the entire sea-floor package (<span class="hlt">pressure</span> gauge, data logger and analyzer, <span class="hlt">acoustic</span> modem, <span class="hlt">acoustic</span> release and relocation aids) into a single unit, i.e. a standard benthos sphere. PACT thereby reduces costs, minimizes the deployment efforts, while maximizing reliability and maintenance intervals. Several PACT systems are scheduled for their first deployment off Indonesia during 2009. In this presentation, the technical specifications</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDM28006G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDM28006G"><span>DNS of a non-equilibrium adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> turbulent boundary layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gungor, Taygun R.; Gungor, Ayse G.; Maciel, Yvan; Simens, Mark P.</p> <p>2017-11-01</p> <p>A new direct numerical simulation (DNS) dataset of a non-equilibrium adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> (APG) turbulent boundary layer (TBL) that evolves from a zero-<span class="hlt">pressure-gradient</span> (ZPG) TBL to a TBL which is very close to separation at Reθ is around 8200 is presented. There are two simulations running together in the DNS computational setup. The APG TBL spans Reθ = 1476 - 8276 . Mean velocity results do not satisfy the log law as the defect in the velocity increases. The production and the Reynolds stress peak are observed around y /δ* = 1 after the flow is evolved up to a certain point. The new dataset is compared with other datasets in terms of mean values, Reynolds stresses and turbulent kinetic energy budgets and using this comparison scaling study is performed. Funded by in part by ITU-AYP and NSERC of Canada.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19780023928','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19780023928"><span>Correlation of combustor <span class="hlt">acoustic</span> power levels inferred from internal fluctuating <span class="hlt">pressure</span> measurements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vonglahn, U. H.</p> <p>1978-01-01</p> <p>Combustion chamber <span class="hlt">acoustic</span> power levels inferred from internal fluctuating <span class="hlt">pressure</span> measurements are correlated with operating conditions and chamber geometries over a wide range. The variables include considerations of chamber design (can, annular, and reverse-flow annular) and size, number of fuel nozzles, burner staging and fuel split, airflow and heat release rates, and chamber inlet <span class="hlt">pressure</span> and temperature levels. The correlated data include those obtained with combustion component development rigs as well as engines.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730024448','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730024448"><span>On the relationship between <span class="hlt">acoustic</span> energy density flux near the jet axis and far field <span class="hlt">acoustic</span> intensity</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Maestrello, L.</p> <p>1973-01-01</p> <p>By measurement and analysis, the relationship between the distribution of the outflow of <span class="hlt">acoustic</span> energy over the jet boundary and the far-field intensity is considered. The physical quantity used is the <span class="hlt">gradient</span> of the <span class="hlt">pressure</span> evaluated on a geometrical plane at the smallest possible radial distance from the jet axis, but outside the vortical region, in the area where the homogeneous wave equation is reasonably well satisfied. The numerical and experimental procedures involved have been checked out by using a known source. Results indicate that the <span class="hlt">acoustic</span> power output per unit length of the jet, in the region from which the sound emanates, peaks at approximately 9 diameters downstream. The <span class="hlt">acoustic</span> emission for a jet Strouhal number of about 0.3 exceeds the emission for all other Strouhal numbers nearly everywhere along the measurement plane. However, the far-field peak intensity distribution obtained from the contribution of each station was found to depend on the spatial extent of the region where sound emanates from the jet, which, in turn, depends more on the far-field angle than on the Strouhal number.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5137745','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5137745"><span>Evolution of directional hearing in moths via conversion of bat detection devices to asymmetric <span class="hlt">pressure</span> <span class="hlt">gradient</span> receivers</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Reid, Andrew; Marin-Cudraz, Thibaut</p> <p>2016-01-01</p> <p>Small animals typically localize sound sources by means of complex internal connections and baffles that effectively increase time or intensity differences between the two ears. However, some miniature <span class="hlt">acoustic</span> species achieve directional hearing without such devices, indicating that other mechanisms have evolved. Using 3D laser vibrometry to measure tympanum deflection, we show that female lesser waxmoths (Achroia grisella) can orient toward the 100-kHz male song, because each ear functions independently as an asymmetric <span class="hlt">pressure</span> <span class="hlt">gradient</span> receiver that responds sharply to high-frequency sound arriving from an azimuth angle 30° contralateral to the animal's midline. We found that females presented with a song stimulus while running on a locomotion compensation sphere follow a trajectory 20°–40° to the left or right of the stimulus heading but not directly toward it, movement consistent with the tympanum deflections and suggestive of a monaural mechanism of auditory tracking. Moreover, females losing their track typically regain it by auditory scanning—sudden, wide deviations in their heading—and females initially facing away from the stimulus quickly change their general heading toward it, orientation indicating superior ability to resolve the front–rear ambiguity in source location. X-ray computer-aided tomography (CT) scans of the moths did not reveal any internal coupling between the two ears, confirming that an <span class="hlt">acoustic</span> insect can localize a sound source based solely on the distinct features of each ear. PMID:27849607</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_8 --> <div id="page_9" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="161"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MS%26E..254p2004G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MS%26E..254p2004G"><span>The Effect of Fabric Position to the Distribution of <span class="hlt">Acoustic</span> <span class="hlt">Pressure</span> Field in Ultrasonic Bath</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gürses, B. O.; Özdemir, A. O.; Tonay, Ö.; Şener, M.; Perinçek, S.</p> <p>2017-10-01</p> <p>Nowadays, the use of ultrasonic energy in textile wet processes at industrial-scale is limited. It is largely due to the lack of understanding about design, operational and performance characteristics of the ultrasonic bath, suitable for textile treatments. In the context of this study, the effect of fabric position, as one of the design parameter, to the distribution of <span class="hlt">acoustic</span> <span class="hlt">pressure</span> field in ultrasonic bath was investigated. The ultrasonic bath in the size 20×30 cm2 with one transducer at frequency 40 kHz was used in experiments. The cotton fabric with 1 mm thickness was moved along vertical and horizontal directions of the ultrasonic bath. The <span class="hlt">acoustic</span> field and cavitation volume density in the bath is analyzed by COMSOL Multiphysic. The cavitation volume density is calculated by comparing the <span class="hlt">pressure</span> points in the bath with cavitation threshold <span class="hlt">pressure</span>. Consequently, it was found that the position of the textile material in the ultrasonic bath is one of the most important factors to achieve the uniform and maximum <span class="hlt">acoustic</span> cavitation field. So, it should be taken into consideration during the design of industrial-scale ultrasonic bath used in textile wet processes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012ApPhL.100q3701M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012ApPhL.100q3701M"><span>Precise and programmable manipulation of microbubbles by two-dimensional standing surface <span class="hlt">acoustic</span> waves</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Meng, Long; Cai, Feiyan; Chen, Juanjuan; Niu, Lili; Li, Yanming; Wu, Junru; Zheng, Hairong</p> <p>2012-04-01</p> <p>A microfluidic device is developed to transport microbubbles (MBs) along a desired trajectory in fluid by introducing the phase-shift to a planar standing surface <span class="hlt">acoustic</span> wave (SSAW). The radiation force of SSAW due to the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> <span class="hlt">gradient</span> modulated by a phase-shift can move MBs to anticipated potential wells in a programmable manner. The resolution of the transportation is approximately 2.2 µm and the estimated radiation force on the MBs is on the order of 10-9 N. This device can be used for manipulation of bioparticles, cell sorting, tissue engineering, and other biomedical applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1713547P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1713547P"><span>The Phase Rule in a System Subject to a <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Podladchikov, Yuri; Connolly, James; Powell, Roger; Aardvark, Alberto</p> <p>2015-04-01</p> <p>It can be shown by diligent application of Lagrange's method of undetermined multipliers that the phase rule in a system subject to a <span class="hlt">pressure</span> <span class="hlt">gradient</span> is: � + 赑 ≥ ρ. We explore the consequence of this important relationship for natural systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19750020309','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19750020309"><span><span class="hlt">Pressure</span> <span class="hlt">gradient</span> effects on heat transfer to reusable surface insulation tile-array gaps</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Throckmorton, D. A.</p> <p>1975-01-01</p> <p>An experimental investigation was performed to determine the effect of <span class="hlt">pressure</span> <span class="hlt">gradient</span> on the heat transfer within space shuttle reusable surface insulation (RSI) tile-array gaps under thick, turbulent boundary-layer conditions. Heat-transfer and <span class="hlt">pressure</span> measurements were obtained on a curved array of full-scale simulated RSI tiles in a tunnel-wall boundary layer at a nominal free-stream Mach number and free-stream Reynolds numbers. Transverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> of varying degree were induced over the model surface by rotating the curved array with respect to the flow. Definition of the tunnel-wall boundary-layer flow was obtained by measurement of boundary-layer pitot <span class="hlt">pressure</span> profiles, wall <span class="hlt">pressure</span>, and heat transfer. Flat-plate heat-transfer data were correlated and a method was derived for prediction of heat transfer to a smooth curved surface in the highly three-dimensional tunnel-wall boundary-layer flow. <span class="hlt">Pressure</span> on the floor of the RSI tile-array gap followed the trends of the external surface <span class="hlt">pressure</span>. Heat transfer to the surface immediately downstream of a transverse gap is higher than that for a smooth surface at the same location. Heating to the wall of a transverse gap, and immediately downstream of it, at its intersection with a longitudinal gap is significantly greater than that for the simple transverse gap.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19960048065','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19960048065"><span>A Neural Network/<span class="hlt">Acoustic</span> Emission Analysis of Impact Damaged Graphite/Epoxy <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>Walker, James L.; Hill, Erik v. K.; Workman, Gary L.; Russell, Samuel S.</p> <p>1995-01-01</p> <p><span class="hlt">Acoustic</span> emission (AE) signal analysis has been used to measure the effects of impact damage on burst <span class="hlt">pressure</span> in 5.75 inch diameter, inert propellant filled, filament wound <span class="hlt">pressure</span> vessels. The AE data were collected from fifteen graphite/epoxy <span class="hlt">pressure</span> vessels featuring five damage states and three resin systems. A burst <span class="hlt">pressure</span> prediction model was developed by correlating the AE amplitude (frequency) distribution, generated during the first <span class="hlt">pressure</span> ramp to 800 psig (approximately 25% of the average expected burst <span class="hlt">pressure</span> for an undamaged vessel) to known burst <span class="hlt">pressures</span> using a four layered back propagation neural network. The neural network, trained on three vessels from each resin system, was able to predict burst <span class="hlt">pressures</span> with a worst case error of 5.7% for the entire fifteen bottle set.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26627789','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26627789"><span>Reconstruction of an <span class="hlt">acoustic</span> <span class="hlt">pressure</span> field in a resonance tube by particle image velocimetry.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kuzuu, K; Hasegawa, S</p> <p>2015-11-01</p> <p>A technique for estimating an <span class="hlt">acoustic</span> field in a resonance tube is suggested. The estimation of an <span class="hlt">acoustic</span> field in a resonance tube is important for the development of the thermoacoustic engine, and can be conducted employing two sensors to measure <span class="hlt">pressure</span>. While this measurement technique is known as the two-sensor method, care needs to be taken with the location of <span class="hlt">pressure</span> sensors when conducting <span class="hlt">pressure</span> measurements. In the present study, particle image velocimetry (PIV) is employed instead of a <span class="hlt">pressure</span> measurement by a sensor, and two-dimensional velocity vector images are extracted as sequential data from only a one- time recording made by a video camera of PIV. The spatial velocity amplitude is obtained from those images, and a <span class="hlt">pressure</span> distribution is calculated from velocity amplitudes at two points by extending the equations derived for the two-sensor method. By means of this method, problems relating to the locations and calibrations of multiple <span class="hlt">pressure</span> sensors are avoided. Furthermore, to verify the accuracy of the present method, the experiments are conducted employing the conventional two-sensor method and laser Doppler velocimetry (LDV). Then, results by the proposed method are compared with those obtained with the two-sensor method and LDV.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930040417&hterms=curvature&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dcurvature','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930040417&hterms=curvature&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dcurvature"><span>Turbulent boundary layers subjected to multiple curvatures and <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bandyopadhyay, Promode R.; Ahmed, Anwar</p> <p>1993-01-01</p> <p>The effects of abruptly applied cycles of curvatures and <span class="hlt">pressure</span> <span class="hlt">gradients</span> on turbulent boundary layers are examined experimentally. Two two-dimensional curved test surfaces are considered: one has a sequence of concave and convex longitudinal surface curvatures and the other has a sequence of convex and concave curvatures. The choice of the curvature sequences were motivated by a desire to study the asymmetric response of turbulent boundary layers to convex and concave curvatures. The relaxation of a boundary layer from the effects of these two opposite sequences has been compared. The effect of the accompaying sequences of <span class="hlt">pressure</span> <span class="hlt">gradient</span> has also been examined but the effect of curvature dominates. The growth of internal layers at the curvature junctions have been studied. Measurements of the Gortler and corner vortex systems have been made. The boundary layer recovering from the sequence of concave to convex curvature has a sustained lower skin friction level than in that recovering from the sequence of convex to concave curvature. The amplification and suppression of turbulence due to the curvature sequences have also been studied.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940028441','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940028441"><span>Modification of the MML turbulence model for adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> flows. M.S. Thesis - Akron Univ., 1993</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Conley, Julianne M.</p> <p>1994-01-01</p> <p>Computational fluid dynamics is being used increasingly to predict flows for aerospace propulsion applications, yet there is still a need for an easy to use, computationally inexpensive turbulence model capable of accurately predicting a wide range of turbulent flows. The Baldwin-Lomax model is the most widely used algebraic model, even though it has known difficulties calculating flows with strong adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> and large regions of separation. The modified mixing length model (MML) was developed specifically to handle the separation which occurs on airfoils and has given significantly better results than the Baldwin-Lomax model. The success of these calculations warrants further evaluation and development of MML. The objective of this work was to evaluate the performance of MML for zero and adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> flows, and modify it as needed. The Proteus Navier-Stokes code was used for this study and all results were compared with experimental data and with calculations made using the Baldwin-Lomax algebraic model, which is currently available in Proteus. The MML model was first evaluated for zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> flow over a flat plate, then modified to produce the proper boundary layer growth. Additional modifications, based on experimental data for three adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> flows, were also implemented. The adapted model, called MMLPG (modified mixing length model for <span class="hlt">pressure</span> <span class="hlt">gradient</span> flows), was then evaluated for a typical propulsion flow problem, flow through a transonic diffuser. Three cases were examined: flow with no shock, a weak shock and a strong shock. The results of these calculations indicate that the objectives of this study have been met. Overall, MMLPG is capable of accurately predicting the adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> flows examined in this study, giving generally better agreement with experimental data than the Baldwin-Lomax model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/866488','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/866488"><span><span class="hlt">Acoustic</span> cooling engine</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Hofler, Thomas J.; Wheatley, John C.; Swift, Gregory W.; Migliori, Albert</p> <p>1988-01-01</p> <p>An <span class="hlt">acoustic</span> cooling engine with improved thermal performance and reduced internal losses comprises a compressible fluid contained in a resonant <span class="hlt">pressure</span> vessel. The fluid has a substantial thermal expansion coefficient and is capable of supporting an <span class="hlt">acoustic</span> standing wave. A thermodynamic element has first and second ends and is located in the resonant <span class="hlt">pressure</span> vessel in thermal communication with the fluid. The thermal response of the thermodynamic element to the <span class="hlt">acoustic</span> standing wave pumps heat from the second end to the first end. The thermodynamic element permits substantial flow of the fluid through the thermodynamic element. An <span class="hlt">acoustic</span> driver cyclically drives the fluid with an <span class="hlt">acoustic</span> standing wave. The driver is at a location of maximum <span class="hlt">acoustic</span> impedance in the resonant <span class="hlt">pressure</span> vessel and proximate the first end of the thermodynamic element. A hot heat exchanger is adjacent to and in thermal communication with the first end of the thermodynamic element. The hot heat exchanger conducts heat from the first end to portions of the resonant <span class="hlt">pressure</span> vessel proximate the hot heat exchanger. The hot heat exchanger permits substantial flow of the fluid through the hot heat exchanger. The resonant <span class="hlt">pressure</span> vessel can include a housing less than one quarter wavelength in length coupled to a reservoir. The housing can include a reduced diameter portion communicating with the reservoir. The frequency of the <span class="hlt">acoustic</span> driver can be continuously controlled so as to maintain resonance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009RScI...80g3902D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009RScI...80g3902D"><span>Liquid mercury sound velocity measurements under high <span class="hlt">pressure</span> and high temperature by picosecond <span class="hlt">acoustics</span> in a diamond anvils cell</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Decremps, F.; Belliard, L.; Couzinet, B.; Vincent, S.; Munsch, P.; Le Marchand, G.; Perrin, B.</p> <p>2009-07-01</p> <p>Recent improvements to measure ultrasonic sound velocities of liquids under extreme conditions are described. Principle and feasibility of picosecond <span class="hlt">acoustics</span> in liquids embedded in a diamond anvils cell are given. To illustrate the capability of these advances in the sound velocity measurement technique, original high <span class="hlt">pressure</span> and high temperature results on the sound velocity of liquid mercury up to 5 GPa and 575 K are given. This high <span class="hlt">pressure</span> technique will certainly be useful in several fundamental and applied problems in physics and many other fields such as geophysics, nonlinear <span class="hlt">acoustics</span>, underwater sound, petrology or physical <span class="hlt">acoustics</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25448425','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25448425"><span>Alignment of an <span class="hlt">acoustic</span> manipulation device with cepstral analysis of electronic impedance data.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hughes, D A; Qiu, Y; Démoré, C; Weijer, C J; Cochran, S</p> <p>2015-02-01</p> <p><span class="hlt">Acoustic</span> particle manipulation is an emerging technology that uses ultrasonic standing waves to position objects with <span class="hlt">pressure</span> <span class="hlt">gradients</span> and <span class="hlt">acoustic</span> radiation forces. To produce strong standing waves, the transducer and the reflector must be aligned properly such that they are parallel to each other. This can be a difficult process due to the need to visualise the ultrasound waves and as higher frequencies are introduced, this alignment requires higher accuracy. In this paper, we present a method for aligning <span class="hlt">acoustic</span> resonators with cepstral analysis. This is a simple signal processing technique that requires only the electrical impedance measurement data of the resonator, which is usually recorded during the fabrication process of the device. We first introduce the mathematical basis of cepstral analysis and then demonstrate and validate it using a computer simulation of an <span class="hlt">acoustic</span> resonator. Finally, the technique is demonstrated experimentally to create many parallel linear traps for 10 μm fluorescent beads inside an <span class="hlt">acoustic</span> resonator. Copyright © 2014 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27350150','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27350150"><span>Inhaled Beta Agonist Bronchodilator Does Not Affect Trans-diaphragmatic <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> but Decreases Lower Esophageal Sphincter Retention <span class="hlt">Pressure</span> in Patients with Chronic Obstructive Pulmonary Disease (COPD) and Gastroesophageal Reflux Disease (GERD).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Del Grande, Leonardo M; Herbella, Fernando A M; Bigatao, Amilcar M; Jardim, Jose R; Patti, Marco G</p> <p>2016-10-01</p> <p>Chronic obstructive pulmonary disease (COPD) patients have a high incidence of gastroesophageal reflux disease (GERD) whose pathophysiology seems to be linked to an increased trans-diaphragmatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> and not to a defective esophagogastric barrier. Inhaled beta agonist bronchodilators are a common therapy used by patients with COPD. This drug knowingly not only leads to a decrease in the lower esophageal sphincter (LES) resting <span class="hlt">pressure</span>, favoring GERD, but also may improve ventilatory parameters, therefore preventing GERD. This study aims to evaluate the effect of inhaled beta agonist bronchodilators on the trans-diaphragmatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> and the esophagogastric barrier. We studied 21 patients (mean age 67 years, 57 % males) with COPD and GERD. All patients underwent high-resolution manometry and esophageal pH monitoring. Abdominal and thoracic <span class="hlt">pressure</span>, trans-diaphragmatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> (abdominal-thoracic <span class="hlt">pressure</span>), and the LES retention <span class="hlt">pressure</span> (LES basal <span class="hlt">pressure</span>-transdiaphragmatic <span class="hlt">gradient</span>) were measured before and 5 min after inhaling beta agonist bronchodilators. The administration of inhaled beta agonist bronchodilators leads to the following: (a) a simultaneous increase in abdominal and thoracic <span class="hlt">pressure</span> not affecting the trans-diaphragmatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> and (b) a decrease in the LES resting <span class="hlt">pressure</span> with a reduction of the LES retention <span class="hlt">pressure</span>. In conclusion, inhaled beta agonist bronchodilators not only increase the thoracic <span class="hlt">pressure</span> but also lead to an increased abdominal <span class="hlt">pressure</span> favoring GERD by affecting the esophagogastric barrier.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040141463&hterms=left&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dleft','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040141463&hterms=left&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dleft"><span>Doppler echo evaluation of pulmonary venous-left atrial <span class="hlt">pressure</span> <span class="hlt">gradients</span>: human and numerical model studies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Firstenberg, M. S.; Greenberg, N. L.; Smedira, N. G.; Prior, D. L.; Scalia, G. M.; Thomas, J. D.; Garcia, M. J.</p> <p>2000-01-01</p> <p>The simplified Bernoulli equation relates fluid convective energy derived from flow velocities to a <span class="hlt">pressure</span> <span class="hlt">gradient</span> and is commonly used in clinical echocardiography to determine <span class="hlt">pressure</span> differences across stenotic orifices. Its application to pulmonary venous flow has not been described in humans. Twelve patients undergoing cardiac surgery had simultaneous high-fidelity pulmonary venous and left atrial <span class="hlt">pressure</span> measurements and pulmonary venous pulsed Doppler echocardiography performed. Convective <span class="hlt">gradients</span> for the systolic (S), diastolic (D), and atrial reversal (AR) phases of pulmonary venous flow were determined using the simplified Bernoulli equation and correlated with measured actual <span class="hlt">pressure</span> differences. A linear relationship was observed between the convective (y) and actual (x) <span class="hlt">pressure</span> differences for the S (y = 0.23x + 0.0074, r = 0.82) and D (y = 0.22x + 0.092, r = 0.81) waves, but not for the AR wave (y = 0. 030x + 0.13, r = 0.10). Numerical modeling resulted in similar slopes for the S (y = 0.200x - 0.127, r = 0.97), D (y = 0.247x - 0. 354, r = 0.99), and AR (y = 0.087x - 0.083, r = 0.96) waves. Consistent with numerical modeling, the convective term strongly correlates with but significantly underestimates actual <span class="hlt">gradient</span> because of large inertial forces.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/10924058','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/10924058"><span>Doppler echo evaluation of pulmonary venous-left atrial <span class="hlt">pressure</span> <span class="hlt">gradients</span>: human and numerical model studies.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Firstenberg, M S; Greenberg, N L; Smedira, N G; Prior, D L; Scalia, G M; Thomas, J D; Garcia, M J</p> <p>2000-08-01</p> <p>The simplified Bernoulli equation relates fluid convective energy derived from flow velocities to a <span class="hlt">pressure</span> <span class="hlt">gradient</span> and is commonly used in clinical echocardiography to determine <span class="hlt">pressure</span> differences across stenotic orifices. Its application to pulmonary venous flow has not been described in humans. Twelve patients undergoing cardiac surgery had simultaneous high-fidelity pulmonary venous and left atrial <span class="hlt">pressure</span> measurements and pulmonary venous pulsed Doppler echocardiography performed. Convective <span class="hlt">gradients</span> for the systolic (S), diastolic (D), and atrial reversal (AR) phases of pulmonary venous flow were determined using the simplified Bernoulli equation and correlated with measured actual <span class="hlt">pressure</span> differences. A linear relationship was observed between the convective (y) and actual (x) <span class="hlt">pressure</span> differences for the S (y = 0.23x + 0.0074, r = 0.82) and D (y = 0.22x + 0.092, r = 0.81) waves, but not for the AR wave (y = 0. 030x + 0.13, r = 0.10). Numerical modeling resulted in similar slopes for the S (y = 0.200x - 0.127, r = 0.97), D (y = 0.247x - 0. 354, r = 0.99), and AR (y = 0.087x - 0.083, r = 0.96) waves. Consistent with numerical modeling, the convective term strongly correlates with but significantly underestimates actual <span class="hlt">gradient</span> because of large inertial forces.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDL26012K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDL26012K"><span>Characterization of Rare Reverse Flow Events in Adverse <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> Turbulent Boundary Layers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kaehler, Christian J.; Bross, Matthew; Fuchs, Thomas</p> <p>2017-11-01</p> <p>Time-resolved tomographic flow fields measured in the viscous sublayer region of a turbulent boundary layer subjected to an adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> (APG) are examined with the aim to resolve and characterize reverse flow events at Reτ = 5000. The fields were measured using a novel high resolution tomographic particle tracking technique. It is shown that this technique is able to fully resolve mean and time dependent features of the complex three-dimensional flow with high accuracy down to very near-wall distances ( 10 μm). From time resolved Lagrangian particle trajectories, statistical information as well as instantaneous topological features of near-wall flow events are deduced. Similar to the zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> case (ZPG), it was found that individual events with reverse flow components still occur relatively rarely under the action of the <span class="hlt">pressure</span> <span class="hlt">gradient</span> investigated here. However, reverse flow events comprised of many individual events, are shown to appear in relatively organized groupings in both spanwise and streamise directions. Furthermore, instantaneous measurements of reverse flow events show that these events are associated with the motion of low-momentum streaks in the near-wall region. This work is supported by the Priority Programme SPP 1881 Turbulent Superstructures and the individual project Grant KA1808/8-2 of the Deutsche Forschungsgemeinschaft.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA185785','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA185785"><span>Research on <span class="hlt">Acoustical</span> Scattering, Diffraction Catastrophes, Optics of Bubbles, Photoacoustics, and <span class="hlt">Acoustical</span> Phase Conjugation.</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1987-09-15</p> <p>optical levitation of bubbles; D. <span class="hlt">Acoustical</span> and optical diffraction catastrophes (theory and optical simulation of transverse cusps, experiments with...35 C. Optical Levitation of Bubbles in Water by the Radiation <span class="hlt">Pressure</span> of a Laser Beam: An <span class="hlt">Acoustically</span> Quiet Levitator ...radiation <span class="hlt">pressure</span> of a laser beam: an <span class="hlt">acoustically</span> quiet levitator ," J. <span class="hlt">Acoust</span> . Soc. Am. (submitted July 1987). C. Books (and sections thereof) Published</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10164E..0QR','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10164E..0QR"><span><span class="hlt">Acoustic</span> design of boundary segments in aircraft fuselages using topology optimization and a specialized <span class="hlt">acoustic</span> <span class="hlt">pressure</span> function</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Radestock, Martin; Rose, Michael; Monner, Hans Peter</p> <p>2017-04-01</p> <p>In most aviation applications, a major cost benefit can be achieved by a reduction of the system weight. Often the <span class="hlt">acoustic</span> properties of the fuselage structure are not in the focus of the primary design process, too. A final correction of poor <span class="hlt">acoustic</span> properties is usually done using insulation mats in the chamber between the primary and secondary shell. It is plausible that a more sophisticated material distribution in that area can result in a substantially reduced weight. Topology optimization is a well-known approach to reduce material of compliant structures. In this paper an adaption of this method to <span class="hlt">acoustic</span> problems is investigated. The gap full of insulation mats is suitably parameterized to achieve different material distributions. To find advantageous configurations, the objective in the underlying topology optimization is chosen to obtain good <span class="hlt">acoustic</span> <span class="hlt">pressure</span> patterns in the aircraft cabin. An important task in the optimization is an adequate Finite Element model of the system. This can usually not be obtained from commercially available programs due to the lack of special sensitivity data with respect to the design parameters. Therefore an appropriate implementation of the algorithm has been done, exploiting the vector and matrix capabilities in the MATLABQ environment. Finally some new aspects of the Finite Element implementation will also be presented, since they are interesting on its own and can be generalized to efficiently solve other partial differential equations as well.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhCS.879a2009N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhCS.879a2009N"><span><span class="hlt">Acoustic</span> emission analysis of crack resistance and fracture behavior of 20GL steel having the <span class="hlt">gradient</span> microstructure and strength</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nikulin, S.; Nikitin, A.; Belov, V.; Rozhnov, A.; Turilina, V.; Anikeenko, V.; Khatkevich, V.</p> <p>2017-07-01</p> <p>The crack resistances as well as fracture behavior of 20GL steel quenched with a fast-moving water stream and having <span class="hlt">gradient</span> microstructure and strength are analyzed. Crack resistance tests with quenched and normalized flat rectangular specimens having different cut lengths loaded by three-point bending with <span class="hlt">acoustic</span> emission measurements have been performed. The critical J-integral has been used as the crack resistance parameter of the material. Quenching with a fast moving water stream leads to <span class="hlt">gradient</span> (along a specimen wall thickness) strengthening of steel due to highly refined <span class="hlt">gradient</span> microstructure formation of the troostomartensite type. Quenching with a fast-moving water stream increases crack resistance Jc , of 20GL steel by a factor of ∼ 1.5. The fracture accrues gradually with the load in the normalized specimens while the initiated crack is hindered in the variable ductility layer and further arrested in the more ductile core in the quenched specimens.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017OcMod.116....1E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017OcMod.116....1E"><span>High-order accurate finite-volume formulations for the <span class="hlt">pressure</span> <span class="hlt">gradient</span> force in layered ocean models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Engwirda, Darren; Kelley, Maxwell; Marshall, John</p> <p>2017-08-01</p> <p>Discretisation of the horizontal <span class="hlt">pressure</span> <span class="hlt">gradient</span> force in layered ocean models is a challenging task, with non-trivial interactions between the thermodynamics of the fluid and the geometry of the layers often leading to numerical difficulties. We present two new finite-volume schemes for the <span class="hlt">pressure</span> <span class="hlt">gradient</span> operator designed to address these issues. In each case, the horizontal acceleration is computed as an integration of the contact <span class="hlt">pressure</span> force that acts along the perimeter of an associated momentum control-volume. A pair of new schemes are developed by exploring different control-volume geometries. Non-linearities in the underlying equation-of-state definitions and thermodynamic profiles are treated using a high-order accurate numerical integration framework, designed to preserve hydrostatic balance in a non-linear manner. Numerical experiments show that the new methods achieve high levels of consistency, maintaining hydrostatic and thermobaric equilibrium in the presence of strongly-sloping layer geometries, non-linear equations-of-state and non-uniform vertical stratification profiles. These results suggest that the new <span class="hlt">pressure</span> <span class="hlt">gradient</span> formulations may be appropriate for general circulation models that employ hybrid vertical coordinates and/or terrain-following representations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JAP...123q4902G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JAP...123q4902G"><span>Reflected wave manipulation by inhomogeneous impedance via varying-depth <span class="hlt">acoustic</span> liners</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guo, Jingwen; Zhang, Xin; Fang, Yi; Fattah, Ryu</p> <p>2018-05-01</p> <p><span class="hlt">Acoustic</span> liners, consisting of a perforated panel affixed to a honeycomb core with a rigid back plate, are widely used for noise attenuation purpose. In this study, by exploiting inhomogeneous impedance properties, we report an experimental and numerical study on a liner-type <span class="hlt">acoustic</span> metasurface, which possesses the functionality of both reflected wave manipulation and sound energy attenuation simultaneously. To realize the inhomogeneous <span class="hlt">acoustic</span> impedance, an <span class="hlt">acoustic</span> metasurface constructed by varying-depth <span class="hlt">acoustic</span> liners is designed and fabricated. The reflected sound <span class="hlt">pressure</span> fields induced by the metasurface are obtained in both experiments and simulations. A complete characterization of this metasurface is performed, including the effects of depth <span class="hlt">gradient</span>, incident angle, and incident frequency. Anomalous reflection, apparent negative reflection, and conversion from an incident wave to a surface wave with strong energy dissipation are achieved by the structure. Moreover, our proposed structure can overcome the single frequency performance limitation that exists in conventional metasurfaces and performs well in a broadband frequency range. The proposed <span class="hlt">acoustic</span> metasurface offers flexibility in controlling the direction of sound wave propagation with energy dissipation property and holds promise for various applications of noise reduction.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_9 --> <div id="page_10" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="181"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ExFl...59...86R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ExFl...59...86R"><span>Unit Reynolds number, Mach number and <span class="hlt">pressure</span> <span class="hlt">gradient</span> effects on laminar-turbulent transition in two-dimensional boundary layers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Risius, Steffen; Costantini, Marco; Koch, Stefan; Hein, Stefan; Klein, Christian</p> <p>2018-05-01</p> <p>The influence of unit Reynolds number (Re_1=17.5× 106-80× 106 {m}^{-1}), Mach number (M= 0.35-0.77) and incompressible shape factor (H_{12} = 2.50-2.66) on laminar-turbulent boundary layer transition was systematically investigated in the Cryogenic Ludwieg-Tube Göttingen (DNW-KRG). For this investigation the existing two-dimensional wind tunnel model, PaLASTra, which offers a quasi-uniform streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span>, was modified to reduce the size of the flow separation region at its trailing edge. The streamwise temperature distribution and the location of laminar-turbulent transition were measured by means of temperature-sensitive paint (TSP) with a higher accuracy than attained in earlier measurements. It was found that for the modified PaLASTra model the transition Reynolds number (Re_{ {tr}}) exhibits a linear dependence on the <span class="hlt">pressure</span> <span class="hlt">gradient</span>, characterized by H_{12}. Due to this linear relation it was possible to quantify the so-called `unit Reynolds number effect', which is an increase of Re_{ {tr}} with Re_1. By a systematic variation of M, Re_1 and H_{12} in combination with a spectral analysis of freestream disturbances, a stabilizing effect of compressibility on boundary layer transition, as predicted by linear stability theory, was detected (`Mach number effect'). Furthermore, two expressions were derived which can be used to calculate the transition Reynolds number as a function of the amplitude of total <span class="hlt">pressure</span> fluctuations, Re_1 and H_{12}. To determine critical N-factors, the measured transition locations were correlated with amplification rates, calculated by incompressible and compressible linear stability theory. By taking into account the spectral level of total <span class="hlt">pressure</span> fluctuations at the frequency of the most amplified Tollmien-Schlichting wave at transition location, the scatter in the determined critical N-factors was reduced. Furthermore, the receptivity coefficients dependence on incidence angle of <span class="hlt">acoustic</span> waves was used to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27986288','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27986288"><span>A practical approach for predicting retention time shifts due to <span class="hlt">pressure</span> and temperature <span class="hlt">gradients</span> in ultra-high-<span class="hlt">pressure</span> liquid chromatography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Åsberg, Dennis; Chutkowski, Marcin; Leśko, Marek; Samuelsson, Jörgen; Kaczmarski, Krzysztof; Fornstedt, Torgny</p> <p>2017-01-06</p> <p>Large <span class="hlt">pressure</span> <span class="hlt">gradients</span> are generated in ultra-high-<span class="hlt">pressure</span> liquid chromatography (UHPLC) using sub-2μm particles causing significant temperature <span class="hlt">gradients</span> over the column due to viscous heating. These <span class="hlt">pressure</span> and temperature <span class="hlt">gradients</span> affect retention and ultimately result in important selectivity shifts. In this study, we developed an approach for predicting the retention time shifts due to these <span class="hlt">gradients</span>. The approach is presented as a step-by-step procedure and it is based on empirical linear relationships describing how retention varies as a function of temperature and <span class="hlt">pressure</span> and how the average column temperature increases with the flow rate. It requires only four experiments on standard equipment, is based on straightforward calculations, and is therefore easy to use in method development. The approach was rigorously validated against experimental data obtained with a quality control method for the active pharmaceutical ingredient omeprazole. The accuracy of retention time predictions was very good with relative errors always less than 1% and in many cases around 0.5% (n=32). Selectivity shifts observed between omeprazole and the related impurities when changing the flow rate could also be accurately predicted resulting in good estimates of the resolution between critical peak pairs. The approximations which the presented approach are based on were all justified. The retention factor as a function of <span class="hlt">pressure</span> and temperature was studied in an experimental design while the temperature distribution in the column was obtained by solving the fundamental heat and mass balance equations for the different experimental conditions. We strongly believe that this approach is sufficiently accurate and experimentally feasible for this separation to be a valuable tool when developing a UHPLC method. After further validation with other separation systems, it could become a useful approach in UHPLC method development, especially in the pharmaceutical industry where</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930092289','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930092289"><span>Similar solutions for the compressible laminar boundary layer with heat transfer and <span class="hlt">pressure</span> <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cohen, Clarence B; Reshotko, Eli</p> <p>1956-01-01</p> <p>Stewartson's transformation is applied to the laminar compressible boundary-layer equations and the requirement of similarity is introduced, resulting in a set of ordinary nonlinear differential equations previously quoted by Stewartson, but unsolved. The requirements of the system are Prandtl number of 1.0, linear viscosity-temperature relation across the boundary layer, an isothermal surface, and the particular distributions of free-stream velocity consistent with similar solutions. This system admits axial <span class="hlt">pressure</span> <span class="hlt">gradients</span> of arbitrary magnitude, heat flux normal to the surface, and arbitrary Mach numbers. The system of differential equations is transformed to integral system, with the velocity ratio as the independent variable. For this system, solutions are found by digital computation for <span class="hlt">pressure</span> <span class="hlt">gradients</span> varying from that causing separation to the infinitely favorable <span class="hlt">gradient</span> and for wall temperatures from absolute zero to twice the free-stream stagnation temperature. Some solutions for separated flows are also presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21663931','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21663931"><span>Application of SH surface <span class="hlt">acoustic</span> waves for measuring the viscosity of liquids in function of <span class="hlt">pressure</span> 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>Kiełczyński, P; Szalewski, M; Balcerzak, A; Rostocki, A J; Tefelski, D B</p> <p>2011-12-01</p> <p>Viscosity measurements were carried out on triolein at <span class="hlt">pressures</span> from atmospheric up to 650 MPa and in the temperature range from 10°C to 40°C using ultrasonic measuring setup. Bleustein-Gulyaev SH surface <span class="hlt">acoustic</span> waves waveguides were used as viscosity sensors. Additionally, <span class="hlt">pressure</span> changes occurring during phase transition have been measured over the same temperature range. Application of ultrasonic SH surface <span class="hlt">acoustic</span> waves in the liquid viscosity measurements at high <span class="hlt">pressure</span> has many advantages. It enables viscosity measurement during phase transitions and in the high-<span class="hlt">pressure</span> range where the classical viscosity measurement methods cannot operate. Measurements of phase transition kinetics and viscosity of liquids at high <span class="hlt">pressures</span> and various temperatures (isotherms) is a novelty. The knowledge of changes in viscosity in function of <span class="hlt">pressure</span> and temperature can help to obtain a deeper insight into thermodynamic properties of liquids. Copyright © 2011 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014APS..DFDL27002P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014APS..DFDL27002P"><span>New Models for Velocity/<span class="hlt">Pressure-Gradient</span> Correlations in Turbulent Boundary Layers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Poroseva, Svetlana; Murman, Scott</p> <p>2014-11-01</p> <p>To improve the performance of Reynolds-Averaged Navier-Stokes (RANS) turbulence models, one has to improve the accuracy of models for three physical processes: turbulent diffusion, interaction of turbulent <span class="hlt">pressure</span> and velocity fluctuation fields, and dissipative processes. The accuracy of modeling the turbulent diffusion depends on the order of a statistical closure chosen as a basis for a RANS model. When the Gram-Charlier series expansions for the velocity correlations are used to close the set of RANS equations, no assumption on Gaussian turbulence is invoked and no unknown model coefficients are introduced into the modeled equations. In such a way, this closure procedure reduces the modeling uncertainty of fourth-order RANS (FORANS) closures. Experimental and direct numerical simulation data confirmed the validity of using the Gram-Charlier series expansions in various flows including boundary layers. We will address modeling the velocity/<span class="hlt">pressure-gradient</span> correlations. New linear models will be introduced for the second- and higher-order correlations applicable to two-dimensional incompressible wall-bounded flows. Results of models' validation with DNS data in a channel flow and in a zero-<span class="hlt">pressure</span> <span class="hlt">gradient</span> boundary layer over a flat plate will be demonstrated. A part of the material is based upon work supported by NASA under award NNX12AJ61A.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/9277520','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/9277520"><span>Protein osmotic <span class="hlt">pressure</span> <span class="hlt">gradients</span> and microvascular reflection coefficients.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Drake, R E; Dhother, S; Teague, R A; Gabel, J C</p> <p>1997-08-01</p> <p>Microvascular membranes are heteroporous, so the mean osmotic reflection coefficient for a microvascular membrane (sigma d) is a function of the reflection coefficient for each pore. Investigators have derived equations for sigma d based on the assumption that the protein osmotic <span class="hlt">pressure</span> <span class="hlt">gradient</span> across the membrane (delta II) does not vary from pore to pore. However, for most microvascular membranes, delta II probably does vary from pore to pore. In this study, we derived a new equation for sigma d. According to our equation, pore-to-pore differences in delta II increase the effect of small pores and decrease the effect of large pores on the overall membrane osmotic reflection coefficient. Thus sigma d for a heteroporous membrane may be much higher than previously derived equations indicate. Furthermore, pore-to-pore delta II differences increase the effect of plasma protein osmotic <span class="hlt">pressure</span> to oppose microvascular fluid filtration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70028438','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70028438"><span>Role of transient water <span class="hlt">pressure</span> in quarrying: A subglacial experiment using <span class="hlt">acoustic</span> emissions</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Cohen, D.; Hooyer, T.S.; Iverson, N.R.; Thomason, J.F.; Jackson, M.</p> <p>2006-01-01</p> <p>Probably the most important mechanism of glacial erosion is quarrying: the growth and coalescence of cracks in subglacial bedrock and dislodgement of resultant rock fragments. Although evidence indicates that erosion rates depend on sliding speed, rates of crack growth in bedrock may be enhanced by changing stresses on the bed caused by fluctuating basal water <span class="hlt">pressure</span> in zones of ice-bed separation. To study quarrying in real time, a granite step, 12 cm high with a crack in its stoss surface, was installed at the bed of Engabreen, Norway. <span class="hlt">Acoustic</span> emission sensors monitored crack growth events in the step as ice slid over it. Vertical stresses, water <span class="hlt">pressure</span>, and cavity height in the lee of the step were also measured. Water was pumped to the lee of the step several times over 8 days. Pumping initially caused opening of a leeward cavity, which then closed after pumping was stopped and water <span class="hlt">pressure</span> decreased. During cavity closure, <span class="hlt">acoustic</span> emissions emanating mostly from the vicinity of the base of the crack in the step increased dramatically. With repeated pump tests this crack grew with time until the step's lee surface was quarried. Our experiments indicate that fluctuating water <span class="hlt">pressure</span> caused stress thresholds required for crack growth to be exceeded. Natural basal water <span class="hlt">pressure</span> fluctuations should also concentrate stresses on rock steps, increasing rates of crack growth. Stress changes on the bed due to water <span class="hlt">pressure</span> fluctuations will increase in magnitude and duration with cavity size, which may help explain the effect of sliding speed on erosion rates. Copyright 2006 by the American Geophysical Union.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApPhL.112q3503L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApPhL.112q3503L"><span>Controllable asymmetric transmission via gap-tunable <span class="hlt">acoustic</span> metasurface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Bingyi; Jiang, Yongyuan</p> <p>2018-04-01</p> <p>In this work, we utilize the <span class="hlt">acoustic</span> <span class="hlt">gradient</span> metasurface (AGM) of a bilayer configuration to realize the controllable asymmetric transmission. Relying on the adjustable gap between the two composing layers, the metasurface could switch from symmetric transmission to asymmetric transmission at a certain gap value. The underlying mechanism is attributed to the interference between the forward diffracted waves scattered by the surface bound waves at two air-AGM interfaces, which is apparently influenced by the interlayer distance. We further utilize the hybrid <span class="hlt">acoustic</span> elements to construct the desired <span class="hlt">gradient</span> metasurface with a tunable gap and validate the controllable asymmetric transmission with full-wave simulations. Our work provides the solution for actively controlling the transmission property of an <span class="hlt">acoustic</span> element, which shows potential application in <span class="hlt">acoustic</span> communication as a dynamic tunable <span class="hlt">acoustic</span> diode.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940009274','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940009274"><span>Drop dynamics in space and interference with <span class="hlt">acoustic</span> field (M-15)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yamanaka, Tatsuo</p> <p>1993-01-01</p> <p>The objective of the experiment is to study contactless positioning of liquid drops, excitation of capillary waves on the surface of <span class="hlt">acoustically</span> levitated liquid drops, and deformation of liquid drops by means of <span class="hlt">acoustic</span> radiation <span class="hlt">pressure</span>. Contactless positioning technologies are very important in space materials processing because the melt is processed without contacting the wall of a crucible which can easily contaminate the melt specifically for high melting temperatures and chemically reactive materials. Among the contactless positioning technologies, an <span class="hlt">acoustic</span> technology is especially important for materials unsusceptible to electromagnetic fields such as glasses and ceramics. The shape of a levitated liquid drop in the weightless condition is determined by its surface tension and the internal and external <span class="hlt">pressure</span> distribution. If the surface temperature is constant and there exist neither internal nor external <span class="hlt">pressure</span> perturbations, the levitated liquid drop forms a shape of perfect sphere. If temperature <span class="hlt">gradients</span> on the surface and internal or external <span class="hlt">pressure</span> perturbations exist, the liquid drop forms various modes of shapes with proper vibrations. A rotating liquid drop was specifically studied not only as a classical problem of theoretical mechanics to describe the shapes of the planets of the solar system, as well as their arrangement, but it is also more a contemporary problem of modern non-linear mechanics. In the experiment, we are expecting to observe various shapes of a liquid drop such as cocoon, tri-lobed, tetropod, multi-lobed, and doughnut.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3913518','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3913518"><span>Experimental Study on the Flow Regimes and <span class="hlt">Pressure</span> <span class="hlt">Gradients</span> of Air-Oil-Water Three-Phase Flow in Horizontal Pipes</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Al-Hadhrami, Luai M.; Shaahid, S. M.; Tunde, Lukman O.; Al-Sarkhi, A.</p> <p>2014-01-01</p> <p>An experimental investigation has been carried out to study the flow regimes and <span class="hlt">pressure</span> <span class="hlt">gradients</span> of air-oil-water three-phase flows in 2.25 ID horizontal pipe at different flow conditions. The effects of water cuts, liquid and gas velocities on flow patterns and <span class="hlt">pressure</span> <span class="hlt">gradients</span> have been studied. The experiments have been conducted at 20°C using low viscosity Safrasol D80 oil, tap water and air. Superficial water and oil velocities were varied from 0.3 m/s to 3 m/s and air velocity varied from 0.29 m/s to 52.5 m/s to cover wide range of flow patterns. The experiments were performed for 10% to 90% water cuts. The flow patterns were observed and recorded using high speed video camera while the <span class="hlt">pressure</span> drops were measured using <span class="hlt">pressure</span> transducers and U-tube manometers. The flow patterns show strong dependence on water fraction, gas velocities, and liquid velocities. The observed flow patterns are stratified (smooth and wavy), elongated bubble, slug, dispersed bubble, and annular flow patterns. The <span class="hlt">pressure</span> <span class="hlt">gradients</span> have been found to increase with the increase in gas flow rates. Also, for a given superficial gas velocity, the <span class="hlt">pressure</span> <span class="hlt">gradients</span> increased with the increase in the superficial liquid velocity. The <span class="hlt">pressure</span> <span class="hlt">gradient</span> first increases and then decreases with increasing water cut. In general, phase inversion was observed with increase in the water cut. The experimental results have been compared with the existing unified Model and a good agreement has been noticed. PMID:24523645</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24523645','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24523645"><span>Experimental study on the flow regimes and <span class="hlt">pressure</span> <span class="hlt">gradients</span> of air-oil-water three-phase flow in horizontal pipes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Al-Hadhrami, Luai M; Shaahid, S M; Tunde, Lukman O; Al-Sarkhi, A</p> <p>2014-01-01</p> <p>An experimental investigation has been carried out to study the flow regimes and <span class="hlt">pressure</span> <span class="hlt">gradients</span> of air-oil-water three-phase flows in 2.25 ID horizontal pipe at different flow conditions. The effects of water cuts, liquid and gas velocities on flow patterns and <span class="hlt">pressure</span> <span class="hlt">gradients</span> have been studied. The experiments have been conducted at 20 °C using low viscosity Safrasol D80 oil, tap water and air. Superficial water and oil velocities were varied from 0.3 m/s to 3 m/s and air velocity varied from 0.29 m/s to 52.5 m/s to cover wide range of flow patterns. The experiments were performed for 10% to 90% water cuts. The flow patterns were observed and recorded using high speed video camera while the <span class="hlt">pressure</span> drops were measured using <span class="hlt">pressure</span> transducers and U-tube manometers. The flow patterns show strong dependence on water fraction, gas velocities, and liquid velocities. The observed flow patterns are stratified (smooth and wavy), elongated bubble, slug, dispersed bubble, and annular flow patterns. The <span class="hlt">pressure</span> <span class="hlt">gradients</span> have been found to increase with the increase in gas flow rates. Also, for a given superficial gas velocity, the <span class="hlt">pressure</span> <span class="hlt">gradients</span> increased with the increase in the superficial liquid velocity. The <span class="hlt">pressure</span> <span class="hlt">gradient</span> first increases and then decreases with increasing water cut. In general, phase inversion was observed with increase in the water cut. The experimental results have been compared with the existing unified Model and a good agreement has been noticed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28380260','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28380260"><span>A numerical study of the <span class="hlt">acoustic</span> radiation due to eddy current-cryostat interactions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Yaohui; Liu, Feng; Zhou, Xiaorong; Li, Yu; Crozier, Stuart</p> <p>2017-06-01</p> <p>To investigate the <span class="hlt">acoustic</span> radiation due to eddy current-cryostat interactions and perform a qualitative analysis on noise reduction methods. In order to evaluate the sound <span class="hlt">pressure</span> level (SPL) of the eddy current induced warm bore wall vibration, a Finite Element (FE) model was created to simulate the noises from both the warm bore wall vibration and the <span class="hlt">gradient</span> coil assembly. For the SPL reduction of the warm bore wall vibration, we first improved the active shielding of the <span class="hlt">gradient</span> coil, thus reducing the eddy current on the warm bore wall. A damping treatment was then applied to the warm bore wall to control the <span class="hlt">acoustic</span> radiation. Initial simulations show that the SPL of the warm bore wall is higher than that of the <span class="hlt">gradient</span> assembly with typical design shielding ratios at many frequencies. Subsequent simulation results of eddy current control and damping treatment application show that the average SPL reduction of the warm bore wall can be as high as 9.6 dB, and even higher in some frequency bands. Combining eddy current control and suggested damping scheme, the noise level in a MRI system can be effectively reduced. © 2017 American Association of Physicists in Medicine.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JCrGr.487...65B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JCrGr.487...65B"><span><span class="hlt">Acoustic</span> vibration effects in classical nucleation theory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Baird, James K.; Su, C.-H.</p> <p>2018-04-01</p> <p><span class="hlt">Acoustic</span> vibration is often used to improve the yield of crystals and nanoparticles growing from solutions and melts. As there is still a debate on how <span class="hlt">acoustic</span> vibration actually works, we have examined the possibility that <span class="hlt">acoustic</span> <span class="hlt">pressure</span> can affect the rate of nucleation. Our method is based on an expansion of the free energy of the nucleus in powers of the <span class="hlt">acoustic</span> <span class="hlt">pressure</span>. With the assumption that the period of the sound wave is short as compared to the time scale for nucleation, we replace the powers of the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> by their time averages, retaining the average of the square of the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> as the leading term. By assuming a nucleus having spherical shape, we use the Young-Laplace equation to relate the <span class="hlt">pressure</span> inside the nucleus to the ambient <span class="hlt">pressure</span>. Without making further approximations not already standard in classical nucleation theory, we find that the proximate effect of <span class="hlt">acoustic</span> <span class="hlt">pressure</span> is to reduce both the size of the critical nucleus as well as the work required to form it from monomers. As the work serves as the activation energy, the ultimate effect of <span class="hlt">acoustic</span> <span class="hlt">pressure</span> is to increase the rate of nucleation. If we assume that the atomic structure of the nucleus is the same as that of an ordinary solid, however, we find the compressibility is too small for <span class="hlt">acoustic</span> vibration effects to be noticeable. If on the other hand, we assume that the structure is similar to that of a loosely bound colloidal particle, then the effects of <span class="hlt">acoustic</span> vibration become potentially observable.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27118817','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27118817"><span>Effects of Continuous Positive Airway <span class="hlt">Pressure</span> on Middle Ear <span class="hlt">Pressure</span> and <span class="hlt">Acoustic</span> Stapedial Reflex.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Jinrang; Li, Keliang</p> <p>2016-08-01</p> <p>This study investigated the effects of continuous positive airway <span class="hlt">pressure</span> (CPAP) on middle ear <span class="hlt">pressure</span> and <span class="hlt">acoustic</span> stapedial reflex and the correlation between CPAP and middle ear <span class="hlt">pressure</span>. Prospective cohort study. Tertiary hospitals. Fifty patients with obstructive sleep apnea-hypopnea syndrome were assigned to the study group, and 50 healthy volunteers were assigned to the control group. The subjects underwent standard tympanometry while wearing a CPAP device (ie, simulated CPAP treatment), which was set to 0, 5, 10, and 15 cm H2O, respectively. Tympanometry was performed before and after swallowing at each <span class="hlt">pressure</span> of CPAP treatment. The mean middle ear <span class="hlt">pressures</span> were 21.2, 22.6, 22.7, and 23.4 daPa (before swallowing) and 21.6, 42.6, 81.4, and 118.6 daPa (after swallowing) in the study group and 17.6, 18.7, 19.5, and 20.8 daPa (before swallowing) and 17.7, 44.2, 85.6, and 120.5 daPa (after swallowing) in the control group at the CPAPs of 0, 5, 10, and 15 cm H2O, respectively. While the CPAPs were at 0 and 15 cm H2O, the stapedial muscle reflex at 1.0 kHz did not have a significant difference between the 2 groups (χ(2) = 0.521, P = .470). The Pearson correlation coefficient of the CPAP <span class="hlt">pressure</span> and the middle ear <span class="hlt">pressure</span> after swallowing was 0.812 (P < .001). CPAP affected middle ear <span class="hlt">pressure</span> and was directly proportional to the <span class="hlt">pressure</span> of the CPAP. However, CPAP treatment had no significant effect on stapedial muscle reflex. © American Academy of Otolaryngology—Head and Neck Surgery Foundation 2016.</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> Dependence of Signal Amplitudes for Electrostriction Laser-Induced Thermal <span class="hlt">Acoustics</span></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 <span class="hlt">acoustics</span> (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 <span class="hlt">acoustic</span> grating) was averaged for each of 11 flow conditions and compared to the expected theoretical dependence 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('http://hdl.handle.net/2060/19810018494','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19810018494"><span>Radio jet refraction in galactic atmospheres with static <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Henriksen, R. N.; Vallee, J. P.; Bridle, A. H.</p> <p>1981-01-01</p> <p>A theory of double radio sources which have a 'Z' or 'S' morphology is proposed, based on the refraction of radio jets in the extended atmosphere of an elliptical galaxy. The model describes a collimated jet of supersonic material bending self-consistently under the influence of external static <span class="hlt">pressure</span> <span class="hlt">gradients</span>. Gravity and magnetic fields are neglected in the simplest case except insofar as they determine the static <span class="hlt">pressure</span> distribution. The calculation is a straightforward extension of a method used to calculate a ram-<span class="hlt">pressure</span> model for twin radio trails ('C' morphology). It may also be described as a continuous-jet version of a buoyancy model proposed in 1973. The model has the added virtue of invoking a galactic atmosphere similar to those already indicated by X-ray measurements of some other radio galaxies and by models for the collimation of other radio jets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890000421&hterms=Acoustic+levitation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DAcoustic%2Blevitation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890000421&hterms=Acoustic+levitation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DAcoustic%2Blevitation"><span>Determining Equilibrium Position For <span class="hlt">Acoustical</span> Levitation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Barmatz, M. B.; Aveni, G.; Putterman, S.; Rudnick, J.</p> <p>1989-01-01</p> <p>Equilibrium position and orientation of <span class="hlt">acoustically</span>-levitated weightless object determined by calibration technique on Earth. From calibration data, possible to calculate equilibrium position and orientation in presence of Earth gravitation. Sample not levitated <span class="hlt">acoustically</span> during calibration. Technique relies on Boltzmann-Ehrenfest adiabatic-invariance principle. One converts resonant-frequency-shift data into data on normalized <span class="hlt">acoustical</span> potential energy. Minimum of energy occurs at equilibrium point. From <span class="hlt">gradients</span> of <span class="hlt">acoustical</span> potential energy, one calculates <span class="hlt">acoustical</span> restoring force or torque on objects as function of deviation from equilibrium position or orientation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4873643','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4873643"><span>Iso-<span class="hlt">acoustic</span> focusing of cells for size-insensitive acousto-mechanical phenotyping</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Augustsson, Per; Karlsen, Jonas T.; Su, Hao-Wei; Bruus, Henrik; Voldman, Joel</p> <p>2016-01-01</p> <p>Mechanical phenotyping of single cells is an emerging tool for cell classification, enabling assessment of effective parameters relating to cells' interior molecular content and structure. Here, we present iso-<span class="hlt">acoustic</span> focusing, an equilibrium method to analyze the effective <span class="hlt">acoustic</span> impedance of single cells in continuous flow. While flowing through a microchannel, cells migrate sideways, influenced by an <span class="hlt">acoustic</span> field, into streams of increasing <span class="hlt">acoustic</span> impedance, until reaching their cell-type specific point of zero <span class="hlt">acoustic</span> contrast. We establish an experimental procedure and provide theoretical justifications and models for iso-<span class="hlt">acoustic</span> focusing. We describe a method for providing a suitable <span class="hlt">acoustic</span> contrast <span class="hlt">gradient</span> in a cell-friendly medium, and use <span class="hlt">acoustic</span> forces to maintain that <span class="hlt">gradient</span> in the presence of destabilizing forces. Applying this method we demonstrate iso-<span class="hlt">acoustic</span> focusing of cell lines and leukocytes, showing that <span class="hlt">acoustic</span> properties provide phenotypic information independent of size. PMID:27180912</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27180912','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27180912"><span>Iso-<span class="hlt">acoustic</span> focusing of cells for size-insensitive acousto-mechanical phenotyping.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Augustsson, Per; Karlsen, Jonas T; Su, Hao-Wei; Bruus, Henrik; Voldman, Joel</p> <p>2016-05-16</p> <p>Mechanical phenotyping of single cells is an emerging tool for cell classification, enabling assessment of effective parameters relating to cells' interior molecular content and structure. Here, we present iso-<span class="hlt">acoustic</span> focusing, an equilibrium method to analyze the effective <span class="hlt">acoustic</span> impedance of single cells in continuous flow. While flowing through a microchannel, cells migrate sideways, influenced by an <span class="hlt">acoustic</span> field, into streams of increasing <span class="hlt">acoustic</span> impedance, until reaching their cell-type specific point of zero <span class="hlt">acoustic</span> contrast. We establish an experimental procedure and provide theoretical justifications and models for iso-<span class="hlt">acoustic</span> focusing. We describe a method for providing a suitable <span class="hlt">acoustic</span> contrast <span class="hlt">gradient</span> in a cell-friendly medium, and use <span class="hlt">acoustic</span> forces to maintain that <span class="hlt">gradient</span> in the presence of destabilizing forces. Applying this method we demonstrate iso-<span class="hlt">acoustic</span> focusing of cell lines and leukocytes, showing that <span class="hlt">acoustic</span> properties provide phenotypic information independent of size.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26092411','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26092411"><span><span class="hlt">Acoustic</span>-noise-optimized diffusion-weighted imaging.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ott, Martin; Blaimer, Martin; Grodzki, David M; Breuer, Felix A; Roesch, Julie; Dörfler, Arnd; Heismann, Björn; Jakob, Peter M</p> <p>2015-12-01</p> <p>This work was aimed at reducing <span class="hlt">acoustic</span> noise in diffusion-weighted MR imaging (DWI) that might reach <span class="hlt">acoustic</span> noise levels of over 100 dB(A) in clinical practice. A diffusion-weighted readout-segmented echo-planar imaging (EPI) sequence was optimized for <span class="hlt">acoustic</span> noise by utilizing small readout segment widths to obtain low <span class="hlt">gradient</span> slew rates and amplitudes instead of faster k-space coverage. In addition, all other <span class="hlt">gradients</span> were optimized for low slew rates. Volunteer and patient imaging experiments were conducted to demonstrate the feasibility of the method. <span class="hlt">Acoustic</span> noise measurements were performed and analyzed for four different DWI measurement protocols at 1.5T and 3T. An <span class="hlt">acoustic</span> noise reduction of up to 20 dB(A) was achieved, which corresponds to a fourfold reduction in <span class="hlt">acoustic</span> perception. The image quality was preserved at the level of a standard single-shot (ss)-EPI sequence, with a 27-54% increase in scan time. The diffusion-weighted imaging technique proposed in this study allowed a substantial reduction in the level of <span class="hlt">acoustic</span> noise compared to standard single-shot diffusion-weighted EPI. This is expected to afford considerably more patient comfort, but a larger study would be necessary to fully characterize the subjective changes in patient experience.</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/24370000','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24370000"><span>Very high <span class="hlt">pressure</span> liquid chromatography using core-shell particles: quantitative analysis of fast <span class="hlt">gradient</span> separations without post-run times.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Stankovich, Joseph J; Gritti, Fabrice; Stevenson, Paul G; Beaver, Lois A; Guiochon, Georges</p> <p>2014-01-17</p> <p>Five methods for controlling the mobile phase flow rate for <span class="hlt">gradient</span> elution analyses using very high <span class="hlt">pressure</span> liquid chromatography (VHPLC) were tested to determine thermal stability of the column during rapid <span class="hlt">gradient</span> separations. To obtain rapid separations, instruments are operated at high flow rates and high inlet <span class="hlt">pressure</span> leading to uneven thermal effects across columns and additional time needed to restore thermal equilibrium between successive analyses. The purpose of this study is to investigate means to minimize thermal instability and obtain reliable results by measuring the reproducibility of the results of six replicate <span class="hlt">gradient</span> separations of a nine component RPLC standard mixture under various experimental conditions with no post-run times. <span class="hlt">Gradient</span> separations under different conditions were performed: constant flow rates, two sets of constant <span class="hlt">pressure</span> operation, programmed flow constant <span class="hlt">pressure</span> operation, and conditions which theoretically should yield a constant net heat loss at the column's wall. The results show that using constant flow rates, programmed flow constant <span class="hlt">pressures</span>, and constant heat loss at the column's wall all provide reproducible separations. However, performing separations using a high constant <span class="hlt">pressure</span> with programmed flow reduces the analysis time by 16% compared to constant flow rate methods. For the constant flow rate, programmed flow constant <span class="hlt">pressure</span>, and constant wall heat experiments no equilibration time (post-run time) was required to obtain highly reproducible data. Copyright © 2013 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/8149707','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/8149707"><span>Assessment of coronary artery stenosis <span class="hlt">pressure</span> <span class="hlt">gradient</span> by quantitative coronary arteriography in patients with coronary artery disease.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Atar, D; Ramanujam, P S; Saunamäki, K; Haunsø, S</p> <p>1994-01-01</p> <p>The aim of the study described here was to correlate coronary artery (CA) stenosis <span class="hlt">pressure</span> <span class="hlt">gradients</span> calculated by quantitative coronary arteriography (QCA) to invasively measured transstenotic <span class="hlt">pressure</span> drops in patients with anginal symptoms and with known or suspected coronary artery disease. Furthermore, the known mathematical models are improved by introducing (1) <span class="hlt">pressure</span> catheter-corrected minimal stenosis area, (2) modification of flow assumptions, and (3) stenosis exit angle. Included in the study were 45 patients with 61 stenoses. The visually estimated CA lesion severity in these non-complex stenoses was in the equivocal range of 40-70%. All measurements were performed after intracoronary administration of nifedipine and nitroglycerin. Stenosis dimensions were assessed from magnified cinefilms, using hand-held calipers. Highly significant overall correlation was found between measured and calculated <span class="hlt">pressure</span> <span class="hlt">gradients</span> with correction for the impact of the intracoronary catheter (P < 0.00001, r = 0.84). In particular, a substantial number of stenoses with haemodynamically-insignificant <span class="hlt">pressure</span> <span class="hlt">gradients</span> were identified by hydrodynamic calculations. In conclusion, the great majority of the coronary artery stenoses could be classified reliably by QCA as being haemodynamically insignificant or significant, respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20000059222','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20000059222"><span>Flow Duct Data for Validation of <span class="hlt">Acoustic</span> Liner Codes for Impedance Eduction</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ahuja, K. K.; Munro, Scott; Gaeta, R. J., Jr.</p> <p>2000-01-01</p> <p>The objective of the study reported here was to acquire <span class="hlt">acoustic</span> and flow data with hard and lined duct wall duct sections for validation of a liner prediction code being developed at NASA LaRC. Both the mean flowfield and <span class="hlt">acoustic</span> flowfields were determined in a cross-plane of the rectangular duct. A flow duct facility with <span class="hlt">acoustic</span> drivers connected to a rectangular (4.7 x 2.0 inch) source section and a linear <span class="hlt">acoustic</span> liner mounted downstream of the source section was used in this study. The liner section was designed to allow liner materials to be placed on all 4 walls of the duct. The test liner was of the locally-reacting type and was made from a ceramic material. The material, consisting of a tubular structure, was provided by NASA LaRC. The liner was approximately 8.89 cm (3.5 inches) thick. For the current study, only the two "short" sides of the duct were lined with liner material. The other two sides were hard walls. Two especially built instrumentation sections were attached on either sides of the liner section to allow <span class="hlt">acoustic</span> and flow measurements to be made upstream and downstream of the liner. The two instrumentation duct sections were built to allow measurement of <span class="hlt">acoustic</span> and flow properties at planes perpendicular to flow upstream and downstream of the liner section. The instrumentation section was also designed to provide a streamwise <span class="hlt">gradient</span> in <span class="hlt">acoustic</span> (complex) <span class="hlt">pressure</span> from which the <span class="hlt">acoustic</span> particle velocity, needed for the model validation, can be computed. Flow measurements included <span class="hlt">pressure</span>, temperature, and velocity profiles upstream of the liner section. The in-flow sound <span class="hlt">pressure</span> levels and phases were obtained with a microphone probe equipped with a nose cone in two cross planes upstream of the liner and two cross plane downstream of the liner. In addition to the <span class="hlt">acoustic</span> measurements at the cross planes. axial centerline <span class="hlt">acoustic</span> data was acquired using an axially traversing microphone probe which was traversed from a location</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26685055','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26685055"><span>Respiratory Muscle Strength, Sound <span class="hlt">Pressure</span> Level, and Vocal <span class="hlt">Acoustic</span> Parameters and Waist Circumference of Children With Different Nutritional Status.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pascotini, Fernanda dos Santos; Ribeiro, Vanessa Veis; Christmann, Mara Keli; Tomasi, Lidia Lis; Dellazzana, Amanda Alves; Haeffner, Leris Salete Bonfanti; Cielo, Carla Aparecida</p> <p>2016-01-01</p> <p>Relate respiratory muscle strength (RMS), sound <span class="hlt">pressure</span> (SP) level, and vocal <span class="hlt">acoustic</span> parameters to the abdominal circumference (AC) and nutritional status of children. This is a cross-sectional study. Eighty-two school children aged between 8 and 10 years, grouped by nutritional states (eutrophic, overweight, or obese) and AC percentile (≤25, 25-75, and ≥75), were included in the study. Evaluations of maximal inspiratory <span class="hlt">pressure</span> (IPmax) and maximal expiratory <span class="hlt">pressure</span> (EPmax) were conducted using the manometer and SP and <span class="hlt">acoustic</span> parameters through the Multi-Dimensional Voice Program Advanced (KayPENTAX, Montvale, New Jersey). There were significant differences (P < 0.05) in the EPmax of children with AC between the 25th and 75th percentiles (72.4) and those less than or equal to the 25th percentile (61.9) and in the SP of those greater than or equal to the 75th percentile (73.4) and less than or equal to the 25th percentile (66.6). The IPmax, EPmax, SP levels, and <span class="hlt">acoustic</span> variables were not different in relation to the nutritional states of the children. There was a strong and positive correlation between the coefficient of amplitude perturbations (shimmer), the harmonics-to-noise ratio and the variation of the fundamental frequency, respectively, 0.79 and 0.71. RMS and <span class="hlt">acoustic</span> voice characteristics in children do not appear to be influenced by nutritional states, and respiratory <span class="hlt">pressure</span> does not interfere with <span class="hlt">acoustic</span> voice characteristics. However, localized fat, represented by the AC, alters the EPmax and the SP, each of which increases as the AC increases. Copyright © 2016 The Voice Foundation. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25172821','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25172821"><span>Incorporating high-<span class="hlt">pressure</span> electroosmotic pump and a nano-flow <span class="hlt">gradient</span> generator into a miniaturized liquid chromatographic system for peptide analysis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Apeng; Lynch, Kyle B; Wang, Xiaochun; Lu, Joann J; Gu, Congying; Liu, Shaorong</p> <p>2014-09-24</p> <p>We integrate a high-<span class="hlt">pressure</span> electroosmotic pump (EOP), a nanoflow <span class="hlt">gradient</span> generator, and a capillary column into a miniaturized liquid chromatographic system that can be directly coupled with a mass spectrometer for proteomic analysis. We have recently developed a low-cost high-<span class="hlt">pressure</span> EOP capable of generating <span class="hlt">pressure</span> of tens of thousands psi, ideal for uses in miniaturized HPLC. The pump worked smoothly when it was used for isocratic elutions. When it was used for <span class="hlt">gradient</span> elutions, generating reproducible <span class="hlt">gradient</span> profiles was challenging; because the pump rate fluctuated when the pump was used to pump high-content organic solvents. This presents an issue for separating proteins/peptides since high-content organic solvents are often utilized. In this work, we solve this problem by incorporating our high-<span class="hlt">pressure</span> EOP with a nano-flow <span class="hlt">gradient</span> generator so that the EOP needs only to pump an aqueous solution. With this combination, we develop a capillary-based nano-HPLC system capable of performing nano-flow <span class="hlt">gradient</span> elution; the pump rate is stable, and the <span class="hlt">gradient</span> profiles are reproducible and can be conveniently tuned. To demonstrate its utility, we couple it with either a UV absorbance detector or a mass spectrometer for peptide separations. Copyright © 2014. Published by Elsevier B.V.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29761086','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29761086"><span>Aortic-Brachial Pulse Wave Velocity Ratio: A Measure of Arterial Stiffness <span class="hlt">Gradient</span> Not Affected by Mean Arterial <span class="hlt">Pressure</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fortier, Catherine; Desjardins, Marie-Pier; Agharazii, Mohsen</p> <p>2018-03-01</p> <p>Aortic stiffness, measured by carotid-femoral pulse wave velocity (cf-PWV), is used for the prediction of cardiovascular risk. This mini-review describes the nonlinear relationship between cf-PWV and operational blood <span class="hlt">pressure</span>, presents the proposed methods to adjust for this relationship, and discusses a potential place for aortic-brachial PWV ratio (a measure of arterial stiffness <span class="hlt">gradient</span>) as a blood <span class="hlt">pressure</span>-independent measure of vascular aging. PWV is inherently dependent on the operational blood <span class="hlt">pressure</span>. In cross-sectional studies, PWV adjustment for mean arterial <span class="hlt">pressure</span> (MAP) is preferred, but still remains a nonoptimal approach, as the relationship between PWV and blood <span class="hlt">pressure</span> is nonlinear and varies considerably among individuals due to heterogeneity in genetic background, vascular tone, and vascular remodeling. Extrapolations from the blood <span class="hlt">pressure</span>-independent stiffness parameter β (β 0 ) have led to the creation of stiffness index β, which can be used for local stiffness. A similar approach has been used for cardio-ankle PWV to generate a blood <span class="hlt">pressure</span>-independent cardio-ankle vascular index (CAVI). It was recently demonstrated that stiffness index β and CAVI remain slightly blood <span class="hlt">pressure</span>-dependent, and a more appropriate formula has been proposed to make the proper adjustments. On the other hand, the negative impact of aortic stiffness on clinical outcomes is thought to be mediated through attenuation or reversal of the arterial stiffness <span class="hlt">gradient</span>, which can also be influenced by a reduction in peripheral medium-sized muscular arteries in conditions that predispose to accelerate vascular aging. Arterial stiffness <span class="hlt">gradient</span>, assessed by aortic-brachial PWV ratio, is emerging to be at least as good as cf-PWV for risk prediction, but has the advantage of not being affected by operating MAP. The negative impacts of aortic stiffness on clinical outcomes are proposed to be mediated through attenuation or reversal of arterial stiffness <span class="hlt">gradient</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28753738','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28753738"><span>Modification of splenic stiffness on <span class="hlt">acoustic</span> radiation force impulse parallels the variation of portal <span class="hlt">pressure</span> induced by transjugular intrahepatic portosystemic shunt.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>De Santis, Adriano; Nardelli, Silvia; Bassanelli, Chiara; Lupo, Marinella; Iegri, Claudia; Di Ciesco, Carmela Anna; Forlino, Mariana; Farcomeni, Alessio; Riggio, Oliviero</p> <p>2018-03-01</p> <p>Spleen and liver stiffness (LS) measured by <span class="hlt">acoustic</span> radiation force impulse (ARFI) imaging has been shown to be useful in identifying patients with portal hypertension. The study aims to establish if the modification of portal <span class="hlt">pressure</span> induced by a transjugular intrahepatic portosystemic shunt (TIPS) parallels the modification of spleen or LS measured by ARFI in order to understand if ARFI may be used to monitor the modification of portal <span class="hlt">pressure</span> in patients with cirrhosis. Thirty-eight patients with severe portal hypertension underwent LS and spleen stiffness (SS) before TIPS and 1 week after TIPS. Portal atrial <span class="hlt">gradient</span> (PAG) was measured before and after the shunt opening. Portal atrial <span class="hlt">gradient</span> decreased significantly from 19.5 to 6 mmHg (P < 0.001). SS decreased significantly after TIPS (pre-TIPS 3.7 m/s vs post-TIPS 3. 1 m/s; P < 0.001), and LS was also significantly modified by TIPS (pre-TIPS 2.8 m/s vs post-TIPS 2.4 m/s; P = 0.003). PAG and SS values measured before and after TIPS were significantly correlated (r = 0.56; P < 0.001); on the other hand, PAG and LS were not (r = 0.19; P = 0.27). Two patients developed a persistent hepatic encephalopathy refractory to medical treatment and were submitted to the reduction of the stent diameter. The modification of SS was parallel to the modification of PAG. Spleen stiffness is superior to LS in detecting the modification of portal <span class="hlt">pressure</span> induced by TIPS. This makes SS a potential non-invasive method to monitor the modification of portal hypertension. Further investigations are needed to establish applicability and clinical utility of this promising tool in the treatment of portal hypertension. © 2017 Journal of Gastroenterology and Hepatology Foundation and John Wiley & Sons Australia, Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994MsT.........17M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994MsT.........17M"><span>Compressible turbulence measurements in a supersonic boundary layer including favorable <span class="hlt">pressure</span> <span class="hlt">gradient</span> effects</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Miller, Raymond S.</p> <p>1994-12-01</p> <p>The effect of a favorable <span class="hlt">pressure</span> <span class="hlt">gradient</span> on the turbulent flow structure in a Mach 2.9 boundary layer (Re/m approximately equal to 1.5 x 10(exp 7)) is investigated experimentally. Conventional flow and hot film measurements of turbulent fluctuation properties have been made upstream of and along an expansion ramp. Upstream measurements were taken in a zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> boundary layer 44 cm from the nozzle throat in a 6.35 cm square test section. Measurements are obtained in the boundary layer, above the expansion ramp, 71.5 cm from the nozzle throat. Mean flow and turbulent flow characteristics are measured in all three dimensions. Comparisons are made between data obtained using single and multiple-overheat cross-wire anemometry as well as conventional mean flow probes. Conventional flow measurements were taken using a Pitot probe and a 10 degree cone static probe. Flow visualization was conducted via imaging techniques (Schlieren and shadowgraph photographs). Results suggest that compressibility effects, as seen through the density fluctuations in the Reynolds shear stress, are roughly 10% relative to the mean velocity and are large relative to the velocity fluctuations. This is also observed in the total Reynolds shear stress; compressibility accounts for 50-75% of the total shear. This is particularly true in the favorable <span class="hlt">pressure</span> <span class="hlt">gradient</span> region, where though the peak fluctuation intensities are diminished, the streamwise component of the mean flow is larger, hence the contribution of the compressibility term is significant in the Reynolds shear.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140002798','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140002798"><span>Vandenberg Air Force Base <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> Wind Study</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shafer, Jaclyn A.</p> <p>2013-01-01</p> <p>Warning category winds can adversely impact day-to-day space lift operations at Vandenberg Air Force Base (VAFB) in California. NASA's Launch Services Program and other programs at VAFB use wind forecasts issued by the 30 Operational Support Squadron Weather Flight (30 OSSWF) to determine if they need to limit activities or protect property such as a launch vehicle. The 30 OSSWF tasked the AMU to develop an automated Excel graphical user interface that includes <span class="hlt">pressure</span> <span class="hlt">gradient</span> thresholds between specific observing stations under different synoptic regimes to aid forecasters when issuing wind warnings. This required the AMU to determine if relationships between the variables existed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NucFu..58d6006S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NucFu..58d6006S"><span>On the physics of the <span class="hlt">pressure</span> and temperature <span class="hlt">gradients</span> in the edge of tokamak plasmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stacey, Weston M.</p> <p>2018-04-01</p> <p>An extended plasma fluid theory including atomic physics, radiation, electromagnetic and themodynamic forces, external sources of particles, momentum and energy, and kinetic ion orbit loss is employed to derive theoretical expressions that display the role of the various factors involved in the determination of the <span class="hlt">pressure</span> and temperature <span class="hlt">gradients</span> in the edge of tokamak plasmas. Calculations for current experiments are presented to illustrate the magnitudes of various effects including strong radiative and atomic physics edge cooling effects and strong reduction in ion particle and energy fluxes due to ion orbit loss in the plasma edge. An important new insight is the strong relation between rotation and the edge <span class="hlt">pressure</span> <span class="hlt">gradient</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DFDG32008A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DFDG32008A"><span>Experimental Measurements of a High Reynolds Num- ber Adverse <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> Turbulent Boundary Layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Atkinson, Callum; Amili, Omid; Stanislas, Michel; Cuvier, Christophe; Foucaut, Jean-Marc; Srinath, Sricharan; Laval, Jean-Philippe; Kaehler, Christian; Hain, Rainer; Scharnowski, Sven; Schroeder, Andreas; Geisler, Reinhard; Agocs, Janos; Roese, Anni; Willert, Christian; Klinner, Joachim; Soria, Julio</p> <p>2016-11-01</p> <p>The study of adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> turbulent boundary layers is complicated by the need to characterise both the local <span class="hlt">pressure</span> <span class="hlt">gradient</span> and it's upstream flow history. It is therefore necessary to measure a significant streamwise domain at a resolution sufficient to resolve the small scales features. To achieve this collaborative particle image velocimetry (PIV) measurements were performed in the large boundary layer wind-tunnel at the Laboratoire de Mecanique de Lille, including: planar measurements spanning a streamwise domain of 3.5m using 16 cameras covering 15 δ spanwise wall-normal stereo-PIV measurements, high-speed micro-PIV of the near wall region and wall shear stress; and streamwise wall-normal PIV in the viscous sub layer. Details of the measurements and preliminary results will be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29234459','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29234459"><span>A Structure Design Method for Reduction of MRI <span class="hlt">Acoustic</span> Noise.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nan, Jiaofen; Zong, Nannan; Chen, Qiqiang; Zhang, Liangliang; Zheng, Qian; Xia, Yongquan</p> <p>2017-01-01</p> <p>The <span class="hlt">acoustic</span> problem of the split <span class="hlt">gradient</span> coil is one challenge in a Magnetic Resonance Imaging and Linear Accelerator (MRI-LINAC) system. In this paper, we aimed to develop a scheme to reduce the <span class="hlt">acoustic</span> noise of the split <span class="hlt">gradient</span> coil. First, a split <span class="hlt">gradient</span> assembly with an asymmetric configuration was designed to avoid vibration in same resonant modes for the two assembly cylinders. Next, the outer ends of the split main magnet were constructed using horn structures, which can distribute the <span class="hlt">acoustic</span> field away from patient region. Finally, a finite element method (FEM) was used to quantitatively evaluate the effectiveness of the above <span class="hlt">acoustic</span> noise reduction scheme. Simulation results found that the noise could be maximally reduced by 6.9 dB and 5.6 dB inside and outside the central gap of the split MRI system, respectively, by increasing the length of one <span class="hlt">gradient</span> assembly cylinder by 20 cm. The optimized horn length was observed to be 55 cm, which could reduce noise by up to 7.4 dB and 5.4 dB inside and outside the central gap, respectively. The proposed design could effectively reduce the <span class="hlt">acoustic</span> noise without any influence on the application of other noise reduction methods.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090004558','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090004558"><span>Evaluation of <span class="hlt">Acoustic</span> Emission NDE of Kevlar Composite Over Wrapped <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>Horne, Michael R.; Madaras, Eric I.</p> <p>2008-01-01</p> <p><span class="hlt">Pressurization</span> and failure tests of small Kevlar/epoxy COPV bottles were conducted during 2006 and 2007 by Texas Research Institute Austin, Inc., at TRI facilities. This is a report of the analysis of the <span class="hlt">Acoustic</span> Emission (AE) data collected during those tests. Results of some of the tests indicate a possibility that AE can be used to track the stress-rupture degradation of COPV vessels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5059748','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5059748"><span>Spontaneous assembly of chemically encoded two-dimensional coacervate droplet arrays by <span class="hlt">acoustic</span> wave patterning</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Tian, Liangfei; Martin, Nicolas; Bassindale, Philip G.; Patil, Avinash J.; Li, Mei; Barnes, Adrian; Drinkwater, Bruce W.; Mann, Stephen</p> <p>2016-01-01</p> <p>The spontaneous assembly of chemically encoded, molecularly crowded, water-rich micro-droplets into periodic defect-free two-dimensional arrays is achieved in aqueous media by a combination of an <span class="hlt">acoustic</span> standing wave <span class="hlt">pressure</span> field and in situ complex coacervation. <span class="hlt">Acoustically</span> mediated coalescence of primary droplets generates single-droplet per node micro-arrays that exhibit variable surface-attachment properties, spontaneously uptake dyes, enzymes and particles, and display spatial and time-dependent fluorescence outputs when exposed to a reactant diffusion <span class="hlt">gradient</span>. In addition, coacervate droplet arrays exhibiting dynamical behaviour and exchange of matter are prepared by inhibiting coalescence to produce <span class="hlt">acoustically</span> trapped lattices of droplet clusters that display fast and reversible changes in shape and spatial configuration in direct response to modulations in the <span class="hlt">acoustic</span> frequencies and fields. Our results offer a novel route to the design and construction of ‘water-in-water' micro-droplet arrays with controllable spatial organization, programmable signalling pathways and higher order collective behaviour. PMID:27708286</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..MARC23009Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..MARC23009Q"><span>Broadband enhanced transmission of <span class="hlt">acoustic</span> waves through serrated metal gratings</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Qi, Dong-Xiang; Fan, Ren-Hao; Deng, Yu-Qiang; Peng, Ru-Wen; Wang, Mu; Jiangnan University Collaboration</p> <p></p> <p>In this talk, we present our studies on broadband properties of <span class="hlt">acoustic</span> waves through metal gratings. We have demonstrated that serrated metal gratings, which introduce <span class="hlt">gradient</span> coatings, can give rise to broadband transmission enhancement of <span class="hlt">acoustic</span> waves. Here, we have experimentally and theoretically studied the <span class="hlt">acoustic</span> transmission properties of metal gratings with or without serrated boundaries. The average transmission is obviously enhanced for serrated metal gratings within a wide frequency range, while the Fabry-Perot resonance is significantly suppressed. An effective medium hypothesis with varying <span class="hlt">acoustic</span> impedance is proposed to analyze the mechanism, which was verified through comparison with finite-element simulation. The serrated boundary supplies <span class="hlt">gradient</span> mass distribution and <span class="hlt">gradient</span> normal <span class="hlt">acoustic</span> impedance, which could efficiently reduce the boundary reflection. Further, by increasing the region of the serrated boundary, we present a broadband high-transmission grating for wide range of incident angle. Our results may have potential applications to broadband <span class="hlt">acoustic</span> imaging, <span class="hlt">acoustic</span> sensing and new <span class="hlt">acoustic</span> devices. References: [1] Dong-Xiang Qi, Yu-Qiang Deng, Di-Hu Xu, Ren-Hao Fan, Ru-Wen Peng, Ze-Guo Chen, Ming-Hui Lu, X. R. Huang and Mu Wang, Appl. Phys. Lett. 106, 011906 (2015); [2] Dong-Xiang Qi, Ren-Hao Fan, Ru-Wen Peng, Xian-Rong Huang, Ming-Hui Lu, Xu Ni, Qing Hu, and Mu Wang, Applied Physics Letters 101, 061912 (2012).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930015352','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930015352"><span>Experimental Study of a Three-Dimensional Shear-Driven Turbulent Boundary Layer with Streamwise Adverse <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Driver, David M.; Johnston, James P.</p> <p>1990-01-01</p> <p>The effects of a strong adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> on a three-dimensional turbulent boundary layer are studied in an axisymmetric spinning cylinder geometry. Velocity measurements made with a three-component laser Doppler velocimeter include all three mean flow components, all six Reynolds stress components, and all ten triple-product correlations. Reynolds stress diminishes as the flow becomes three-dimensional. Lower levels of shear stress were seen to persist under adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> conditions. This low level of stress was seen to roughly correlate with the magnitude of cross-flow (relative to free stream flow) for this experiment as well as most of the other experiments in the literature. Variations in <span class="hlt">pressure</span> <span class="hlt">gradient</span> do not appear to alter this correlation. For this reason, it is hypothesized that a three-dimensional boundary layer is more prone to separate than a two-dimensional boundary layer, although it could not be directly shown here. None of the computations performed with either a Prandtl mixing length, k-epsilon, or a Launder-Reece-Rodi full Reynolds-stress model were able to predict the reduction in Reynolds stress.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29651628','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29651628"><span>Intracranial and Intraocular <span class="hlt">Pressure</span> at the Lamina Cribrosa: <span class="hlt">Gradient</span> Effects.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jóhannesson, Gauti; Eklund, Anders; Lindén, Christina</p> <p>2018-04-12</p> <p>A <span class="hlt">pressure</span> difference between the intraocular and intracranial compartments at the site of the lamina cribrosa has been hypothesized to have a pathophysiological role in several optic nerve head diseases. This paper reviews the current literature on the translamina cribrosa <span class="hlt">pressure</span> difference (TLCPD), the associated <span class="hlt">pressure</span> <span class="hlt">gradient</span>, and its potential pathophysiological role, as well as the methodology to assess TLCPD. For normal-tension glaucoma (NTG), initial studies indicated low intracranial <span class="hlt">pressure</span> (ICP) while recent findings indicate that a reduced ICP is not mandatory. Data from studies on the elevated TLCPD as a pathophysiological factor of NTG are equivocal. From the identification of potential postural effects on the cerebrospinal fluid (CSF) communication between the intracranial and retrolaminar space, we hypothesize that the missing link could be a dysfunction of an occlusion mechanism of the optic nerve sheath around the optic nerve. In upright posture, this could cause an elevated TLCPD even with normal ICP and we suggest that this should be investigated as a pathophysiological component in NTG patients.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22979871','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22979871"><span>The <span class="hlt">acoustic</span> velocity, refractive index, and equation of state of liquid ammonia dihydrate under high <span class="hlt">pressure</span> and high temperature.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ma, Chunli; Wu, Xiaoxin; Huang, Fengxian; Zhou, Qiang; Li, Fangfei; Cui, Qiliang</p> <p>2012-09-14</p> <p>High-<span class="hlt">pressure</span> and high-temperature Brillouin scattering studies have been performed on liquid of composition corresponding to the ammonia dihydrate stoichiometry (NH(3)·2H(2)O) in a diamond anvil cell. Using the measured Brillouin frequency shifts from 180° back- and 60° platelet-scattering geometries, the <span class="hlt">acoustic</span> velocity, refractive index, density, and adiabatic bulk modulus have been determined under <span class="hlt">pressure</span> up to freezing point along the 296, 338, 376, and 407 K isotherms. Along these four isotherms, the <span class="hlt">acoustic</span> velocities increase smoothly with increasing <span class="hlt">pressure</span> but decrease with the increased temperature. However, the <span class="hlt">pressure</span> dependence of the refractive indexes on the four isotherms exhibits a change in slope around 1.5 GPa. The bulk modulus increases linearly with <span class="hlt">pressure</span> and its slope, dB/dP, decreases from 6.83 at 296 K to 4.41 at 407 K. These new datasets improve our understanding of the <span class="hlt">pressure</span>- and temperature-induced molecular structure changes in the ammonia-water binary system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008EPJST.154..271D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008EPJST.154..271D"><span>Thermodynamic properties of isomeric pentanols under elevated <span class="hlt">pressures</span> determined by the <span class="hlt">acoustic</span> method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dzida, M.</p> <p>2008-02-01</p> <p>Three isomeric pentanols were studied: pentan-1-ol, 2-methyl-1-buta- nol, and 2-methyl-2-butanol. Isobaric heat capacities and internal <span class="hlt">pressure</span> at <span class="hlt">pressures</span> up to 100 MPa and temperatures ranging from 293 K to 318 K were determined by the <span class="hlt">acoustic</span> method. In calculations the measured speeds of sound as function of temperature and <span class="hlt">pressure</span> together with densities as function of temperature under atmospheric <span class="hlt">pressure</span> and the literature isobaric heat capacities for the atmospheric <span class="hlt">pressure</span> were used. To this end, the method, based on the suggestion of Davis and Gordon [1] was applied. The results obtained show that the effect of <span class="hlt">pressure</span> on and the values of isobaric heat capacity and internal presure of 2-methyl-2-butanol is higher than that of pentan-1-ol, 2-methyl-1-butanol over the whole <span class="hlt">pressure</span> range. That facilitates telling 2-methyl-2-butanol from pentan-1-ol and 2-methyl-1-butanol.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DFDL35002M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DFDL35002M"><span>Wall-<span class="hlt">pressure</span> fluctuations beneath a spatially evolving turbulent boundary layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mahesh, Krishnan; Kumar, Praveen</p> <p>2016-11-01</p> <p>Wall-<span class="hlt">pressure</span> fluctuations beneath a turbulent boundary layer are important in applications dealing with structural deformation and <span class="hlt">acoustics</span>. Simulations are performed for flat plate and axisymmetric, spatially evolving zero-<span class="hlt">pressure-gradient</span> turbulent boundary layers at inflow Reynolds number of 1400 and 2200 based on momentum thickness. The simulations generate their own inflow using the recycle-rescale method. The results for mean velocity and second-order statistics show excellent agreement with the data available in literature. The spectral characteristics of wall-<span class="hlt">pressure</span> fluctuations and their relation to flow structure will be discussed. This work is supported by ONR.</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.ncbi.nlm.nih.gov/pubmed/28703367','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28703367"><span>Temporal relationship between instantaneous <span class="hlt">pressure</span> <span class="hlt">gradients</span> and peak-to-peak systolic ejection <span class="hlt">gradient</span> in congenital aortic stenosis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Boe, Brian A; Norris, Mark D; Zampi, Jeffrey D; Rocchini, Albert P; Ensing, Gregory J</p> <p>2017-12-01</p> <p>We sought to identify a time during cardiac ejection when the instantaneous <span class="hlt">pressure</span> <span class="hlt">gradient</span> (IPG) correlated best, and near unity, with peak-to-peak systolic ejection <span class="hlt">gradient</span> (PPSG) in patients with congenital aortic stenosis. Noninvasive echocardiographic measurement of IPG has limited correlation with cardiac catheterization measured PPSG across the spectrum of disease severity of congenital aortic stenosis. A major contributor is the observation that these measures are inherently different with a variable relationship dependent on the degree of stenosis. Hemodynamic data from cardiac catheterizations utilizing simultaneous <span class="hlt">pressure</span> measurements from the left ventricle (LV) and ascending aorta (AAo) in patients with congenital valvar aortic stenosis was retrospectively reviewed over the past 5 years. The cardiac cycle was standardized for all patients using the percentage of total LV ejection time (ET). Instantaneous <span class="hlt">gradient</span> at 5% intervals of ET were compared to PPSG using linear regression and Bland-Altman analysis. A total of 22 patients underwent catheterization at a median age of 13.7 years (interquartile range [IQR] 10.3-18.0) and median weight of 51.1 kg (IQR 34.2-71.6). The PPSG was 46.5 ± 12.6 mm Hg (mean ± SD) and correlated suboptimally with the maximum and mean IPG. The midsystolic IPG (occurring at 50% of ET) had the strongest correlation with the PPSG ( PPSG = 0.97(IPG50%)-1.12, R 2  = 0.88), while the IPG at 55% of ET was closest to unity ( PPSG = 0.997(IPG55%)-1.17, R 2  = 0.87). The commonly measured maximum and mean IPG are suboptimal estimates of the PPSG in congenital aortic stenosis. Using catheter-based data, IPG at 50%-55% of ejection correlates well with PPSG. This may allow for a more accurate estimation of PPSG via noninvasive assessment of IPG. © 2017 Wiley Periodicals, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120001736','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120001736"><span>Simulation of <span class="hlt">Acoustics</span> for Ares I Scale Model <span class="hlt">Acoustic</span> Tests</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Putnam, Gabriel; Strutzenberg, Louise L.</p> <p>2011-01-01</p> <p>The Ares I Scale Model <span class="hlt">Acoustics</span> Test (ASMAT) is a series of live-fire tests of scaled rocket motors meant to simulate the conditions of the Ares I launch configuration. These tests have provided a well documented set of high fidelity <span class="hlt">acoustic</span> measurements useful for validation including data taken over a range of test conditions and containing phenomena like Ignition Over-<span class="hlt">Pressure</span> and water suppression of <span class="hlt">acoustics</span>. To take advantage of this data, a digital representation of the ASMAT test setup has been constructed and test firings of the motor have been simulated using the Loci/CHEM computational fluid dynamics software. Results from ASMAT simulations with the rocket in both held down and elevated configurations, as well as with and without water suppression have been compared to <span class="hlt">acoustic</span> data collected from similar live-fire tests. Results of <span class="hlt">acoustic</span> comparisons have shown good correlation with the amplitude and temporal shape of <span class="hlt">pressure</span> features and reasonable spectral accuracy up to approximately 1000 Hz. Major plume and <span class="hlt">acoustic</span> features have been well captured including the plume shock structure, the igniter pulse transient, and the ignition overpressure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012ApPhL.100e4101B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012ApPhL.100e4101B"><span>Thermally induced secondary atomization of droplet in an <span class="hlt">acoustic</span> field</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Basu, Saptarshi; Saha, Abhishek; Kumar, Ranganathan</p> <p>2012-01-01</p> <p>We study the thermal effects that lead to instability and break up in <span class="hlt">acoustically</span> levitated vaporizing fuel droplets. For selective liquids, atomization occurs at the droplet equator under external heating. Short wavelength [Kelvin-Helmholtz (KH)] instability for diesel and bio-diesel droplets triggers this secondary atomization. Vapor <span class="hlt">pressure</span>, latent heat, and specific heat govern the vaporization rate and temperature history, which affect the surface tension <span class="hlt">gradient</span> and gas phase density, ultimately dictating the onset of KH instability. We develop a criterion based on Weber number to define a condition for the inception of secondary atomization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940008881','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940008881"><span>Active control of <span class="hlt">acoustic</span> <span class="hlt">pressure</span> fields using smart material technologies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Banks, H. T.; Smith, R. C.</p> <p>1993-01-01</p> <p>An overview describing the use of piezoceramic patches in reducing noise in a structural <span class="hlt">acoustics</span> setting is presented. The passive and active contributions due to patches which are bonded to an Euler-Bernoulli beam or thin shell are briefly discussed and the results are incorporated into a 2-D structural <span class="hlt">acoustics</span> model. In this model, an exterior noise source causes structural vibrations which in turn lead to interior noise as a result of nonlinear fluid/structure coupling mechanism. Interior sound <span class="hlt">pressure</span> levels are reduced via patches bonded to the flexible boundary (a beam in this case) which generate pure bending moments when an out-of-phase voltage is applied. Well-posedness results for the infinite dimensional system are discussed and a Galerkin scheme for approximating the system dynamics is outlined. Control is implemented by using linear quadratic regulator (LQR) optimal control theory to calculate gains for the linearized system and then feeding these gains back into the nonlinear system of interest. The effectiveness of this strategy for this problem is illustrated in an example.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900002973','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900002973"><span><span class="hlt">Acoustic</span> controlled rotation and orientation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Barmatz, Martin B. (Inventor); Allen, James L. (Inventor)</p> <p>1989-01-01</p> <p><span class="hlt">Acoustic</span> energy is applied to a pair of locations spaced about a chamber, to control rotation of an object levitated in the chamber. Two <span class="hlt">acoustic</span> transducers applying energy of a single <span class="hlt">acoustic</span> mode, one at each location, can (one or both) serve to levitate the object in three dimensions as well as control its rotation. Slow rotation is achieved by initially establishing a large phase difference and/or <span class="hlt">pressure</span> ratio of the <span class="hlt">acoustic</span> waves, which is sufficient to turn the object by more than 45 deg, which is immediately followed by reducing the phase difference and/or <span class="hlt">pressure</span> ratio to maintain slow rotation. A small phase difference and/or <span class="hlt">pressure</span> ratio enables control of the angular orientation of the object without rotating it. The sphericity of an object can be measured by its response to the <span class="hlt">acoustic</span> energy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017amos.confE..20W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017amos.confE..20W"><span>Remote <span class="hlt">Acoustic</span> Imaging of Geosynchronous Satellites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Watson, Z.; Hart, M.</p> <p></p> <p>Identification and characterization of orbiting objects that are not spatially resolved are challenging problems for traditional remote sensing methods. Hyper temporal imaging, enabled by fast, low-noise electro-optical detectors is a new sensing modality which may allow the direct detection of <span class="hlt">acoustic</span> resonances on satellites enabling a new regime of signature and state detection. Detectable signatures may be caused by the oscillations of solar panels, high-gain antennae, or other on-board subsystems driven by thermal <span class="hlt">gradients</span>, fluctuations in solar radiation <span class="hlt">pressure</span>, worn reaction wheels, or orbit maneuvers. Herein we present the first hyper-temporal observations of geosynchronous satellites. Data were collected at the Kuiper 1.54-meter telescope in Arizona using an experimental dual-channel imaging instrument that simultaneously measures light in two orthogonally polarized beams at sampling rates extending up to 1 kHz. In these observations, we see evidence of <span class="hlt">acoustic</span> resonances in the polarization state of satellites. The technique is expected to support object identification and characterization of on-board components and to act as a discriminant between active satellites, debris, and passive bodies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PhDT........45D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PhDT........45D"><span>Propellant injection strategy for suppressing <span class="hlt">acoustic</span> combustion instability</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Diao, Qina</p> <p></p> <p>Shear-coaxial injector elements are often used in liquid-propellant-rocket thrust chambers, where combustion instabilities remain a significant problem. A conventional solution to the combustion instability problem relies on passive control techniques that use empirically-developed hardware such as <span class="hlt">acoustic</span> baffles and tuned cavities. In addition to adding weight and decreasing engine performance, these devices are designed using trial-and-error methods, which do not provide the capability to predict the overall system stability characteristics in advance. In this thesis, two novel control strategies that are based on propellant fluid dynamics were investigated for mitigating <span class="hlt">acoustic</span> instability involving shear-coaxial injector elements. The new control strategies would use a set of controlled injectors allowing local adjustment of propellant flow patterns for each operating condition, particularly when instability could become a problem. One strategy relies on reducing the oxidizer-fuel density <span class="hlt">gradient</span> by blending heavier methane with the main fuel, hydrogen. Another strategy utilizes modifying the equivalence ratio to affect the <span class="hlt">acoustic</span> impedance through mixing and reaction rate changes. The potential effectiveness of these strategies was assessed by conducting unit-physics experiments. Two different model combustors, one simulating a single-element injector test and the other a double-element injector test, were designed and tested for flame-<span class="hlt">acoustic</span> interaction. For these experiments, the Reynolds number of the central oxygen jet was kept between 4700 and 5500 making the injector flames sufficiently turbulent. A compression driver, mounted on one side of the combustor wall, provided controlled <span class="hlt">acoustic</span> excitation to the injector flames, simulating the initial phase of flame-<span class="hlt">acoustic</span> interaction. <span class="hlt">Acoustic</span> excitation was applied either as band-limited white noise forcing between 100 Hz and 5000 Hz or as single-frequency, fixed-amplitude forcing at 1150 Hz</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22129011','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22129011"><span>Ice particles trapped by temperature <span class="hlt">gradients</span> at mbar <span class="hlt">pressure</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kelling, Thorben; Wurm, Gerhard; Dürmann, Christoph</p> <p>2011-11-01</p> <p>In laboratory experiments we observe that ice particles (≤100 μm) entrained in a low <span class="hlt">pressure</span> atmosphere (~1 mbar) get trapped by temperature <span class="hlt">gradients</span> between three reservoirs at different temperature. Confining elements are a peltier element at 250 K (bottom), a liquid nitrogen reservoir at 77 K (top), and the surrounding vacuum chamber at 293 K. Particle levitation and trapping is modeled by an interplay of thermophoresis, photophoresis, and gravity. A number of ice particles are trapped simultaneously in close spatial distance to each other at least up to minutes and are accessible for further experiments. © 2011 American Institute of Physics</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011RScI...82k5105K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011RScI...82k5105K"><span>Ice particles trapped by temperature <span class="hlt">gradients</span> at mbar <span class="hlt">pressure</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kelling, Thorben; Wurm, Gerhard; Dürmann, Christoph</p> <p>2011-11-01</p> <p>In laboratory experiments we observe that ice particles (⩽100 μm) entrained in a low <span class="hlt">pressure</span> atmosphere (˜1 mbar) get trapped by temperature <span class="hlt">gradients</span> between three reservoirs at different temperature. Confining elements are a peltier element at 250 K (bottom), a liquid nitrogen reservoir at 77 K (top), and the surrounding vacuum chamber at 293 K. Particle levitation and trapping is modeled by an interplay of thermophoresis, photophoresis, and gravity. A number of ice particles are trapped simultaneously in close spatial distance to each other at least up to minutes and are accessible for further experiments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFMMR13A1665G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFMMR13A1665G"><span><span class="hlt">Acoustic</span> emissions monitoring and synchrotron X-ray diffraction analysis of mineral dehydrations 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>Gasc, J.; Guillon, S.; Schubnel, A. J.; Brunet, F.; Lathe, C.; Mueller, H.</p> <p>2009-12-01</p> <p>We have monitored from in-situ X-ray diffraction coupled to <span class="hlt">Acoustic</span> Emission (AE) imaging, the behavior of several materials under elevated <span class="hlt">pressures</span> and temperatures (quartz, kaolinite, serpentinite). The samples were placed in a boron-epoxy assembly with an 8mm edge-length and loaded in the MAX80 cubic multi-anvil press installed on the German synchrotron (HASYLAB-DESY, Hamburg). AE were recorded using six piezoceramic transducers (2 MHz eigen frequency) glued on each of the six WC anvils. Full waveforms were acquired using an eight channel digital oscilloscope and a continuous <span class="hlt">acoustic</span> recorder. Our system was first tested using quartz beads (500μm) aggregates. During cold compression performed on these samples many <span class="hlt">acoustic</span> events were recorded and located inside the samples. These are obviously related to the fragile fracturing of the quartz due to the porosity loss. During the heating cycles performed on the same samples, the <span class="hlt">acoustic</span> activity progressively vanishes between 300 and 400°C indicating the transition to the ductile regime towards higher temperatures. Further experiments were performed by mixing 20wt% of kaolinite to the quartz. As a result, the amount of <span class="hlt">acoustic</span> emissions recorded during cold compression is significantly reduced. This is thought to be a result of the ductile behaviour of kaolinite even at low temperatures. This assumption has been confirmed by performing experiments on pure kaolinite which did not produce <span class="hlt">acoustic</span> emissions during cold compression nor during heating cycles up to 1000°C (i.e. beyond the kaolinite dehydration temperature). This set of experiments clearly established that no <span class="hlt">acoustic</span> activity is produced by the assembly and that AEs produced by the samples are accurately located by the software. The behaviour of serpentinite dehydration was then investigated under various <span class="hlt">pressure</span> conditions (i.e. various volume changes), from ~0.6 to ~40kbars. These experiments were performed under deviatoric stress conditions</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.8287S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.8287S"><span><span class="hlt">Acoustic</span> emissions monitoring and synchrotron X-ray diffraction analysis of mineral dehydrations 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>Schubnel, Alexandre; Julien, Gasc; Sophie, Guillon; Fabrice, Brunet; Christian, Lathe; Hans-Joachim, Mueller</p> <p>2010-05-01</p> <p>We have monitored from in-situ X-ray diffraction coupled to <span class="hlt">Acoustic</span> Emission (AE) imaging, the behavior of several materials under elevated <span class="hlt">pressures</span> and temperatures (quartz, kaolinite, serpentinite). The samples were placed in a boron-epoxy assembly with an 8mm edge-length and loaded in the MAX80 cubic multi-anvil press installed on the German synchrotron (HASYLAB-DESY, Hamburg). AE were recorded using six piezoceramic transducers (2 MHz eigen frequency) glued on each of the six WC anvils. Full waveforms were acquired using an eight channel digital oscilloscope and a continuous <span class="hlt">acoustic</span> recorder. Our system was first tested using quartz beads (500μm) aggregates. During cold compression performed on these samples many <span class="hlt">acoustic</span> events were recorded and located inside the samples. These are obviously related to the fragile fracturing of the quartz due to the porosity loss. During the heating cycles performed on the same samples, the <span class="hlt">acoustic</span> activity progressively vanishes between 300 and 400°C indicating the transition to the ductile regime towards higher temperatures. Further experiments were performed by mixing 20wt% of kaolinite to the quartz. As a result, the amount of <span class="hlt">acoustic</span> emissions recorded during cold compression is significantly reduced. This is thought to be a result of the ductile behaviour of kaolinite even at low temperatures. This assumption has been confirmed by performing experiments on pure kaolinite which did not produce <span class="hlt">acoustic</span> emissions during cold compression nor during heating cycles up to 1000°C (i.e. beyond the kaolinite dehydration temperature). This set of experiments clearly established that no <span class="hlt">acoustic</span> activity is produced by the assembly and that AEs produced by the samples are accurately located by the software. The behaviour of serpentinite dehydration was then investigated under various <span class="hlt">pressure</span> conditions (i.e. various volume changes), from ~0.6 to ~40kbars. These experiments were performed under deviatoric stress conditions</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17572748','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17572748"><span><span class="hlt">Pressure</span> measurement in supersonic air flow by differential absorptive laser-induced thermal <span class="hlt">acoustics</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hart, Roger C; Herring, G C; Balla, R Jeffrey</p> <p>2007-06-15</p> <p>Nonintrusive, off-body flow barometry in Mach 2 airflow has been demonstrated in a large-scale supersonic wind tunnel using seedless laser-induced thermal <span class="hlt">acoustics</span> (LITA). The static <span class="hlt">pressure</span> of the gas flow is determined with a novel differential absorption measurement of the ultrasonic sound produced by the LITA pump process. Simultaneously, the streamwise velocity and static gas temperature of the same spatially resolved sample volume were measured with this nonresonant time-averaged LITA technique. Mach number, temperature, and <span class="hlt">pressure</span> have 0.2%, 0.4%, and 4% rms agreement, respectively, in comparison with known free-stream conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090011252','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090011252"><span><span class="hlt">Pressure</span> Measurement in Supersonic Air Flow by Differential Absorptive Laser-Induced Thermal <span class="hlt">Acoustics</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hart, Roger C.; Herring, Gregory C.; Balla, Robert J.</p> <p>2007-01-01</p> <p>Nonintrusive, off-body flow barometry in Mach-2 airflow has been demonstrated in a large-scale supersonic wind tunnel using seedless laser-induced thermal <span class="hlt">acoustics</span> (LITA). The static <span class="hlt">pressure</span> of the gas flow is determined with a novel differential absorption measurement of the ultrasonic sound produced by the LITA pump process. Simultaneously, stream-wise velocity and static gas temperature of the same spatially-resolved sample volume were measured with this nonresonant time-averaged LITA technique. Mach number, temperature and <span class="hlt">pressure</span> have 0.2%, 0.4%, and 4% rms agreement, respectively, in comparison with known free-stream conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27165918','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27165918"><span>Automatic Calculation of Hydrostatic <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> in Patients with Head Injury: A Pilot Study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Moss, Laura; Shaw, Martin; Piper, Ian; Arvind, D K; Hawthorne, Christopher</p> <p>2016-01-01</p> <p>The non-surgical management of patients with traumatic brain injury is the treatment and prevention of secondary insults, such as low cerebral perfusion <span class="hlt">pressure</span> (CPP). Most clinical <span class="hlt">pressure</span> monitoring systems measure <span class="hlt">pressure</span> relative to atmospheric <span class="hlt">pressure</span>. If a patient is managed with their head tilted up, relative to their arterial <span class="hlt">pressure</span> transducer, then a hydrostatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> (HPG) can act against arterial <span class="hlt">pressure</span> and cause significant errors in calculated CPP.To correct for HPG, the arterial <span class="hlt">pressure</span> transducer should be placed level with the intracranial <span class="hlt">pressure</span> transducer. However, this is not always achieved. In this chapter, we describe a pilot study investigating the application of speckled computing (or "specks") for the automatic monitoring of the patient's head tilt and subsequent automatic calculation of HPG. In future applications this will allow us to automatically correct CPP to take into account any HPG.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19840022155','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840022155"><span><span class="hlt">Acoustic</span> <span class="hlt">pressures</span> emanating from a turbomachine stage</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ramachandra, S. M.</p> <p>1984-01-01</p> <p>A knowledge of the <span class="hlt">acoustic</span> energy emission of each blade row of a turbomachine is useful for estimating the overall noise level of the machine and for determining its discrete frequency noise content. Because of the close spacing between the rotor and stator of a compressor stage, the strong aerodynamic interactions between them have to be included in obtaining the resultant flow field. A three dimensional theory for determining the discrete frequency noise content of an axial compressor consisting of a rotor and a stator each with a finite number of blades are outlined. The lifting surface theory and the linearized equation of an ideal, nonsteady compressible fluid motion are used for thin blades of arbitrary cross section. The combined <span class="hlt">pressure</span> field at a point of the fluid is constructed by linear addition of the rotor and stator solutions together with an interference factor obtained by matching them for net zero vorticity behind the stage.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19960015858','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19960015858"><span>A Study of the Development of Steady and Periodic Unsteady Turbulent Wakes Through Curved Channels at Positive, Zero, and Negative Streamwise <span class="hlt">Pressure</span> <span class="hlt">Gradients</span>, Part 1</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schobeiri, M. T.; John, J.</p> <p>1996-01-01</p> <p>The turbomachinery wake flow development is largely influenced by streamline curvature and streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The objective of this investigation is to study the development of the wake under the influence of streamline curvature and streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The experimental investigation is carried out in two phases. The first phase involves the study of the wake behind a stationary circular cylinder (steady wake) in curved channels at positive, zero, and negative streamwise <span class="hlt">pressure</span> <span class="hlt">gradients</span>. The mean velocity and Reynolds stress components are measured using a X-hot-film probe. The measured quantities obtained in probe coordinates are transformed to a curvilinear coordinate system along the wake centerline and are presented in similarity coordinates. The results of the steady wakes suggest strong asymmetry in velocity and Reynolds stress components. However, the velocity defect profiles in similarity coordinates are almost symmetrical and follow the same distribution as the zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> straight wake. The results of Reynolds stress distributions show higher values on the inner side of the wake than the outer side. Other quantities, including the decay of maximum velocity defect, growth of wake width, and wake integral parameters, are also presented for the three different <span class="hlt">pressure</span> <span class="hlt">gradient</span> cases of steady wake. The decay rate of velocity defect is fastest for the negative streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span> case and slowest for the positive <span class="hlt">pressure</span> <span class="hlt">gradient</span> case. Conversely, the growth of the wake width is fastest for the positive streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span> case and slowest for the negative streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The second phase studies the development of periodic unsteady wakes generated by the circular cylinders of the rotating wake generator in a curved channel at zero streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span>. Instantaneous velocity components of the periodic unsteady wakes, measured with a stationary X-hot-film probe, are analyzed by the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26741378','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26741378"><span>Fractional Ablative Laser Followed by Transdermal <span class="hlt">Acoustic</span> <span class="hlt">Pressure</span> Wave Device to Enhance the Drug Delivery of Aminolevulinic Acid: In Vivo Fluorescence Microscopy Study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Waibel, Jill S; Rudnick, Ashley; Nousari, Carlos; Bhanusali, Dhaval G</p> <p>2016-01-01</p> <p>Topical drug delivery is the foundation of all dermatological therapy. Laser-assisted drug delivery (LAD) using fractional ablative laser is an evolving modality that may allow for a greater precise depth of penetration by existing topical medications, as well as more efficient transcutaneous delivery of large drug molecules. Additional studies need to be performed using energy-driven methods that may enhance drug delivery in a synergistic manner. Processes such as iontophoresis, electroporation, sonophoresis, and the use of photomechanical waves aid in penetration. This study evaluated in vivo if there is increased efficacy of fractional CO2 ablative laser with immediate <span class="hlt">acoustic</span> <span class="hlt">pressure</span> wave device. Five patients were treated and biopsied at 4 treatment sites: 1) topically applied aminolevulinic acid (ALA) alone; 2) fractional ablative CO2 laser and topical ALA alone; 3) fractional ablative CO2 laser and transdermal <span class="hlt">acoustic</span> <span class="hlt">pressure</span> wave device delivery system; and 4) topical ALA with transdermal delivery system. The comparison of the difference in the magnitude of diffusion with both lateral spread of ALA and depth diffusion of ALA was measured by fluorescence microscopy. For fractional ablative CO2 laser, ALA, and transdermal <span class="hlt">acoustic</span> <span class="hlt">pressure</span> wave device, the protoporphyrin IX lateral fluorescence was 0.024 mm on average vs 0.0084 mm for fractional ablative CO2 laser and ALA alone. The diffusion for the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> wave device was an order of magnitude greater. We found that our combined approach of fractional ablative CO2 laser paired with the transdermal <span class="hlt">acoustic</span> <span class="hlt">pressure</span> wave device increased the depth of penetration of ALA.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10240E..0HW','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10240E..0HW"><span>Accelerating <span class="hlt">gradient</span> improvement using shape-tailor laser front in radiation <span class="hlt">pressure</span> acceleration progress</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, W. P.; Shen, B. F.; Xu, Z. Z.</p> <p>2017-05-01</p> <p>The accelerating <span class="hlt">gradient</span> of a proton beam is crucial for stable radiation <span class="hlt">pressure</span> acceleration (RPA) because the multi-dimensional instabilities increase γ times slower in the relativistic region. In this paper, a shape-tailored laser is proposed to significantly accelerate the ions in a controllable high accelerating <span class="hlt">gradient</span>. In this method, the fastest ions initially rest in the middle of the foil are controlled to catch the compressed electron layer at the end of the hole-boring stage, thus the light-sail stage can start as soon as possible. Then the compressed electron layer is accelerated tightly together with the fastest ions by the shaped laser intensity, which further increases the accelerating <span class="hlt">gradient</span> in the light-sail stage. Such tailored pulse may be beneficial for the RPA driven by the 10-fs 10 petawatt laser in the future.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1078317','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1078317"><span>Particle analysis in an <span class="hlt">acoustic</span> cytometer</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Kaduchak, Gregory; Ward, Michael D</p> <p>2012-09-18</p> <p>The present invention is a method and apparatus for <span class="hlt">acoustically</span> manipulating one or more particles. <span class="hlt">Acoustically</span> manipulated particles may be separated by size. The particles may be flowed in a flow stream and <span class="hlt">acoustic</span> radiation <span class="hlt">pressure</span>, which may be radial, may be applied to the flow stream. This application of <span class="hlt">acoustic</span> radiation <span class="hlt">pressure</span> may separate the particles. In one embodiment, the particles may be separated by size, and as a further example, the larger particles may be transported to a central axis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18617977','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18617977"><span>Optical analysis of time-averaged multiscale Bessel beams generated by a tunable <span class="hlt">acoustic</span> <span class="hlt">gradient</span> index of refraction lens.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>McLeod, Euan; Arnold, Craig B</p> <p>2008-07-10</p> <p>Current methods for generating Bessel beams are limited to fixed beam sizes or, in the case of conventional adaptive optics, relatively long switching times between beam shapes. We analyze the multiscale Bessel beams created using an alternative rapidly switchable device: a tunable <span class="hlt">acoustic</span> <span class="hlt">gradient</span> index (TAG) lens. The shape of the beams and their nondiffracting, self-healing characteristics are studied experimentally and explained theoretically using both geometric and Fourier optics. By adjusting the electrical driving signal, we can tune the ring spacings, the size of the central spot, and the working distance of the lens. The results presented here will enable researchers to employ dynamic Bessel beams generated by TAG lenses.</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.ncbi.nlm.nih.gov/pubmed/27859549','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27859549"><span>On the accurate analysis of vibroacoustics in head insert <span class="hlt">gradient</span> coils.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Winkler, Simone A; Alejski, Andrew; Wade, Trevor; McKenzie, Charles A; Rutt, Brian K</p> <p>2017-10-01</p> <p>To accurately analyze vibroacoustics in MR head <span class="hlt">gradient</span> coils. A detailed theoretical model for <span class="hlt">gradient</span> coil vibroacoustics, including the first description and modeling of Lorentz damping, is introduced and implemented in a multiphysics software package. Numerical finite-element method simulations were used to establish a highly accurate vibroacoustic model in head <span class="hlt">gradient</span> coils in detail, including the newly introduced Lorentz damping effect. Vibroacoustic coupling was examined through an additional modal analysis. Thorough experimental studies were used to validate simulations. Average experimental sound <span class="hlt">pressure</span> levels (SPLs) and accelerations over the 0-3000 Hz frequency range were 97.6 dB, 98.7 dB, and 95.4 dB, as well as 20.6 g, 8.7 g, and 15.6 g for the X-, Y-, and Z-<span class="hlt">gradients</span>, respectively. A reasonable agreement between simulations and measurements was achieved. Vibroacoustic coupling showed a coupled resonance at 2300 Hz for the Z-<span class="hlt">gradient</span> that is responsible for a sharp peak and the highest SPL value in the <span class="hlt">acoustic</span> spectrum. We have developed and used more realistic multiphysics simulation methods to gain novel insights into the underlying concepts for vibroacoustics in head <span class="hlt">gradient</span> coils, which will permit improved analyses of existing <span class="hlt">gradient</span> coils and novel SPL reduction strategies for future <span class="hlt">gradient</span> coil designs. Magn Reson Med 78:1635-1645, 2017. © 2016 International Society for Magnetic Resonance in Medicine. © 2016 International Society for Magnetic Resonance in Medicine.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20020024643','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20020024643"><span>Flow Control Device Evaluation for an Internal Flow with an Adverse <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jenkins, Luther N.; Gorton, Susan Althoff; Anders, Scott G.</p> <p>2002-01-01</p> <p>The effectiveness of several active and passive devices to control flow in an adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> with secondary flows present was evaluated in the 15 Inch Low Speed Tunnel at NASA Langley Research Center. In this study, passive micro vortex generators, micro bumps, and piezoelectric synthetic jets were evaluated for their flow control characteristics using surface static <span class="hlt">pressures</span>, flow visualization, and 3D Stereo Digital Particle Image Velocimetry. Data also were acquired for synthetic jet actuators in a zero flow environment. It was found that the micro vortex generator is very effective in controlling the flow environment for an adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span>, even in the presence of secondary vortical flow. The mechanism by which the control is effected is a re-energization of the boundary layer through flow mixing. The piezoelectric synthetic jet actuators must have sufficient velocity output to produce strong longitudinal vortices if they are to be effective for flow control. The output of these devices in a laboratory or zero flow environment will be different than the output in a flow environment. In this investigation, the output was higher in the flow environment, but the stroke cycle in the flow did not indicate a positive inflow into the synthetic jet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12703693','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12703693"><span><span class="hlt">Acoustic</span> and mechanical response of reservoir rocks under variable saturation and effective <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>Ravazzoli, C L; Santos, J E; Carcione, J M</p> <p>2003-04-01</p> <p>We investigate the <span class="hlt">acoustic</span> and mechanical properties of a reservoir sandstone saturated by two immiscible hydrocarbon fluids, under different saturations and <span class="hlt">pressure</span> conditions. The modeling of static and dynamic deformation processes in porous rocks saturated by immiscible fluids depends on many parameters such as, for instance, porosity, permeability, pore fluid, fluid saturation, fluid <span class="hlt">pressures</span>, capillary <span class="hlt">pressure</span>, and effective stress. We use a formulation based on an extension of Biot's theory, which allows us to compute the coefficients of the stress-strain relations and the equations of motion in terms of the properties of the single phases at the in situ conditions. The dry-rock moduli are obtained from laboratory measurements for variable confining <span class="hlt">pressures</span>. We obtain the bulk compressibilities, the effective <span class="hlt">pressure</span>, and the ultrasonic phase velocities and quality factors for different saturations and pore-fluid <span class="hlt">pressures</span> ranging from normal to abnormally high values. The objective is to relate the seismic and ultrasonic velocity and attenuation to the microstructural properties and <span class="hlt">pressure</span> conditions of the reservoir. The problem has an application in the field of seismic exploration for predicting pore-fluid <span class="hlt">pressures</span> and saturation regimes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018APExp..11e7301L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018APExp..11e7301L"><span>Metasurface-based angle-selective multichannel <span class="hlt">acoustic</span> refractor</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Bingyi; Jiang, Yongyuan</p> <p>2018-05-01</p> <p>We theoretically study the angle-selective refractions of an impedance-matched <span class="hlt">acoustic</span> <span class="hlt">gradient</span>-index metasurface, which is integrated with a rigid bar array of a deep subwavelength period. An interesting refraction order appears under the all-angle incidence despite the existence of a critical angle, and notably, the odevity of the phase-discretization level apparently selects the transmitted diffraction orders. We utilize the strategy of multilayered media design to realize a three-channel <span class="hlt">acoustic</span> refractor, which shows good promise for constructing multifunctional diffractive <span class="hlt">acoustic</span> elements for <span class="hlt">acoustic</span> communication.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25753157','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25753157"><span>MRI measurements of intracranial <span class="hlt">pressure</span> in the upright posture: The effect of the hydrostatic <span class="hlt">pressure</span> <span class="hlt">gradient</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Alperin, Noam; Lee, Sang H; Bagci, Ahmet M</p> <p>2015-10-01</p> <p>To add the hydrostatic component of the cerebrospinal fluid (CSF) <span class="hlt">pressure</span> to magnetic resonance imaging (MRI)-derived intracranial <span class="hlt">pressure</span> (ICP) measurements in the upright posture for derivation of <span class="hlt">pressure</span> value in a central cranial location often used in invasive ICP measurements. Additional analyses were performed using data previously collected from 10 healthy subjects scanned in supine and sitting positions with a 0.5T vertical gap MRI scanner (GE Medical). Pulsatile blood and CSF flows to and from the brain were quantified using cine phase-contrast. Intracranial compliance and <span class="hlt">pressure</span> were calculated using a previously described method. The vertical distance between the location of the CSF flow measurement and a central cranial location was measured manually in the mid-sagittal T1 -weighted image obtained in the upright posture. The hydrostatic <span class="hlt">pressure</span> <span class="hlt">gradient</span> of a CSF column with similar height was then added to the MR-ICP value. After adjustment for the hydrostatic component, the mean ICP value was reduced by 7.6 mmHg. Mean ICP referenced to the central cranial level was -3.4 ± 1.7 mmHg compared to the unadjusted value of +4.3 ± 1.8 mmHg. In the upright posture, the hydrostatic <span class="hlt">pressure</span> component needs to be added to the MRI-derived ICP values for compatibility with invasive ICP at a central cranial location. © 2015 Wiley Periodicals, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26490348','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26490348"><span><span class="hlt">Acoustic</span> noise reduction in T 1- and proton-density-weighted turbo spin-echo imaging.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ott, Martin; Blaimer, Martin; Breuer, Felix; Grodzki, David; Heismann, Björn; Jakob, Peter</p> <p>2016-02-01</p> <p>To reduce <span class="hlt">acoustic</span> noise levels in T 1-weighted and proton-density-weighted turbo spin-echo (TSE) sequences, which typically reach <span class="hlt">acoustic</span> noise levels up to 100 dB(A) in clinical practice. Five <span class="hlt">acoustic</span> noise reduction strategies were combined: (1) <span class="hlt">gradient</span> ramps and shapes were changed from trapezoidal to triangular, (2) variable-encoding-time imaging was implemented to relax the phase-encoding <span class="hlt">gradient</span> timing, (3) RF pulses were adapted to avoid the need for reversing the polarity of the slice-rewinding <span class="hlt">gradient</span>, (4) readout bandwidth was increased to provide more time for <span class="hlt">gradient</span> activity on other axes, (5) the number of slices per TR was reduced to limit the total <span class="hlt">gradient</span> activity per unit time. We evaluated the influence of each measure on the <span class="hlt">acoustic</span> noise level, and conducted in vivo measurements on a healthy volunteer. Sound recordings were taken for comparison. An overall <span class="hlt">acoustic</span> noise reduction of up to 16.8 dB(A) was obtained by the proposed strategies (1-4) and the acquisition of half the number of slices per TR only. Image quality in terms of SNR and CNR was found to be preserved. The proposed measures in this study allowed a threefold reduction in the <span class="hlt">acoustic</span> perception of T 1-weighted and proton-density-weighted TSE sequences compared to a standard TSE-acquisition. This could be achieved without visible degradation of image quality, showing the potential to improve patient comfort and scan acceptability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22481769','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22481769"><span>High-<span class="hlt">acoustic</span>-impedance tantalum oxide layers for insulating <span class="hlt">acoustic</span> reflectors.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Capilla, Jose; Olivares, Jimena; Clement, Marta; Sangrador, Jesús; Iborra, Enrique; Devos, Arnaud</p> <p>2012-03-01</p> <p>This work describes the assessment of the <span class="hlt">acoustic</span> properties of sputtered tantalum oxide films intended for use as high-impedance films of <span class="hlt">acoustic</span> reflectors for solidly mounted resonators operating in the gigahertz frequency range. The films are grown by sputtering a metallic tantalum target under different oxygen and argon gas mixtures, total <span class="hlt">pressures</span>, pulsed dc powers, and substrate biases. The structural properties of the films are assessed through infrared absorption spectroscopy and X-ray diffraction measurements. Their <span class="hlt">acoustic</span> impedance is assessed by deriving the mass density from X-ray reflectometry measurements and the <span class="hlt">acoustic</span> velocity from picosecond <span class="hlt">acoustic</span> spectroscopy and the analysis of the frequency response of the test resonators.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPA....7f5211Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPA....7f5211Z"><span>A low frequency <span class="hlt">acoustic</span> insulator by using the <span class="hlt">acoustic</span> metasurface to a Helmholtz resonator</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Xiang; Cai, Li; Yu, Dianlong; Lu, Zhimiao; Wen, Jihong</p> <p>2017-06-01</p> <p><span class="hlt">Acoustic</span> metasurfaces (AMSs) are able to manipulate wavefronts at an anomalous angle through a subwavelength layer. Their application provide a new way to control sound waves in addition to traditional materials. In this work, we introduced the AMS into the design of a Helmholtz resonator (HR) and studied the <span class="hlt">acoustic</span> transmission through the modified HR in a pipe with one branch. The variation of sound insulation capacity with the phase <span class="hlt">gradient</span> of the AMS was studied, and the results show that the AMS can remarkably lower the frequency band of the sound insulation without increasing the size. Our investigation provides a new degree of freedom for <span class="hlt">acoustic</span> control with a Helmholtz resonator, which is of great significance in <span class="hlt">acoustic</span> metasurface theory and sound insulation design.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910034781&hterms=sensors+pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dsensors%2Bpressure','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910034781&hterms=sensors+pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dsensors%2Bpressure"><span>The effects of <span class="hlt">pressure</span> sensor <span class="hlt">acoustics</span> on airdata derived from a high-angle-of-attack flush airdata sensing (HI-FADS) system</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Whitmore, Stephen R.; Moes, Timothy R.</p> <p>1991-01-01</p> <p>The accuracy of a prototype nonintrusive airdata system derived for high-angle-of-attack measurements was demonstrated for quasi-steady maneuvers as great as 55 degrees during phase one of the F-18 high alpha research vehicle flight test program. This system consists of a matrix of nine <span class="hlt">pressure</span> ports arranged in annular rings on the aircraft nose, and estimates the complete airdata set utilizing flow modeling and nonlinear regression. Particular attention is paid to the effects of <span class="hlt">acoustical</span> distortions within the individual <span class="hlt">pressure</span> sensors of the HI-FADS <span class="hlt">pressure</span> matrix. A dynamic model to quantify these effects which describes <span class="hlt">acoustical</span> distortion is developed and solved in closed form for frequency response.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhDT.......221S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhDT.......221S"><span>Implementing and testing a panel-based method for modeling <span class="hlt">acoustic</span> scattering from CFD input</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Swift, S. Hales</p> <p></p> <p>Exposure of sailors to high levels of noise in the aircraft carrier deck environment is a problem that has serious human and economic consequences. A variety of approaches to quieting exhausting jets from high-performance aircraft are undergoing development. However, testing of noise abatement solutions at full-scale may be prohibitively costly when many possible nozzle treatments are under consideration. A relatively efficient and accurate means of predicting the noise levels resulting from engine-quieting technologies at personnel locations is needed. This is complicated by the need to model both the direct and the scattered sound field in order to determine the resultant spectrum and levels. While the direct sound field may be obtained using CFD plus surface integral methods such as the Ffowcs-Williams Hawkings method, the scattered sound field is complicated by its dependence on the geometry of the scattering surface--the aircraft carrier deck, aircraft control surfaces and other nearby structures. In this work, a time-domain boundary element method, or TD-BEM, (sometimes referred to in terms of source panels) is proposed and developed that takes advantage of and offers beneficial effects for the substantial planar components of the aircraft carrier deck environment and uses <span class="hlt">pressure</span> <span class="hlt">gradients</span> as its input. This method is applied to and compared with analytical results for planar surfaces, corners and spherical surfaces using an analytic point source as input. The method can also accept input from CFD data on an <span class="hlt">acoustic</span> data surface by using the G1A <span class="hlt">pressure</span> <span class="hlt">gradient</span> formulation to obtain <span class="hlt">pressure</span> <span class="hlt">gradients</span> on the surface from the flow variables contained on the <span class="hlt">acoustic</span> data surface. The method is also applied to a planar scattering surface characteristic of an aircraft carrier flight deck with an <span class="hlt">acoustic</span> data surface from a supersonic jet large eddy simulation, or LES, as input to the scattering model. In this way, the process for modeling the complete</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950014614','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950014614"><span>Wake measurements in a strong adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hoffenberg, R.; Sullivan, John P.; Schneider, S. P.</p> <p>1994-01-01</p> <p>The behavior of wakes in adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> is critical to the performance of high-lift systems for transport aircraft. Wake deceleration is known to lead to sudden thickening and the onset of reversed flow; this 'wake bursting' phenomenon can occur while surface flows remain attached. Although 'wake bursting' is known to be important for high-lift systems, no detailed measurements of 'burst' wakes have ever been reported. Wake bursting has been successfully achieved in the wake of a flat plate as it decelerated in a two-dimensional diffuser, whose sidewalls were forced to remain attached by use of slot blowing. Pilot probe surveys, L.D.V. measurements, and flow visualization have been used to investigate the physics of this decelerated wake, through the onset of reversed flow.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26940013','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26940013"><span>Cardiomyopathy in children: Can we rely on echocardiographic tricuspid regurgitation <span class="hlt">gradient</span> estimates of right ventricular and pulmonary arterial <span class="hlt">pressure</span>?</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lee, Simon; Lytrivi, Irene D; Roytman, Zhanna; Ko, Hyun-Sook Helen; Vinograd, Cheryl; Srivastava, Shubhika</p> <p>2016-10-01</p> <p>Introduction Agreement between echocardiography and right heart catheterisation-derived right ventricular systolic <span class="hlt">pressure</span> is modest in the adult heart failure population, but is unknown in the paediatric cardiomyopathy population. All patients at a single centre from 2001 to 2012 with a diagnosis of cardiomyopathy who underwent echocardiography and catheterisation within 30 days were included in this study. The correlation between tricuspid regurgitation <span class="hlt">gradient</span> and catheterisation-derived right ventricular systolic <span class="hlt">pressure</span> and mean pulmonary artery <span class="hlt">pressure</span> was determined. Agreement between echocardiography and catheterisation-derived right ventricular systolic <span class="hlt">pressure</span> was assessed using Bland-Altman plots. Analysis was repeated for patients who underwent both procedures within 7 days. Haemodynamic data from those with poor agreement and good agreement between echocardiography and catheterisation were compared. A total of 37 patients who underwent 48 catheterisation procedures were included in our study. The median age was 11.8 (0.1-20.6 years) with 22 males (58% total). There was a modest correlation (r=0.65) between echocardiography and catheterisation-derived right ventricular systolic <span class="hlt">pressure</span>, but agreement was poor. Agreement between tricuspid regurgitation <span class="hlt">gradient</span> and right ventricular systolic <span class="hlt">pressure</span> showed wide 95% limits of agreement. There was a modest correlation between the tricuspid regurgitation <span class="hlt">gradient</span> and mean pulmonary artery <span class="hlt">pressure</span> (r=0.6). Shorter time interval between the two studies did not improve agreement. Those with poor agreement between echocardiography and catheterisation had higher right heart <span class="hlt">pressures</span>, but this difference became insignificant after accounting for right atrial <span class="hlt">pressure</span>. Transthoracic echocardiography estimation of right ventricular systolic <span class="hlt">pressure</span> shows modest correlation with right heart <span class="hlt">pressures</span>, but has limited agreement and may underestimate the degree of pulmonary hypertension in paediatric</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19830054819&hterms=employment+work&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Demployment%2Bwork','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19830054819&hterms=employment+work&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Demployment%2Bwork"><span>A comparison of methods for computing the sigma-coordinate <span class="hlt">pressure</span> <span class="hlt">gradient</span> force for flow over sloped terrain in a hybrid theta-sigma model</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Johnson, D. R.; Uccellini, L. W.</p> <p>1983-01-01</p> <p>In connection with the employment of the sigma coordinates introduced by Phillips (1957), problems can arise regarding an accurate finite-difference computation of the <span class="hlt">pressure</span> <span class="hlt">gradient</span> force. Over steeply sloped terrain, the calculation of the sigma-coordinate <span class="hlt">pressure</span> <span class="hlt">gradient</span> force involves computing the difference between two large terms of opposite sign which results in large truncation error. To reduce the truncation error, several finite-difference methods have been designed and implemented. The present investigation has the objective to provide another method of computing the sigma-coordinate <span class="hlt">pressure</span> <span class="hlt">gradient</span> force. Phillips' method is applied for the elimination of a hydrostatic component to a flux formulation. The new technique is compared with four other methods for computing the <span class="hlt">pressure</span> <span class="hlt">gradient</span> force. The work is motivated by the desire to use an isentropic and sigma-coordinate hybrid model for experiments designed to study flow near mountainous terrain.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870033194&hterms=coulomb+law&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dcoulomb%2Blaw','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870033194&hterms=coulomb+law&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dcoulomb%2Blaw"><span>Beam-induced <span class="hlt">pressure</span> <span class="hlt">gradients</span> in the early phase of proton-heated solar flares</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tamres, David H.; Canfield, Richard C.; Mcclymont, A. N.</p> <p>1986-01-01</p> <p>The <span class="hlt">pressure</span> <span class="hlt">gradient</span> induced in a coronal loop by proton beam momentum deposition is calculated and compared with the thermal <span class="hlt">pressure</span> <span class="hlt">gradient</span> arising from nonuniform deposition of beam energy; it is assumed that the transfer of momentum and energy from beam to target occurs via the Coulomb interaciton. Results are presented for both a low mean energy and a high mean energy proton beam injected at the loop apex and characterized by a power-law energy spectrum. The present treatment takes account of the breakdown of the cold target approximation for the low-energy proton beam in the corona, where the thermal speed of target electrons exceeds the beam speed. It is found that proton beam momentum deposition plays a potentially significant role in flare dynamics only in the low mean energy case and only in the corona, where it may dominate the acceleration of target material for as long as several tens of seconds. This conclusion suggest that the presence of low-energy nonthermal protons may be inferred from velocity-sensitive coronal observations in the early impulsive phase.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5316482','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5316482"><span>Broadening of Analyte Streams due to a Transverse <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> in Free-Flow Isoelectric Focusing</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Dutta, Debashis</p> <p>2017-01-01</p> <p><span class="hlt">Pressure</span>-driven cross-flows can arise in free-flow isoelectric focusing systems (FFIEF) due to a non-uniform electroosmotic flow velocity along the channel width induced by the pH <span class="hlt">gradient</span> in this direction. In addition, variations in the channel cross-section as well as unwanted differences in hydrostatic heads at the buffer/sample inlet ports can also lead to such <span class="hlt">pressure-gradients</span> which besides altering the equilibrium position of the sample zones have a tendency to substantially broaden their widths deteriorating the separations. In this situation, a thorough assessment of stream broadening due to transverse <span class="hlt">pressure-gradients</span> in FFIEF devices is necessary in order to establish accurate design rules for the assay. The present article describes a mathematical framework to estimate the noted zone dispersion in FFIEF separations based on the method-of-moments approach under laminar flow conditions. A closed-form expression has been derived for the spatial variance of the analyte streams at their equilibrium positions as a function of the various operating parameters governing the assay performance. This expression predicts the normalized stream variance under the chosen conditions to be determined by two dimensionless Péclet numbers evaluated based on the transverse <span class="hlt">pressure</span>-driven and electrophoretic solute velocities in the separation chamber, respectively. Moreover, the analysis shows that while the stream width can be expected to increase with an increase in the value of the first Péclet number, the opposite trend will be followed with respect to the latter. The noted results have been validated using Monte Carlo simulations that also establish a time/length scale over which the predicted equilibrium stream width is attained in the system. PMID:28081900</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1434514','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1434514"><span><span class="hlt">Acoustic</span> building infiltration measurement system</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>Muehleisen, Ralph T.; Raman, Ganesh</p> <p></p> <p>Systems and methods of detecting and identifying a leak from a container or building. <span class="hlt">Acoustic</span> <span class="hlt">pressure</span> and velocity are measured. <span class="hlt">Acoustic</span> properties are acquired from the measured values. The <span class="hlt">acoustic</span> properties are converted to infiltration/leakage information. Nearfield <span class="hlt">Acoustic</span> Holography (NAH) may be one method to detect the leakages from a container by locating the noise sources.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25771332','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25771332"><span>Influences of non-uniform <span class="hlt">pressure</span> field outside bubbles on the propagation of <span class="hlt">acoustic</span> waves in dilute bubbly liquids.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Yuning; Du, Xiaoze</p> <p>2015-09-01</p> <p>Predictions of the propagation of the <span class="hlt">acoustic</span> waves in bubbly liquids is of great importance for bubble dynamics and related applications (e.g. sonochemistry, sonochemical reactor design, biomedical engineering). In the present paper, an approach for modeling the propagation of the <span class="hlt">acoustic</span> waves in dilute bubbly liquids is proposed through considering the non-uniform <span class="hlt">pressure</span> field outside the bubbles. This approach is validated through comparing with available experimental data in the literature. Comparing with the previous models, our approach mainly improves the predictions of the attenuation of <span class="hlt">acoustic</span> waves in the regions with large kR0 (k is the wave number and R0 is the equilibrium bubble radius). Stability of the oscillating bubbles under <span class="hlt">acoustic</span> excitation are also quantitatively discussed based on the analytical solution. Copyright © 2015 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920015092','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920015092"><span><span class="hlt">Acoustic</span> intensity calculations for axisymmetrically modeled fluid regions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hambric, Stephen A.; Everstine, Gordon C.</p> <p>1992-01-01</p> <p>An algorithm for calculating <span class="hlt">acoustic</span> intensities from a time harmonic <span class="hlt">pressure</span> field in an axisymmetric fluid region is presented. <span class="hlt">Acoustic</span> <span class="hlt">pressures</span> are computed in a mesh of NASTRAN triangular finite elements of revolution (TRIAAX) using an analogy between the scalar wave equation and elasticity equations. <span class="hlt">Acoustic</span> intensities are then calculated from <span class="hlt">pressures</span> and <span class="hlt">pressure</span> derivatives taken over the mesh of TRIAAX elements. Intensities are displayed as vectors indicating the directions and magnitudes of energy flow at all mesh points in the <span class="hlt">acoustic</span> field. A prolate spheroidal shell is modeled with axisymmetric shell elements (CONEAX) and submerged in a fluid region of TRIAAX elements. The model is analyzed to illustrate the <span class="hlt">acoustic</span> intensity method and the usefulness of energy flow paths in the understanding of the response of fluid-structure interaction problems. The structural-<span class="hlt">acoustic</span> analogy used is summarized for completeness. This study uncovered a NASTRAN limitation involving numerical precision issues in the CONEAX stiffness calculation causing large errors in the system matrices for nearly cylindrical cones.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730006564','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730006564"><span>The turbulent boundary layer on a porous plate: An experimental study of the heat transfer behavior with adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Blackwell, B. F.; Kays, W. M.; Moffat, R. J.</p> <p>1972-01-01</p> <p>An experimental investigation of the heat transfer behavior of the near equilibrium transpired turbulent boundary layer with adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> has been carried out. Stanton numbers were measured by an energy balance on electrically heated plates that form the bottom wall of the wind tunnel. Two adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> were studied. Two types of transpiration boundary conditions were investigated. The concept of an equilibrium thermal boundary layer was introduced. It was found that Stanton number as a function of enthalpy thickness Reynolds number is essentially unaffected by adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> with no transpiration. Shear stress, heat flux, and turbulent Prandtl number profiles were computed from mean temperature and velocity profiles. It was concluded that the turbulent Prandtl number is greater than unity in near the wall and decreases continuously to approximately 0.5 at the free stream.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24787565','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24787565"><span>Analysis of the intraocular jet flows and <span class="hlt">pressure</span> <span class="hlt">gradients</span> induced by air and fluid infusion: mechanism of focal chorioretinal damage.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kim, Yong Joon; Jo, Sungkil; Moon, Daruchi; Joo, Youngcheol; Choi, Kyung Seek</p> <p>2014-05-01</p> <p>To comprehend the mechanism of focal chorioretinal damage by analysis of the <span class="hlt">pressure</span> distribution and dynamic <span class="hlt">pressure</span> induced by infused air during fluid-air exchange. A precise simulation featuring a model eye and a fluid circuit was designed to analyze fluid-air exchange. The <span class="hlt">pressure</span> distribution, flow velocity, and dynamic <span class="hlt">pressure</span> induced by infusion of air into an air-filled eye were analyzed using an approach based on fluid dynamics. The size of the port and the infusion <span class="hlt">pressure</span> were varied during simulated iterations. We simulated infusion of an air-filled eye with balanced salt solution (BSS) to better understand the mechanism of chorioretinal damage induced by infused air. Infused air was projected straight toward a point on the retina contralateral to the infusion port (the "vulnerable point"). The highest <span class="hlt">pressure</span> was evident at the vulnerable point, and the lowest <span class="hlt">pressure</span> was recorded on most retinal areas. Simulations using greater infusion <span class="hlt">pressure</span> and a port of larger size were associated with elevations in dynamic <span class="hlt">pressure</span> and the <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The <span class="hlt">pressure</span> <span class="hlt">gradients</span> were 2.8 and 5.1 mm Hg, respectively, when infusion <span class="hlt">pressures</span> of 30 and 50 mm Hg were delivered through a 20-gauge port. The <span class="hlt">pressure</span> <span class="hlt">gradient</span> associated with BSS infusion was greater than that created by air, but lasted for only a moment. Our simulation explains the mechanism of focal chorioretinal damage in numerical terms. Infused air induces a prolonged increase in focal <span class="hlt">pressure</span> on the vulnerable point, and this may be responsible for visual field defects arising after fluid-air exchange. Copyright 2014 The Association for Research in Vision and Ophthalmology, Inc.</p> </li> </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('http://adsabs.harvard.edu/abs/2011APS..DFD.M7003H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011APS..DFD.M7003H"><span>Zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> boundary layer at extreme Reynolds numbers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hultmark, Marcus; Vallikivi, Margit; Smits, Alexander</p> <p>2011-11-01</p> <p>Experiments were conducted in a zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> flat plate boundary layer using the Princeton/ONR High Reynolds number Test Facility (HRTF). The HRTF uses highly compressed air, up to 220 atmospheres, to produce Reynolds numbers up to Reθ =225,000 . This corresponds to a δ+ =65,000 which is one of the highest Reynolds numbers ever measured in a laboratory. When using <span class="hlt">pressure</span> to achieve high Reynolds numbers the size of the measurement probes become critical, thus the need for very small sensors is acute. The streamwise component of velocity was investigated using a nanoscale thermal anemometer (NSTAP) as well as a 200 μm pitot tube. The NSTAP has a spatial resolution as well as a temporal resolution one order of magnitude better than conventional measurement techniques. The data was compared to recent data from a high Reynolds number turbulent pipe flow and it was shown that the two flows are more similar than previous data suggests. Supported under NR Grant N00014-09-1-0263 (program manager Ron Joslin) and NSF Grant CBET-1064257(program manager Henning Winter).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/20999347-vertical-two-phase-flow-regimes-pressure-gradients-under-influence-sds-surfactant','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/20999347-vertical-two-phase-flow-regimes-pressure-gradients-under-influence-sds-surfactant"><span>Vertical two-phase flow regimes and <span class="hlt">pressure</span> <span class="hlt">gradients</span> under the influence of SDS surfactant</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Duangprasert, Tanabordee; Sirivat, Anuvat; Siemanond, Kitipat</p> <p>2008-01-15</p> <p>Two-phase gas/liquid flows in vertical pipes have been systematically investigated. Water and SDS surfactant solutions at various concentrations were used as the working fluids. In particular, we focus our work on the influence of surfactant addition on the flow regimes, the corresponding <span class="hlt">pressure</span> <span class="hlt">gradients</span>, and the bubble sizes and velocity. Adding the surfactant lowers the air critical Reynolds numbers for the bubble-slug flow and the slug flow transitions. The <span class="hlt">pressure</span> <span class="hlt">gradients</span> of SDS solutions are lower than those of pure water especially in the slug flow and the slug-churn flow regimes, implying turbulent drag reduction. At low Re{sub air}, themore » bubble sizes of the surfactant solution are lower than those of pure water due to the increase in viscosity. With increasing and at high Re{sub air}, the bubble sizes of the SDS solution become greater than those of pure water which is attributed to the effect of surface tension. (author)« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JAP...114k4903D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JAP...114k4903D"><span>Physics of thermo-<span class="hlt">acoustic</span> sound generation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Daschewski, M.; Boehm, R.; Prager, J.; Kreutzbruck, M.; Harrer, A.</p> <p>2013-09-01</p> <p>We present a generalized analytical model of thermo-<span class="hlt">acoustic</span> sound generation based on the analysis of thermally induced energy density fluctuations and their propagation into the adjacent matter. The model provides exact analytical prediction of the sound <span class="hlt">pressure</span> generated in fluids and solids; consequently, it can be applied to arbitrary thermal power sources such as thermophones, plasma firings, laser beams, and chemical reactions. Unlike existing approaches, our description also includes <span class="hlt">acoustic</span> near-field effects and sound-field attenuation. Analytical results are compared with measurements of sound <span class="hlt">pressures</span> generated by thermo-<span class="hlt">acoustic</span> transducers in air for frequencies up to 1 MHz. The tested transducers consist of titanium and indium tin oxide coatings on quartz glass and polycarbonate substrates. The model reveals that thermo-<span class="hlt">acoustic</span> efficiency increases linearly with the supplied thermal power and quadratically with thermal excitation frequency. Comparison of the efficiency of our thermo-<span class="hlt">acoustic</span> transducers with those of piezoelectric-based airborne ultrasound transducers using impulse excitation showed comparable sound <span class="hlt">pressure</span> values. The present results show that thermo-<span class="hlt">acoustic</span> transducers can be applied as broadband, non-resonant, high-performance ultrasound sources.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16793107','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16793107"><span><span class="hlt">Acoustical</span> experiment of yogurt fermentation process.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ogasawara, H; Mizutani, K; Ohbuchi, T; Nakamura, T</p> <p>2006-12-22</p> <p>One of the important factors through food manufacturing is hygienic management. Thus, food manufactures prove their hygienic activities by taking certifications like a Hazard Analysis and Critical Control Point (HACCP). This concept also applies to food monitoring. <span class="hlt">Acoustical</span> measurements have advantage for other measurement in food monitoring because they make it possible to measure with noncontact and nondestructive. We tried to monitor lactic fermentation of yogurt by a probing sensor using a pair of <span class="hlt">acoustic</span> transducers. Temperature of the solution changes by the reaction heat of fermentation. Consequently the sound velocity propagated through the solution also changes depending on the temperature. At the same time, the solution change its phase from liquid to gel. The transducers usage in the solution indicates the change of the temperature as the change of the phase difference between two transducers. The <span class="hlt">acoustic</span> method has advantages of nondestructive measurement that reduces contamination of food product by measuring instrument. The sensor was inserted into milk with lactic acid bacterial stain of 19 degrees C and monitored phase retardation of propagated <span class="hlt">acoustic</span> wave and its temperature with thermocouples in the mild. The monitoring result of fermentation from milk to Caspian Sea yogurt by the <span class="hlt">acoustic</span> transducers with the frequency of 3.7 MHz started to show <span class="hlt">gradient</span> change in temperature caused by reaction heat of fermentation but stop the <span class="hlt">gradient</span> change at the end although the temperature still change. The <span class="hlt">gradient</span> change stopped its change because of phase change from liquid to gel. The present method will be able to measure indirectly by setting transducers outside of the measuring object. This noncontact sensing method will have great advantage of reduces risk of food contamination from measuring instrument because the measurement probes are set out of fermentation reactor or food containers. Our proposed method will contribute to the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24209296','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24209296"><span>Fast <span class="hlt">gradient</span> separation by very high <span class="hlt">pressure</span> liquid chromatography: reproducibility of analytical data and influence of delay between successive runs.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Stankovicha, Joseph J; Gritti, Fabrice; Beaver, Lois Ann; Stevensona, Paul G; Guiochon, Georges</p> <p>2013-11-29</p> <p>Five methods were used to implement fast <span class="hlt">gradient</span> separations: constant flow rate, constant column-wall temperature, constant inlet <span class="hlt">pressure</span> at moderate and high <span class="hlt">pressures</span> (controlled by a <span class="hlt">pressure</span> controller),and programmed flow constant <span class="hlt">pressure</span>. For programmed flow constant <span class="hlt">pressure</span>, the flow rates and <span class="hlt">gradient</span> compositions are controlled using input into the method instead of the <span class="hlt">pressure</span> controller. Minor fluctuations in the inlet <span class="hlt">pressure</span> do not affect the mobile phase flow rate in programmed flow. There producibilities of the retention times, the response factors, and the eluted band width of six successive separations of the same sample (9 components) were measured with different equilibration times between 0 and 15 min. The influence of the length of the equilibration time on these reproducibilities is discussed. The results show that the average column temperature may increase from one separation to the next and that this contributes to fluctuation of the results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040087555&hterms=Gradient&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DGradient','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040087555&hterms=Gradient&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DGradient"><span>Improvement in diastolic intraventricular <span class="hlt">pressure</span> <span class="hlt">gradients</span> in patients with HOCM after ethanol septal reduction</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rovner, Aleksandr; Smith, Rebecca; Greenberg, Neil L.; Tuzcu, E. Murat; Smedira, Nicholas; Lever, Harry M.; Thomas, James D.; Garcia, Mario J.</p> <p>2003-01-01</p> <p>We sought to validate measurement of intraventricular <span class="hlt">pressure</span> <span class="hlt">gradients</span> (IVPG) and analyze their change in patients with hypertrophic obstructive cardiomyopathy (HOCM) after ethanol septal reduction (ESR). Quantitative analysis of color M-mode Doppler (CMM) images may be used to estimate diastolic IVPG noninvasively. Noninvasive IVPG measurement was validated in 10 patients undergoing surgical myectomy. Echocardiograms were then analyzed in 19 patients at baseline and after ESR. Pulsed Doppler data through the mitral valve and pulmonary venous flow were obtained. CMM was used to obtain the flow propagation velocity (Vp) and to calculate IVPG off-line. Left atrial <span class="hlt">pressure</span> was estimated with the use of previously validated Doppler equations. Data were compared before and after ESR. CMM-derived IVPG correlated well with invasive measurements obtained before and after surgical myectomy [r = 0.8, P < 0.01, Delta(CMM - invasive IVPG) = 0.09 +/- 0.45 mmHg]. ESR resulted in a decrease of resting LVOT systolic <span class="hlt">gradient</span> from 62 +/- 10 to 29 +/- 5 mmHg (P < 0.001). There was a significant increase in the Vp and IVPG (from 48 +/- 5to 74 +/- 7 cm/s and from 1.5 +/- 0.2 to 2.6 +/- 0.3 mmHg, respectively, P < 0.001 for both). Estimated left atrial <span class="hlt">pressure</span> decreased from 16.2 +/- 1.1 to 11.5 +/- 0.9 mmHg (P < 0.001). The increase in IVPG correlated with the reduction in the LVOT <span class="hlt">gradient</span> (r = 0.6, P < 0.01). Reduction of LVOT obstruction after ESR is associated with an improvement in diastolic suction force. Noninvasive measurements of IVPG may be used as an indicator of diastolic function improvement in HOCM.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910007747','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910007747"><span>The effects of <span class="hlt">pressure</span> sensor <span class="hlt">acoustics</span> on airdata derived from a High-angle-of-attack Flush Airdata Sensing (HI-FADS) system</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.; Moes, Timothy R.</p> <p>1991-01-01</p> <p>The accuracy of a nonintrusive high angle-of-attack flush airdata sensing (HI-FADS) system was verified for quasi-steady flight conditions up to 55 deg angle of attack during the F-18 High Alpha Research Vehicle (HARV) Program. The system is a matrix of nine <span class="hlt">pressure</span> ports arranged in annular rings on the aircraft nose. The complete airdata set is estimated using nonlinear regression. Satisfactory frequency response was verified to the system Nyquist frequency (12.5 Hz). The effects of <span class="hlt">acoustical</span> distortions within the individual <span class="hlt">pressure</span> sensors of the nonintrusive <span class="hlt">pressure</span> matrix on overall system performance are addressed. To quantify these effects, a frequency-response model describing the dynamics of <span class="hlt">acoustical</span> distortion is developed and simple design criteria are derived. The model adjusts measured HI-FADS <span class="hlt">pressure</span> data for the <span class="hlt">acoustical</span> distortion and quantifies the effects of internal sensor geometries on system performance. Analysis results indicate that sensor frequency response characteristics very greatly with altitude, thus it is difficult to select satisfactory sensor geometry for all altitudes. The solution used presample filtering to eliminate resonance effects, and short pneumatic tubing sections to reduce lag effects. Without presample signal conditioning the system designer must use the pneumatic transmission line to attenuate the resonances and accept the resulting altitude variability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17069306','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17069306"><span>A forward model and conjugate <span class="hlt">gradient</span> inversion technique for low-frequency ultrasonic imaging.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>van Dongen, Koen W A; Wright, William M D</p> <p>2006-10-01</p> <p>Emerging methods of hyperthermia cancer treatment require noninvasive temperature monitoring, and ultrasonic techniques show promise in this regard. Various tomographic algorithms are available that reconstruct sound speed or contrast profiles, which can be related to temperature distribution. The requirement of a high enough frequency for adequate spatial resolution and a low enough frequency for adequate tissue penetration is a difficult compromise. In this study, the feasibility of using low frequency ultrasound for imaging and temperature monitoring was investigated. The transient probing wave field had a bandwidth spanning the frequency range 2.5-320.5 kHz. The results from a forward model which computed the propagation and scattering of low-frequency <span class="hlt">acoustic</span> <span class="hlt">pressure</span> and velocity wave fields were used to compare three imaging methods formulated within the Born approximation, representing two main types of reconstruction. The first uses Fourier techniques to reconstruct sound-speed profiles from projection or Radon data based on optical ray theory, seen as an asymptotical limit for comparison. The second uses backpropagation and conjugate <span class="hlt">gradient</span> inversion methods based on <span class="hlt">acoustical</span> wave theory. The results show that the accuracy in localization was 2.5 mm or better when using low frequencies and the conjugate <span class="hlt">gradient</span> inversion scheme, which could be used for temperature monitoring.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19810012482','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19810012482"><span>The influence of a high <span class="hlt">pressure</span> <span class="hlt">gradient</span> on unsteady velocity perturbations in the case of a turbulent supersonic flow</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dussauge, J. P.; Debieve, J. F.</p> <p>1980-01-01</p> <p>The amplification or reduction of unsteady velocity perturbations under the influence of strong flow acceleration or deceleration was studied. Supersonic flows with large velocity, <span class="hlt">pressure</span> <span class="hlt">gradients</span>, and the conditions in which the velocity fluctuations depend on the action of the average <span class="hlt">gradients</span> of <span class="hlt">pressure</span> and velocity rather than turbulence, are described. Results are analyzed statistically and interpreted as a return to laminar process. It is shown that this return to laminar implies negative values in the turbulence production terms for kinetic energy. A simple geometrical representation of the Reynolds stress production is given.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JSV...410..485D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JSV...410..485D"><span>Comment on "the one dimensional <span class="hlt">acoustic</span> field with arbitrary mean axial temperature <span class="hlt">gradient</span> and mean flow" (J.Li and A.S.Morgans, Journal of Sound and Vibration 400 (2017) 248-269)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dokumaci, Erkan</p> <p>2017-12-01</p> <p>In a recent study, Li and Morgans [1] present an ingenious WKB approximation for the <span class="hlt">acoustic</span> plane wave field in a straight uniform duct with mean temperature <span class="hlt">gradient</span> and mean flow. The authors state that the previous solutions are limited to small linear mean temperature <span class="hlt">gradients</span> and low mean flow Mach numbers and claim that their solution applies for arbitrary mean temperature profiles and moderate-to-large mean flow velocity Mach numbers at both low and high frequencies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19740020268&hterms=influence+level&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DTitle%26N%3D0%26No%3D20%26Ntt%3Dthe%2Binfluence%2Blevel%2Bof','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19740020268&hterms=influence+level&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DTitle%26N%3D0%26No%3D20%26Ntt%3Dthe%2Binfluence%2Blevel%2Bof"><span>Load influence on gear noise. [mathematical model for determining <span class="hlt">acoustic</span> <span class="hlt">pressure</span> level as function of load</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Merticaru, V.</p> <p>1974-01-01</p> <p>An original mathematical model is proposed to derive equations for calculation of gear noise. These equations permit the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> level to be determined as a function of load. Application of this method to three parallel gears is reported. The logical calculation scheme is given, as well as the results obtained.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005ASAJ..118.2006M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005ASAJ..118.2006M"><span>Modulated <span class="hlt">acoustic</span> radiation <span class="hlt">pressure</span> and stress-coupling projections</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marston, Philip L.; Thiessen, David B.</p> <p>2005-09-01</p> <p>Low-frequency deformation can be induced at a single frequency using radiation stress oscillations of double-sideband suppressed-carrier ultrasound [P. L. Marston and R. E. Apfel, J. <span class="hlt">Acoust</span>. Soc. Am. 67, 27 (1980)]. The transducer voltage is proportional to a product of low- and high-frequency sine waves. To anticipate the shape and magnitude of induced deformations, it is helpful to expand the distribution of the radiation stress on the object to be deformed as a series of projections [P. L. Marston, J. <span class="hlt">Acoust</span>. Soc. Am. 67, 15 (1980)]. Stress projections are also useful for unmodulated waves: the radiation force is an example. In addition to spherical and nearly spherical objects, recent experiments and calculations have concerned cylindrical objects [S. F. Morse, D. B. Thiessen, and P. L. Marston, Phys. Fluids 8, 3 (1996); W. Wei, D. B. Thiessen, and P. L. Marston, J. <span class="hlt">Acoust</span>. Soc. Am. 116, 202 (2004)]. In standing waves the following projections are nonvanishing in the low <span class="hlt">acoustic</span> frequency limit for appropriately situated dense objects: radial projection [M. J. Marr-Lyon, D. B. Thiessen, and P. L. Marston, Phys. Rev. Lett. 86, 2293 (2001)] and quadrupole projection [P. L. Marston et al., J. <span class="hlt">Acoust</span>. Soc. Am. 69, 1499 (1981)].</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27457561','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27457561"><span>Repeatability of <span class="hlt">gradient</span> ultrahigh <span class="hlt">pressure</span> liquid chromatography-tandem mass spectrometry methods in instrument-controlled thermal environments.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Grinias, James P; Wong, Jenny-Marie T; Kennedy, Robert T</p> <p>2016-08-26</p> <p>The impact of viscous friction on eluent temperature and column efficiency in liquid chromatography is of renewed interest as the need for <span class="hlt">pressures</span> exceeding 1000bar to use with columns packed with sub-2μm particles has grown. One way the development of axial and radial temperature <span class="hlt">gradients</span> that arise due to viscous friction can be affected is by the thermal environment the column is placed in. In this study, a new column oven integrated into an ultrahigh <span class="hlt">pressure</span> liquid chromatograph that enables both still-air and forced-air operating modes is investigated to find the magnitude of the effect of the axial thermal <span class="hlt">gradient</span> that forms in 2.1×100mm columns packed with sub-2μm particles in these modes. Temperature increases of nearly 30K were observed when the generated power of the column exceeded 25W/m. The impact of the heating due to viscous friction on the repeatability of peak capacity, elution time, and peak area ratio to an internal standard for a <span class="hlt">gradient</span> UHPLC-MS/MS method to analyze neurotransmitters was found to be limited. This result indicates that high speed UHPLC-MS/MS <span class="hlt">gradient</span> methods under conditions of high viscous friction may be possible without the negative effects typically observed with isocratic separations under similar conditions. Copyright © 2016 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA114124','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA114124"><span>Properties of Materials Using <span class="hlt">Acoustic</span> Waves.</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1982-05-01</p> <p><span class="hlt">Acoust</span>. Soc. Am. 69, 1624 (1981). R.E. Apfel, "<span class="hlt">Acoustic</span> Cavitation : A Possible Consequence of Biomedical Uses of Ultrasound ," Brit. J. Cancer, in...efforts can be classified into four broad categories; - Applications of <span class="hlt">acoustic</span> levitation; nonlinear <span class="hlt">acoustics</span> and radiation <span class="hlt">pressure</span>; <span class="hlt">acoustic</span> cavitation ...supercooled water - a question of concern to cryobiologists. We have also measured the properties of several lipid oils (only available in less than</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16448061','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16448061"><span>Pseudolinear <span class="hlt">gradient</span> ultrahigh-<span class="hlt">pressure</span> liquid chromatography using an injection valve assembly.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Xiang, Yanqiao; Liu, Yansheng; Stearns, Stanley D; Plistil, Alex; Brisbin, Martin P; Lee, Milton L</p> <p>2006-02-01</p> <p>The use of ultrahigh <span class="hlt">pressures</span> in liquid chromatography (UHPLC) imposes stringent requirements on hardware such as pumps, valves, injectors, connecting tubing, and columns. One of the most difficult components of the UHPLC system to develop has been the sample injector. Static-split injection, which can be performed at <span class="hlt">pressures</span> up to 6900 bar (100,000 psi), consumes a large sample volume and is very irreproducible. A <span class="hlt">pressure</span>-balanced injection valve provided better reproducibility, shorter injection time, reduced sample consumption, and greater ease of use; however, it could only withstand <span class="hlt">pressures</span> up to approximately 1000 bar (15,000 psi). In this study, a new injection valve assembly that can operate at <span class="hlt">pressures</span> as high as 2070 bar (30,000 psi) was evaluated for UHPLC. This assembly contains six miniature electronically controlled needle valves to provide accurate and precise volumes for introduction into the capillary LC column. It was found that sample volumes as small as several tenths of a nanoliter can be injected, which are comparable to the results obtained from the static-split injector. The reproducibilities of retention time, efficiency, and peak area were investigated, and the results showed that the relative standard deviations of these parameters were small enough for quantitative analyses. Separation experiments using the UHPLC system with this new injection valve assembly showed that this new injector is suitable for both isocratic and <span class="hlt">gradient</span> operation modes. A newly designed capillary connector was used at a <span class="hlt">pressure</span> as high as 2070 bar (30,000 psi).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22039815-full-scale-hot-cell-test-acoustic-sensor-dedicated-measurement-internal-gas-pressure-composition-lwr-nuclear-fuel-rod','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22039815-full-scale-hot-cell-test-acoustic-sensor-dedicated-measurement-internal-gas-pressure-composition-lwr-nuclear-fuel-rod"><span>Full-scale hot cell test of an <span class="hlt">acoustic</span> sensor dedicated to measurement of the internal gas <span class="hlt">pressure</span> and composition of a LWR nuclear fuel rod</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>Ferrandis, J. Y.; Rosenkrantz, E.; Leveque, G.</p> <p>2011-07-01</p> <p>A full-scale hot cell test of the internal gas <span class="hlt">pressure</span> and composition measurement by an <span class="hlt">acoustic</span> sensor was carried on successfully between 2008 and 2010 on irradiated fuel rods in the LECA-STAR facility at Cadarache Centre. The <span class="hlt">acoustic</span> sensor has been specially designed in order to provide a nondestructive technique to easily carry out the measurement of the internal gas <span class="hlt">pressure</span> and gas composition of a LWR nuclear fuel rod. This sensor has been achieved in 2007 and is now covered by an international patent. The first positive result, concerning the device behaviour, is that the sensor-operating characteristics have notmore » been altered by a two-year exposure in the hot cell ambient. We performed the gas characterisation contained in irradiated fuel rods. The <span class="hlt">acoustic</span> method accuracy is now {+-}5 bars on the <span class="hlt">pressure</span> measurement result and {+-}0.3% on the evaluated gas composition. The results of the <span class="hlt">acoustic</span> method were compared to puncture results. Another significant conclusion is that the efficiency of the <span class="hlt">acoustic</span> method is not altered by the irradiation time, and possible modification of the cladding properties. These results make it possible to demonstrate the feasibility of the technique on irradiated fuel rods. The transducer and the associated methodology are now operational. (authors)« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930092247','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930092247"><span>Analysis and calculation by integral methods of laminar compressible boundary-layer with heat transfer and with and without <span class="hlt">pressure</span> <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Morduchow, Morris</p> <p>1955-01-01</p> <p>A survey of integral methods in laminar-boundary-layer analysis is first given. A simple and sufficiently accurate method for practical purposes of calculating the properties (including stability) of the laminar compressible boundary layer in an axial <span class="hlt">pressure</span> <span class="hlt">gradient</span> with heat transfer at the wall is presented. For flow over a flat plate, the method is applicable for an arbitrarily prescribed distribution of temperature along the surface and for any given constant Prandtl number close to unity. For flow in a <span class="hlt">pressure</span> <span class="hlt">gradient</span>, the method is based on a Prandtl number of unity and a uniform wall temperature. A simple and accurate method of determining the separation point in a compressible flow with an adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> over a surface at a given uniform wall temperature is developed. The analysis is based on an extension of the Karman-Pohlhausen method to the momentum and the thermal energy equations in conjunction with fourth- and especially higher degree velocity and stagnation-enthalpy profiles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120011839','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120011839"><span>Numerical Study of <span class="hlt">Pressure</span> Fluctuations due to High-Speed Turbulent Boundary Layers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Duan, Lian; Choudhari, Meelan M.; Wu, Minwei</p> <p>2012-01-01</p> <p>Direct numerical simulations (DNS) are used to examine the <span class="hlt">pressure</span> fluctuations generated by fully developed turbulence in supersonic turbulent boundary layers with an emphasis on both <span class="hlt">pressure</span> fluctuations at the wall and the <span class="hlt">acoustic</span> fluctuations radiated into the freestream. The wall and freestream <span class="hlt">pressure</span> fields are first analyzed for a zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> boundary layer with Mach 2.5 and Reynolds number based on momentum thickness of approximately 2835. The single and multi-point statistics reported include the wall <span class="hlt">pressure</span> fluctuation intensities, frequency spectra, space-time correlations, and convection velocities. Single and multi-point statistics of surface <span class="hlt">pressure</span> fluctuations show good agreement with measured data and previously published simulations of turbulent boundary layers under similar flow conditions. Spectral analysis shows that the <span class="hlt">acoustic</span> fluctuations outside the boundary layer region have much lower energy content within the high-frequency region. The space-time correlations reflect the convective nature of the <span class="hlt">pressure</span> field both at the wall and in the freestream, which is characterized by the downstream propagation of <span class="hlt">pressure</span>-carrying eddies. Relative to those at the wall, the <span class="hlt">pressure</span>-carrying eddies associated with the freestream signal are larger and convect at a significantly lower speed. The preliminary DNS results of a Mach 6 boundary layer show that the <span class="hlt">pressure</span> rms in the freestream region is significantly higher than that of the lower Mach number case.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930092249','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930092249"><span>Characteristics of turbulence in boundary layer with zero <span class="hlt">pressure</span> <span class="hlt">gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Klebanoff, P S</p> <p>1955-01-01</p> <p>The results of an experimental investigation of a turbulent boundary layer with zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> are presented. Measurements with the hot-wire anemometer were made of turbulent energy and turbulent shear stress, probability density and flattening factor of u-fluctuation (fluctuation in x-direction), spectra of turbulent energy and shear stress, and turbulent dissipation. The importance of the region near the wall and the inadequacy of the concept of local isotropy are demonstrated. Attention is given to the energy balance and the intermittent character of the outer region of the boundary layer. Also several interesting features of the spectral distribution of the turbulent motions are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ApPhL.108z3501Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ApPhL.108z3501Q"><span><span class="hlt">Acoustic</span> energy harvesting based on a planar <span class="hlt">acoustic</span> metamaterial</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Qi, Shuibao; Oudich, Mourad; Li, Yong; Assouar, Badreddine</p> <p>2016-06-01</p> <p>We theoretically report on an innovative and practical <span class="hlt">acoustic</span> energy harvester based on a defected <span class="hlt">acoustic</span> metamaterial (AMM) with piezoelectric material. The idea is to create suitable resonant defects in an AMM to confine the strain energy originating from an <span class="hlt">acoustic</span> incidence. This scavenged energy is converted into electrical energy by attaching a structured piezoelectric material into the defect area of the AMM. We show an <span class="hlt">acoustic</span> energy harvester based on a meta-structure capable of producing electrical power from an <span class="hlt">acoustic</span> <span class="hlt">pressure</span>. Numerical simulations are provided to analyze and elucidate the principles and the performances of the proposed system. A maximum output voltage of 1.3 V and a power density of 0.54 μW/cm3 are obtained at a frequency of 2257.5 Hz. The proposed concept should have broad applications on energy harvesting as well as on low-frequency sound isolation, since this system acts as both <span class="hlt">acoustic</span> insulator and energy harvester.</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/2017JPhD...50P5104T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhD...50P5104T"><span>Beam aperture modifier design with <span class="hlt">acoustic</span> metasurfaces</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tang, Weipeng; Ren, Chunyu</p> <p>2017-10-01</p> <p>In this paper, we present a design concept of <span class="hlt">acoustic</span> beam aperture modifier using two metasurface-based planar lenses. By appropriately designing the phase <span class="hlt">gradient</span> profile along the metasurface, we obtain a class of <span class="hlt">acoustic</span> convex lenses and concave lenses, which can focus the incoming plane waves and collimate the converging waves, respectively. On the basis of the high converging and diverging capability of these lenses, two kinds of lens combination scheme, including the convex-concave type and convex-convex type, are proposed to tune up the incoming beam aperture as needed. To be specific, the aperture of the <span class="hlt">acoustic</span> beam can be shrunk or expanded through adjusting the phase <span class="hlt">gradient</span> of the pair of lenses and the spacing between them. These lenses and the corresponding aperture modifiers are constructed by the stacking ultrathin labyrinthine structures, which are obtained by the geometry optimization procedure and exhibit high transmission coefficient and a full range of phase shift. The simulation results demonstrate the effectiveness of our proposed beam aperture modifiers. Due to the flexibility in aperture controlling and the simplicity in fabrication, the proposed modifiers have promising potential in applications, such as <span class="hlt">acoustic</span> imaging, nondestructive evaluation, and communication.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19970000447','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19970000447"><span>Nonlinear Bubble Interactions in <span class="hlt">Acoustic</span> <span class="hlt">Pressure</span> Fields</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Barbat, Tiberiu; Ashgriz, Nasser; Liu, Ching-Shi</p> <p>1996-01-01</p> <p>The systems consisting of a two-phase mixture, as clouds of bubbles or drops, have shown many common features in their responses to different external force fields. One of particular interest is the effect of an unsteady <span class="hlt">pressure</span> field applied to these systems, case in which the coupling of the vibrations induced in two neighboring components (two drops or two bubbles) may result in an interaction force between them. This behavior was explained by Bjerknes by postulating that every body that is moving in an accelerating fluid is subjected to a 'kinetic buoyancy' equal with the product of the acceleration of the fluid multiplied by the mass of the fluid displaced by the body. The external sound wave applied to a system of drops/bubbles triggers secondary sound waves from each component of the system. These secondary <span class="hlt">pressure</span> fields integrated over the surface of the neighboring drop/bubble may result in a force additional to the effect of the primary sound wave on each component of the system. In certain conditions, the magnitude of these secondary forces may result in significant changes in the dynamics of each component, thus in the behavior of the entire system. In a system containing bubbles, the sound wave radiated by one bubble at the location of a neighboring one is dominated by the volume oscillation mode and its effects can be important for a large range of frequencies. The interaction forces in a system consisting of drops are much smaller than those consisting of bubbles. Therefore, as a first step towards the understanding of the drop-drop interaction subject to external <span class="hlt">pressure</span> fluctuations, it is more convenient to study the bubble interactions. This paper presents experimental results and theoretical predictions concerning the interaction and the motion of two levitated air bubbles in water in the presence of an <span class="hlt">acoustic</span> field at high frequencies (22-23 KHz).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18939477','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18939477"><span>[An improved case of bedridden mental impairment with normal <span class="hlt">pressure</span> hydrocephalus associated with <span class="hlt">acoustic</span> neurinoma after tumor resection].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sugimoto, Seiichiro; Sugimoto, Akiko; Saita, Kazuko; Kishi, Masahiko; Shioya, Keiichi; Higa, Toshinobu</p> <p>2008-08-01</p> <p>A 67-year-old woman developed gait disturbance, dysarthria, cognitive impairment and incontinence at age 65, and became bedridden. She showed mutism, stupor and lower limb spasticity. Cranial CT and MRI revealed marked ventricular enlargement and a cerebellopontine angle tumor. CSF study showed normal <span class="hlt">pressure</span> (125 mmH2O) and elevated protein (143 mg/dl). Radionuclide cisternography showed redistribution of radionuclide to the ventricles and intraventricular residual radionuclide after 72 hours, which allowed a diagnosis of normal <span class="hlt">pressure</span> hydrocephalus. After removal of the tumor, ventricle size and CSF protein decreased, and the symptoms of cognitive impairment and motor dysfunction resolved. Histological examination showed <span class="hlt">acoustic</span> neurinoma. Over the half of hydrocephalus following <span class="hlt">acoustic</span> neurinoma shows a tendency to improve by surgical resection of the tumor. Neurologists who see cognitively impaired spastic bedridden patients should not overlook this pathology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5436981','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5436981"><span><span class="hlt">Acoustic</span> force measurements on polymer-coated microbubbles in a microfluidic device</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Memoli, Gianluca; Fury, Christopher R.; Baxter, Kate O.; Gélat, Pierre N.; Jones, Philip H.</p> <p>2017-01-01</p> <p>This work presents an acoustofluidic device for manipulating coated microbubbles, designed for the simultaneous use of optical and <span class="hlt">acoustical</span> tweezers. A comprehensive characterization of the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> in the device is presented, obtained by the synergic use of different techniques in the range of <span class="hlt">acoustic</span> frequencies where visual observations showed aggregation of polymer-coated microbubbles. In absence of bubbles, the combined use of laser vibrometry and finite element modelling supported a non-invasive measurement of the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> and an enhanced understanding of the system resonances. Calibrated holographic optical tweezers were used for direct measurements of the <span class="hlt">acoustic</span> forces acting on an isolated microbubble, at low driving <span class="hlt">pressures</span>, and to confirm the spatial distribution of the <span class="hlt">acoustic</span> field. This allowed quantitative <span class="hlt">acoustic</span> <span class="hlt">pressure</span> measurements by particle tracking, using polystyrene beads, and an evaluation of the related uncertainties. This process facilitated the extension of tracking to microbubbles, which have a negative acoustophoretic contrast factor, allowing <span class="hlt">acoustic</span> force measurements on bubbles at higher <span class="hlt">pressures</span> than optical tweezers, highlighting four peaks in the <span class="hlt">acoustic</span> response of the device. Results and methodologies are relevant to acoustofluidic applications requiring a precise characterization of the <span class="hlt">acoustic</span> field and, in general, to biomedical applications with microbubbles or deformable particles. PMID:28599556</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12695886','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12695886"><span>Relationship between magnetic field strength and magnetic-resonance-related <span class="hlt">acoustic</span> noise levels.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Moelker, Adriaan; Wielopolski, Piotr A; Pattynama, Peter M T</p> <p>2003-02-01</p> <p>The need for better signal-to-noise ratios and resolution has pushed magnetic resonance imaging (MRI) towards high-field MR-scanners for which only little data on MR-related <span class="hlt">acoustic</span> noise production have been published. The purpose of this study was to validate the theoretical relationship of sound <span class="hlt">pressure</span> level (SPL) and static magnetic field strength. This is relevant for allowing adequate comparisons of <span class="hlt">acoustic</span> data of MR systems at various magnetic field strengths. <span class="hlt">Acoustic</span> data were acquired during various pulse sequences at field strengths of 0.5, 1.0, 1.5 and 2.0 Tesla using the same MRI unit by means of a Helicon rampable magnet. Continuous-equivalent, i.e. time-averaged, linear SPLs and 1/3-octave band frequencies were recorded. Ramping from 0.5 to 1.0 Tesla and from 1.0 to 2.0 Tesla resulted in an SPL increase of 5.7 and 5.2 dB(L), respectively, when averaged over the various pulse sequences. Most of the <span class="hlt">acoustic</span> energy was in the 1-kHz frequency band, irrespective of magnetic field strength. The relation between field strength and SPL was slightly non-linear, i.e. a slightly less increase at higher field strengths, presumably caused by the elastic properties of the <span class="hlt">gradient</span> coil encasings.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920011167','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920011167"><span><span class="hlt">Acoustic</span> forcing of a liquid drop</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lyell, M. J.</p> <p>1992-01-01</p> <p>The development of systems such as <span class="hlt">acoustic</span> levitation chambers will allow for the positioning and manipulation of material samples (drops) in a microgravity environment. This provides the capability for fundamental studies in droplet dynamics as well as containerless processing work. Such systems use <span class="hlt">acoustic</span> radiation <span class="hlt">pressure</span> forces to position or to further manipulate (e.g., oscillate) the sample. The primary objective was to determine the effect of a viscous <span class="hlt">acoustic</span> field/tangential radiation <span class="hlt">pressure</span> forcing on drop oscillations. To this end, the viscous <span class="hlt">acoustic</span> field is determined. Modified (forced) hydrodynamic field equations which result from a consistent perturbation expansion scheme are solved. This is done in the separate cases of an unmodulated and a modulated <span class="hlt">acoustic</span> field. The effect of the tangential radiation stress on the hydrodynamic field (drop oscillations) is found to manifest as a correction to the velocity field in a sublayer region near the drop/host interface. Moreover, the forcing due to the radiation <span class="hlt">pressure</span> vector at the interface is modified by inclusion of tangential stresses.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011SPIE.8047E..0CD','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011SPIE.8047E..0CD"><span>The <span class="hlt">acoustic</span> vector sensor: a versatile battlefield <span class="hlt">acoustics</span> sensor</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de Bree, Hans-Elias; Wind, Jelmer W.</p> <p>2011-06-01</p> <p>The invention of the Microflown sensor has made it possible to measure <span class="hlt">acoustic</span> particle velocity directly. An <span class="hlt">acoustic</span> vector sensor (AVS) measures the particle velocity in three directions (the source direction) and the <span class="hlt">pressure</span>. The sensor is a uniquely versatile battlefield sensor because its size is a few millimeters and it is sensitive to sound from 10Hz to 10kHz. This article shows field tests results of <span class="hlt">acoustic</span> vector sensors, measuring rifles, heavy artillery, fixed wing aircraft and helicopters. Experimental data shows that the sensor is suitable as a ground sensor, mounted on a vehicle and on a UAV.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PSST...27c5008Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PSST...27c5008Y"><span>Magnetical asymmetry effect in capacitively coupled plasmas: effects of the magnetic field <span class="hlt">gradient</span>, <span class="hlt">pressure</span>, and gap length</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Shali; Chang, Lijie; Zhang, Ya; Jiang, Wei</p> <p>2018-03-01</p> <p>By applying the asymmetric magnetic field to a discharge, the dc self-bias and asymmetric plasma response can be generated even in a geometrically and electrically symmetric system. This is called magnetical asymmetric effect (MAE), which can be a new method to control the ion energy and flux independently (Yang et al 2017 Plasma Process. Polym. 14 1700087). In the present work, the effects of magnetic field <span class="hlt">gradient</span>, gas <span class="hlt">pressure</span> and gap length on MAE are investigated by using a one-dimensional implicit particle-in-cell/Monte Carlo collision simulation. It found that by appropriately increasing the magnetic field <span class="hlt">gradient</span> and the gap length, the range of the self-bias voltage will be enlarged, which can be used as the effective approach to control the ion bombarding energy at the electrodes since the ion energy is determined by the voltage drop across the sheath. It also found that the ion flux asymmetry will disappear at high <span class="hlt">pressure</span> when the magnetic field <span class="hlt">gradient</span> is relative low, due to the frequent electron-neutral collisions can disrupt electron gyromotion and thus the MAE is greatly reduced.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28452741','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28452741"><span><span class="hlt">Pressure</span> dependence of transverse <span class="hlt">acoustic</span> phonon energy in ferropericlase across the spin transition.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fukui, Hiroshi; Baron, Alfred Q R; Ishikawa, Daisuke; Uchiyama, Hiroshi; Ohishi, Yasuo; Tsuchiya, Taku; Kobayashi, Hisao; Matsuzaki, Takuya; Yoshino, Takashi; Katsura, Tomoo</p> <p>2017-06-21</p> <p>We investigated transverse <span class="hlt">acoustic</span> (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 <span class="hlt">pressure</span> above the spin transition <span class="hlt">pressure</span> 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 <span class="hlt">pressure</span>; 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.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850013795','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850013795"><span>High temperature <span class="hlt">acoustic</span> levitator</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Barmatz, M. B. (Inventor)</p> <p>1984-01-01</p> <p>A system is described for <span class="hlt">acoustically</span> levitating an object within a portion of a chamber that is heated to a high temperature, while a driver at the opposite end of the chamber is maintained at a relatively low temperature. The cold end of the chamber is constructed so it can be telescoped to vary the length (L sub 1) of the cold end portion and therefore of the entire chamber, so that the chamber remains resonant to a normal mode frequency, and so that the <span class="hlt">pressure</span> at the hot end of the chamber is maximized. The precise length of the chamber at any given time, is maintained at an optimum resonant length by a feedback loop. The feedback loop includes an <span class="hlt">acoustic</span> <span class="hlt">pressure</span> sensor at the hot end of the chamber, which delivers its output to a control circuit which controls a motor that varies the length (L) of the chamber to a level where the sensed <span class="hlt">acoustic</span> <span class="hlt">pressure</span> is a maximum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130000589','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130000589"><span>Verification of Ares I Liftoff <span class="hlt">Acoustic</span> Environments via the Ares I Scale Model <span class="hlt">Acoustic</span> Test</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Counter, Douglas; Houston, Janice</p> <p>2012-01-01</p> <p>The Ares I Scale Model <span class="hlt">Acoustic</span> Test (ASMAT) program was implemented to verify the predicted Ares I liftoff <span class="hlt">acoustic</span> environments and to determine the <span class="hlt">acoustic</span> reduction gained by using an above deck water sound suppression system. The test article included a 5% scale Ares I vehicle model and Mobile Launcher with tower. <span class="hlt">Acoustic</span> and <span class="hlt">pressure</span> data were measured by over 200 instruments. The ASMAT results are compared to Ares I-X flight data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040112441&hterms=adrenergic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dadrenergic','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040112441&hterms=adrenergic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dadrenergic"><span>Estimation of diastolic intraventricular <span class="hlt">pressure</span> <span class="hlt">gradients</span> by Doppler M-mode echocardiography</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Greenberg, N. L.; Vandervoort, P. M.; Firstenberg, M. S.; Garcia, M. J.; Thomas, J. D.</p> <p>2001-01-01</p> <p>Previous studies have shown that small intraventricular <span class="hlt">pressure</span> <span class="hlt">gradients</span> (IVPG) are important for efficient filling of the left ventricle (LV) and as a sensitive marker for ischemia. Unfortunately, there has previously been no way of measuring these noninvasively, severely limiting their research and clinical utility. Color Doppler M-mode (CMM) echocardiography provides a spatiotemporal velocity distribution along the inflow tract throughout diastole, which we hypothesized would allow direct estimation of IVPG by using the Euler equation. Digital CMM images, obtained simultaneously with intracardiac <span class="hlt">pressure</span> waveforms in six dogs, were processed by numerical differentiation for the Euler equation, then integrated to estimate IVPG and the total (left atrial to left ventricular apex) <span class="hlt">pressure</span> drop. CMM-derived estimates agreed well with invasive measurements (IVPG: y = 0.87x + 0.22, r = 0.96, P < 0.001, standard error of the estimate = 0.35 mmHg). Quantitative processing of CMM data allows accurate estimation of IVPG and tracking of changes induced by beta-adrenergic stimulation. This novel approach provides unique information on LV filling dynamics in an entirely noninvasive way that has previously not been available for assessment of diastolic filling and function.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950029369&hterms=Streaming+Media&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DStreaming%2BMedia','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950029369&hterms=Streaming+Media&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DStreaming%2BMedia"><span><span class="hlt">Acoustic</span> instability driven by cosmic-ray streaming</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Begelman, Mitchell C.; Zweibel, Ellen G.</p> <p>1994-01-01</p> <p>We study the linear stability of compressional waves in a medium through which cosmic rays stream at the Alfven speed due to strong coupling with Alfven waves. <span class="hlt">Acoustic</span> waves can be driven unstable by the cosmic-ray drift, provided that the streaming speed is sufficiently large compared to the thermal sound speed. Two effects can cause instability: (1) the heating of the thermal gas due to the damping of Alfven waves driven unstable by cosmic-ray streaming; and (2) phase shifts in the cosmic-ray <span class="hlt">pressure</span> perturbation caused by the combination of cosmic-ray streaming and diffusion. The instability does not depend on the magnitude of the background cosmic-ray <span class="hlt">pressure</span> <span class="hlt">gradient</span>, and occurs whether or not cosmic-ray diffusion is important relative to streaming. When the cosmic-ray <span class="hlt">pressure</span> is small compared to the gas <span class="hlt">pressure</span>, or cosmic-ray diffusion is strong, the instability manifests itself as a weak overstability of slow magnetosonic waves. Larger cosmic-ray <span class="hlt">pressure</span> gives rise to new hybrid modes, which can be strongly unstable in the limits of both weak and strong cosmic-ray diffusion and in the presence of thermal conduction. Parts of our analysis parallel earlier work by McKenzie & Webb (which were brought to our attention after this paper was accepted for publication), but our treatment of diffusive effects, thermal conduction, and nonlinearities represent significant extensions. Although the linear growth rate of instability is independent of the background cosmic-ray <span class="hlt">pressure</span> <span class="hlt">gradient</span>, the onset of nonlinear eff ects does depend on absolute value of DEL (vector differential operator) P(sub c). At the onset of nonlinearity the fractional amplitude of cosmic-ray <span class="hlt">pressure</span> perturbations is delta P(sub C)/P(sub C) approximately (kL) (exp -1) much less than 1, where k is the wavenumber and L is the <span class="hlt">pressure</span> scale height of the unperturbed cosmic rays. We speculate that the instability may lead to a mode of cosmic-ray transport in which plateaus of uniform cosmic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1985asme.confU....M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1985asme.confU....M"><span>The influence of the radial <span class="hlt">pressure</span> <span class="hlt">gradient</span> on the blade root loss in an annular subsonic nozzle cascade</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Meng, D.; Weng, Z.; Xiang, Y.</p> <p>1985-09-01</p> <p>This paper presents a method for predicting the blade root loss in an annular nozzle cascade in which consideration is given to the influence of the radial <span class="hlt">pressure</span> <span class="hlt">gradient</span> (RPG) on it. The variation of blade root losses under different RPG is obtained experimentally, and finite element method is used to calculate the <span class="hlt">pressure</span> distribution in the blade passage.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22486150-broadband-manipulation-acoustic-wavefronts-pentamode-metasurface','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22486150-broadband-manipulation-acoustic-wavefronts-pentamode-metasurface"><span>Broadband manipulation of <span class="hlt">acoustic</span> wavefronts by pentamode metasurface</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>Tian, Ye; Wei, Qi, E-mail: weiqi@nju.edu.cn; Cheng, Ying</p> <p>2015-11-30</p> <p>An <span class="hlt">acoustic</span> metasurface with a sub-wavelength thickness can manipulate <span class="hlt">acoustic</span> wavefronts freely by the introduction of abrupt phase variation. However, the existence of a narrow bandwidth and a low transmittance limits further applications. Here, we present a broadband and highly transparent <span class="hlt">acoustic</span> metasurface based on a frequency-independent generalized <span class="hlt">acoustic</span> Snell's law and pentamode metamaterials. The proposal employs a <span class="hlt">gradient</span> velocity to redirect refracted waves and pentamode metamaterials to improve impedance matching between the metasurface and the background medium. Excellent wavefront manipulation based on the metasurface is further demonstrated by anomalous refraction, generation of non-diffracting Bessel beam, and sub-wavelength flat focusing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006ApPhL..89u4102X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006ApPhL..89u4102X"><span><span class="hlt">Acoustic</span> method for levitation of small living animals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xie, W. J.; Cao, C. D.; Lü, Y. J.; Hong, Z. Y.; Wei, B.</p> <p>2006-11-01</p> <p>Ultrasonic levitation of some small living animals such as ant, ladybug, and young fish has been achieved with a single-axis <span class="hlt">acoustic</span> levitator. The vitality of ant and ladybug is not evidently influenced during the <span class="hlt">acoustic</span> levitation, whereas that of the young fish is reduced because of the inadequacy of water supply. Numerical analysis shows that the sound <span class="hlt">pressures</span> on the ladybug's surface almost reach the incident <span class="hlt">pressure</span> amplitude p0 due to sound scattering. It is estimated that 99.98% of the <span class="hlt">acoustic</span> energy is reflected away from the ladybug. The <span class="hlt">acoustic</span> radiation <span class="hlt">pressure</span> pa on the ladybug's surface is only 1%-3% of p0, which plays a compression role on the central region and a suction role on the peripheral region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1014872','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1014872"><span><span class="hlt">Acoustic</span> concentration of particles in fluid flow</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Ward, Michael D.; Kaduchak, Gregory</p> <p>2010-11-23</p> <p>An apparatus for <span class="hlt">acoustic</span> concentration of particles in a fluid flow includes a substantially <span class="hlt">acoustically</span> transparent membrane and a vibration generator that define a fluid flow path therebetween. The fluid flow path is in fluid communication with a fluid source and a fluid outlet and the vibration generator is disposed adjacent the fluid flow path and is capable of producing an <span class="hlt">acoustic</span> field in the fluid flow path. The <span class="hlt">acoustic</span> field produces at least one <span class="hlt">pressure</span> minima in the fluid flow path at a predetermined location within the fluid flow path and forces predetermined particles in the fluid flow path to the at least one <span class="hlt">pressure</span> minima.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010018435','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010018435"><span>Measurement of the Turbulence Kinetic Energy Budget of a Turbulent Planar Wake Flow in <span class="hlt">Pressure</span> <span class="hlt">Gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Liu, Xiao-Feng; Thomas, Flint O.; Nelson, Robert C.</p> <p>2001-01-01</p> <p>Turbulence kinetic energy (TKE) is a very important quantity for turbulence modeling and the budget of this quantity in its transport equation can provide insight into the flow physics. Turbulence kinetic energy budget measurements were conducted for a symmetric turbulent wake flow subjected to constant zero, favorable and adverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> in year-three of research effort. The purpose of this study is to clarify the flow physics issues underlying the demonstrated influence of <span class="hlt">pressure</span> <span class="hlt">gradient</span> on wake development and provide experimental support for turbulence modeling. To ensure the reliability of these notoriously difficult measurements, the experimental procedure was carefully designed on the basis of an uncertainty analysis. Four different approaches, based on an isotropic turbulence assumption, a locally axisymmetric homogeneous turbulence assumption, a semi-isotropy assumption and a forced balance of the TKE equation, were applied for the estimate of the dissipation term. The <span class="hlt">pressure</span> transport term is obtained from a forced balance of the turbulence kinetic energy equation. This report will present the results of the turbulence kinetic energy budget measurement and discuss their implication on the development of strained turbulent wakes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19750006922','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19750006922"><span>An experimental investigation of heat transfer to reusable surface insulation tile array gaps in a turbulent boundary layer with <span class="hlt">pressure</span> <span class="hlt">gradient</span>. M.S. Thesis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Throckmorton, D. A.</p> <p>1975-01-01</p> <p>An experimental investigation was performed to determine the effect of <span class="hlt">pressure</span> <span class="hlt">gradient</span> on the heat transfer to space shuttle reusable surface insulation (RSI) tile array gaps under thick, turbulent boundary layer conditions. Heat transfer and <span class="hlt">pressure</span> measurements were obtained on a curved array of full-scale simulated RSI tiles in a tunnel wall boundary layer at a nominal freestream Mach number of 10.3 and freestream unit Reynolds numbers of 1.6, 3.3, and and 6.1 million per meter. Transverse <span class="hlt">pressure</span> <span class="hlt">gradients</span> were induced over the model surface by rotating the curved array with respect to the flow. Definition of the tunnel wall boundary layer flow was obtained by measurement of boundary layer pitot <span class="hlt">pressure</span> profiles, and flat plate wall <span class="hlt">pressure</span> and heat transfer. Flat plate wall heat transfer data were correlated and a method was derived for prediction of smooth, curved array heat transfer in the highly three-dimensional tunnel wall boundary layer flow and simulation of full-scale space shuttle vehicle <span class="hlt">pressure</span> <span class="hlt">gradient</span> levels was assessed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19720007523','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19720007523"><span>Calculation of turbulent boundary layers with heat transfer and <span class="hlt">pressure</span> <span class="hlt">gradient</span> utilizing a compressibility transformation. Part 3: Computer program manual</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schneider, J.; Boccio, J.</p> <p>1972-01-01</p> <p>A computer program is described capable of determining the properties of a compressible turbulent boundary layer with <span class="hlt">pressure</span> <span class="hlt">gradient</span> and heat transfer. The program treats the two-dimensional problem assuming perfect gas and Crocco integral energy solution. A compressibility transformation is applied to the equation for the conservation of mass and momentum, which relates this flow to a low speed constant property flow with simultaneous mass transfer and <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The resulting system of describing equations consists of eight ordinary differential equations which are solved numerically. For Part 1, see N72-12226; for Part 2, see N72-15264.</p> </li> </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/2017AGUFMOS51A1148G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMOS51A1148G"><span>Resolving the Role of the Dynamic <span class="hlt">Pressure</span> in the Burial, Exposure, Scour, and Mobility of Underwater Munitions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gilooly, S.; Foster, D. L.</p> <p>2017-12-01</p> <p>In nearshore environments, the motion of munitions results from a mixture of sediment transport conditions including sheet flow, scour, bedform migration, and momentary liquefaction. Incipient motion can be caused by disruptive shear stresses and <span class="hlt">pressure</span> <span class="hlt">gradients</span>. Foster et al. (2006) incorporated both processes into a single parameter, indicating incipient motion as a function of the bed state. This research looks to evaluate the role of the <span class="hlt">pressure</span> <span class="hlt">gradient</span> in positional state changes such as burial, exposure, and mobility. In the case of munitions, this may include <span class="hlt">pressure</span> <span class="hlt">gradients</span> induced by vortex shedding or the passing wave. <span class="hlt">Pressure</span>-mapped model munitions are being developed to measure the orientation, rotation, and surface <span class="hlt">pressure</span> of the munitions during threshold events leading to a new positional state. These munitions will be deployed in inner surf zone and estuary environments along with <span class="hlt">acoustic</span> Doppler velocimeters (ADVs), pore water <span class="hlt">pressure</span> sensors, a laser grid, and a pencil beam sonar with an azimuth drive. The additional instruments allow for near bed and far field water column and sediment bed sampling. Currently preliminary assessments of various <span class="hlt">pressure</span> sensors and munition designs are underway. Two <span class="hlt">pressure</span> sensors were selected; the thin FlexiForce A201 sensors will be used to indicate munition rolling during threshold events and diaphragm sensors will be used to understand changes in surrounding pore water <span class="hlt">pressure</span> as the munition begins to bury/unbury. Both sensors are expected to give quantitative measurements of dynamic <span class="hlt">pressure</span> <span class="hlt">gradients</span> in the flow field surrounding the munition. Resolving the role of this process will give insight to an improved incipient motion parameter and allow for better munition motion predictions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790024039','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790024039"><span><span class="hlt">Acoustic</span> analysis of the propfan</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Farassat, F.; Succi, G. P.</p> <p>1979-01-01</p> <p>A review of propeller noise prediction technology is presented. Two methods for the prediction of the noise from conventional and advanced propellers in forward flight are described. These methods are based on different time domain formulations. Brief descriptions of the computer algorithms based on these formulations are given. The output of the programs (the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> signature) was Fourier analyzed to get the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> spectrum. The main difference between the two programs is that one can handle propellers with supersonic tip speed while the other is for subsonic tip speed propellers. Comparisons of the calculated and measured <span class="hlt">acoustic</span> data for a conventional and an advanced propeller show good agreement in general.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JAP...120h5106S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JAP...120h5106S"><span>Waveform-preserved unidirectional <span class="hlt">acoustic</span> transmission based on impedance-matched <span class="hlt">acoustic</span> metasurface and phononic crystal</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Song, Ai-Ling; Chen, Tian-Ning; Wang, Xiao-Peng; Wan, Le-Le</p> <p>2016-08-01</p> <p>The waveform distortion happens in most of the unidirectional <span class="hlt">acoustic</span> transmission (UAT) devices proposed before. In this paper, a novel type of waveform-preserved UAT device composed of an impedance-matched <span class="hlt">acoustic</span> metasurface (AMS) and a phononic crystal (PC) structure is proposed and numerically investigated. The <span class="hlt">acoustic</span> <span class="hlt">pressure</span> field distributions and transmittance are calculated by using the finite element method. The subwavelength AMS that can modulate the wavefront of the transmitted wave at will is designed and the band structure of the PC structure is calculated and analyzed. The sound <span class="hlt">pressure</span> field distributions demonstrate that the unidirectional <span class="hlt">acoustic</span> transmission can be realized by the proposed UAT device without changing the waveforms of the output waves, which is the distinctive feature compared with the previous UAT devices. The physical mechanism of the unidirectional <span class="hlt">acoustic</span> transmission is discussed by analyzing the refraction angle changes and partial band gap map. The calculated transmission spectra show that the UAT device is valid within a relatively broad frequency range. The simulation results agree well with the theoretical predictions. The proposed UAT device provides a good reference for designing waveform-preserved UAT devices and has potential applications in many fields, such as medical ultrasound, <span class="hlt">acoustic</span> rectifiers, and noise insulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19820031072&hterms=refraction&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Drefraction','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19820031072&hterms=refraction&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Drefraction"><span>Radio jet refraction in galactic atmospheres with static <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Henriksen, R. N.; Vallee, J. P.; Bridle, A. H.</p> <p>1981-01-01</p> <p>A theory based on the refraction of radio jets in the extended atmosphere of an elliptical galaxy, is proposed for double radio sources with a Z or S morphology. The model describes a collimated jet of supersonic material that bends self-consistently under the influence of external static <span class="hlt">pressure</span> <span class="hlt">gradients</span>, and may alternatively be seen as a continuous-jet version of the buoyancy model proposed by Gull (1973). Emphasis is placed on (1) S-shaped radio sources identified with isolated galaxies, such as 3C 293, whose radio structures should be free of distortions resulting from motion relative to a cluster medium, and (2) small-scale, galaxy-dominated rather than environment-dominated S-shaped sources such as the inner jet structure of Fornax A.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25324056','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25324056"><span>Experimental study of the oscillation of spheres in an <span class="hlt">acoustic</span> levitator.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Andrade, Marco A B; Pérez, Nicolás; Adamowski, Julio C</p> <p>2014-10-01</p> <p>The spontaneous oscillation of solid spheres in a single-axis <span class="hlt">acoustic</span> levitator is experimentally investigated by using a high speed camera to record the position of the levitated sphere as a function of time. The oscillations in the axial and radial directions are systematically studied by changing the sphere density and the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> amplitude. In order to interpret the experimental results, a simple model based on a spring-mass system is applied in the analysis of the sphere oscillatory behavior. This model requires the knowledge of the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> distribution, which was obtained numerically by using a linear finite element method (FEM). Additionally, the linear <span class="hlt">acoustic</span> <span class="hlt">pressure</span> distribution obtained by FEM was compared with that measured with a laser Doppler vibrometer. The comparison between numerical and experimental <span class="hlt">pressure</span> distributions shows good agreement for low values of <span class="hlt">pressure</span> amplitude. When the <span class="hlt">pressure</span> amplitude is increased, the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> distribution becomes nonlinear, producing harmonics of the fundamental frequency. The experimental results of the spheres oscillations for low <span class="hlt">pressure</span> amplitudes are consistent with the results predicted by the simple model based on a spring-mass system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170003412','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170003412"><span><span class="hlt">Acoustic</span> Effects in Classical Nucleation Theory</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Baird, J. K.; Su, C.-H.</p> <p>2017-01-01</p> <p>The effect of sound wave oscillations on the rate of nucleation in a parent phase can be calculated by expanding the free energy of formation of a nucleus of the second phase in powers of the <span class="hlt">acoustic</span> <span class="hlt">pressure</span>. Since the period of sound wave oscillation is much shorter than the time scale for nucleation, the <span class="hlt">acoustic</span> effect can be calculated as a time average of the free energy of formation of the nucleus. The leading non-zero term in the time average of the free energy is proportional to the square of the <span class="hlt">acoustic</span> <span class="hlt">pressure</span>. The Young-Laplace equation for the surface tension of the nucleus can be used to link the time average of the square of the <span class="hlt">pressure</span> in the parent phase to its time average in the nucleus of the second phase. Due to the surface tension, the <span class="hlt">pressure</span> in the nuclear phase is higher than the <span class="hlt">pressure</span> in the parent phase. The effect is to lower the free energy of formation of the nucleus and increase the rate of nucleation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1375222','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1375222"><span><span class="hlt">Acoustic</span> concentration of particles in fluid flow</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>Ward, Michael W.; Kaduchak, Gregory</p> <p></p> <p>Disclosed herein is a <span class="hlt">acoustic</span> concentration of particles in a fluid flow that includes a substantially <span class="hlt">acoustically</span> transparent membrane and a vibration generator that define a fluid flow path therebetween. The fluid flow path is in fluid communication with a fluid source and a fluid outlet and the vibration generator is disposed adjacent the fluid flow path and is capable of producing an <span class="hlt">acoustic</span> field in the fluid flow path. The <span class="hlt">acoustic</span> field produces at least one <span class="hlt">pressure</span> minima in the fluid flow path at a predetermined location within the fluid flow path and forces predetermined particles in the fluidmore » flow path to the at least one <span class="hlt">pressure</span> minima.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004ASAJ..115R2371K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004ASAJ..115R2371K"><span>Relationships between objective <span class="hlt">acoustic</span> indices and <span class="hlt">acoustic</span> comfort evaluation in nonacoustic spaces</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kang, Jian</p> <p>2004-05-01</p> <p>Much attention has been paid to <span class="hlt">acoustic</span> spaces such as concert halls and recording studios, whereas research on nonacoustic buildings/spaces has been rather limited, especially from the viewpoint of <span class="hlt">acoustic</span> comfort. In this research a series of case studies has been carried out on this topic, considering various spaces including shopping mall atrium spaces, library reading rooms, football stadia, swimming spaces, churches, dining spaces, as well as urban open public spaces. The studies focus on the relationships between objective <span class="hlt">acoustic</span> indices such as sound <span class="hlt">pressure</span> level and reverberation time and perceptions of <span class="hlt">acoustic</span> comfort. The results show that the <span class="hlt">acoustic</span> atmosphere is an important consideration in such spaces and the evaluation of <span class="hlt">acoustic</span> comfort may vary considerably even if the objective <span class="hlt">acoustic</span> indices are the same. It is suggested that current guidelines and technical regulations are insufficient in terms of <span class="hlt">acoustic</span> design of these spaces, and the relationships established from the case studies between objective and subjective aspects would be useful for developing further design guidelines. [Work supported partly by the British Academy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15518624','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15518624"><span>Development of exercise-induced arm-leg blood <span class="hlt">pressure</span> <span class="hlt">gradient</span> and abnormal arterial compliance in patients with repaired coarctation of the aorta.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Markham, Larry W; Knecht, Sandra K; Daniels, Stephen R; Mays, Wayne A; Khoury, Philip R; Knilans, Timothy K</p> <p>2004-11-01</p> <p>Often, the lack of systemic arterial hypertension and the lack of a resting arm-leg blood <span class="hlt">pressure</span> <span class="hlt">gradient</span> are used to assess the adequacy of the anatomic result after intervention for coarctation of the aorta (CoA). Some patients with no arm-leg <span class="hlt">gradient</span> at rest may develop a <span class="hlt">gradient</span> with exercise, leading caregivers to question the success of the repair. It is not clear what the prevalence is of patients who have undergone a successful intervention for CoA and have no arm-leg <span class="hlt">gradient</span> at rest but develop a significant <span class="hlt">gradient</span> with exercise and which factors may predict the development of an arm-leg <span class="hlt">gradient</span> with exercise. This study evaluates the prevalence and predictors of an exercise-induced arm-leg <span class="hlt">gradient</span> in subjects who have undergone an apparently successful intervention for CoA.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19740025684','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19740025684"><span>A theoretical and flight test study of <span class="hlt">pressure</span> fluctuations under a turbulent boundary layer. Part 2: Flight test study</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Panton, R. L.; Lowery, R. L.; Reischman, M. M.</p> <p>1967-01-01</p> <p>The study of <span class="hlt">pressure</span> fluctuations under a turbulent boundary layer was undertaken with the objective of extending previous work to lower frequencies. Wind tunnel and flight test measurements are invalid at low frequencies because of extraneous <span class="hlt">acoustic</span> noises and free stream turbulence. A glider was instrumented and used as a test bed to carry microphones into a smooth flow free of <span class="hlt">acoustic</span> noise. Hodgson had previously measured the spectrum of boundary layer noise on a glider wing. These tests showed a drop off at low frequencies that could not be reproduced in any other facility. The measurements were made on the forward fuselage of a glider where the boundary layer could develop naturally and have some length in a zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> before the measurements were made. Two different sets of measurements were made.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1236848','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1236848"><span>Modeling of Propagation of Interacting Cracks Under Hydraulic <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Huang, Hai; Mattson, Earl Douglas; Podgorney, Robert Karl</p> <p></p> <p>A robust and reliable numerical model for fracture initiation and propagation, which includes the interactions among propagating fractures and the coupling between deformation, fracturing and fluid flow in fracture apertures and in the permeable rock matrix, would be an important tool for developing a better understanding of fracturing behaviors of crystalline brittle rocks driven by thermal and (or) hydraulic <span class="hlt">pressure</span> <span class="hlt">gradients</span>. In this paper, we present a physics-based hydraulic fracturing simulator based on coupling a quasi-static discrete element model (DEM) for deformation and fracturing with conjugate lattice network flow model for fluid flow in both fractures and porous matrix. Fracturingmore » is represented explicitly by removing broken bonds from the network to represent microcracks. Initiation of new microfractures and growth and coalescence of the microcracks leads to the formation of macroscopic fractures when external and/or internal loads are applied. The coupled DEM-network flow model reproduces realistic growth pattern of hydraulic fractures. In particular, simulation results of perforated horizontal wellbore clearly demonstrate that elastic interactions among multiple propagating fractures, fluid viscosity, strong coupling between fluid <span class="hlt">pressure</span> fluctuations within fractures and fracturing, and lower length scale heterogeneities, collectively lead to complicated fracturing patterns.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980227970','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980227970"><span>Charts and Tables for Estimating the Stability of the Compressible Laminar Boundary Layer with Heat Transfer and Arbitrary <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tetervin, Neal</p> <p>1959-01-01</p> <p>The minimum critical Reynolds numbers for the similar solutions of the compressible laminar boundary layer computed by Cohen and Reshotko and also for the Falkner and Skan solutions as recomputed by Smith have been calculated by Lin's rapid approximate method for two-dimensional disturbances. These results enable the stability of the compressible laminar boundary layer with heat transfer and <span class="hlt">pressure</span> <span class="hlt">gradient</span> to be easily estimated after the behavior of the boundary layer has been computed by the approximate method of Cohen and Reshotko. The previously reported unusual result (NACA Technical Note 4037) that a highly cooled stagnation point flow is more unstable than a highly cooled flat-plate flow is again encountered. Moreover, this result is found to be part of the more general result that a favorable <span class="hlt">pressure</span> <span class="hlt">gradient</span> is destabilizing for very cool walls when the Mach number is less than that for complete stability. The minimum critical Reynolds numbers for these wall temperature ratios are, however, all larger than any value of the laminar-boundary-layer Reynolds number likely to be encountered. For Mach numbers greater than those for which complete stability occurs a favorable <span class="hlt">pressure</span> <span class="hlt">gradient</span> is stabilizing, even for very cool walls.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980203085','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980203085"><span>Directional Electrostatic Accretion Process Employing <span class="hlt">Acoustic</span> Droplet Formation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Oeftering, Richard (Inventor)</p> <p>1998-01-01</p> <p>The present invention is directed to an apparatus for manufacturing a free standing solid metal part. In the present invention, metal droplets are ejected in a nozzleless fashion from a free surface pool of molten metal by applying focused <span class="hlt">acoustic</span> radiation <span class="hlt">pressure</span>. The <span class="hlt">acoustic</span> radiation <span class="hlt">pressure</span> is produced by high intensity <span class="hlt">acoustic</span> tone bursts emitted from an <span class="hlt">acoustic</span> source positioned at the bottom of the pool which directs the <span class="hlt">acoustic</span> energy at the pool surface. The metal droplets are electrostatically charged so their trajectory can be controlled by electric fields that guide the droplets to predetermined points on a target. The droplets impinge upon the target and solidify with the target material. The accretion of the electrostatically directed solidified droplets forms the free standing metal part.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3991613','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3991613"><span>The Influence of Body Position on Cerebrospinal Fluid <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> and Movement in Cats with Normal and Impaired Craniospinal Communication</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Radoš, Milan; Erceg, Gorislav; Petošić, Antonio; Jurjević, Ivana</p> <p>2014-01-01</p> <p>Intracranial hypertension is a severe therapeutic problem, as there is insufficient knowledge about the physiology of cerebrospinal fluid (CSF) <span class="hlt">pressure</span>. In this paper a new CSF <span class="hlt">pressure</span> regulation hypothesis is proposed. According to this hypothesis, the CSF <span class="hlt">pressure</span> depends on the laws of fluid mechanics and on the anatomical characteristics inside the cranial and spinal space, and not, as is today generally believed, on CSF secretion, circulation and absorption. The volume and <span class="hlt">pressure</span> changes in the newly developed CSF model, which by its anatomical dimensions and basic biophysical features imitates the craniospinal system in cats, are compared to those obtained on cats with and without the blockade of craniospinal communication in different body positions. During verticalization, a long-lasting occurrence of negative CSF <span class="hlt">pressure</span> inside the cranium in animals with normal cranio-spinal communication was observed. CSF <span class="hlt">pressure</span> <span class="hlt">gradients</span> change depending on the body position, but those <span class="hlt">gradients</span> do not enable unidirectional CSF circulation from the hypothetical site of secretion to the site of absorption in any of them. Thus, our results indicate the existence of new physiological/pathophysiological correlations between intracranial fluids, which opens up the possibility of new therapeutic approaches to intracranial hypertension. PMID:24748150</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24748150','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24748150"><span>The influence of body position on cerebrospinal fluid <span class="hlt">pressure</span> <span class="hlt">gradient</span> and movement in cats with normal and impaired craniospinal communication.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Klarica, Marijan; Radoš, Milan; Erceg, Gorislav; Petošić, Antonio; Jurjević, Ivana; Orešković, Darko</p> <p>2014-01-01</p> <p>Intracranial hypertension is a severe therapeutic problem, as there is insufficient knowledge about the physiology of cerebrospinal fluid (CSF) <span class="hlt">pressure</span>. In this paper a new CSF <span class="hlt">pressure</span> regulation hypothesis is proposed. According to this hypothesis, the CSF <span class="hlt">pressure</span> depends on the laws of fluid mechanics and on the anatomical characteristics inside the cranial and spinal space, and not, as is today generally believed, on CSF secretion, circulation and absorption. The volume and <span class="hlt">pressure</span> changes in the newly developed CSF model, which by its anatomical dimensions and basic biophysical features imitates the craniospinal system in cats, are compared to those obtained on cats with and without the blockade of craniospinal communication in different body positions. During verticalization, a long-lasting occurrence of negative CSF <span class="hlt">pressure</span> inside the cranium in animals with normal cranio-spinal communication was observed. CSF <span class="hlt">pressure</span> <span class="hlt">gradients</span> change depending on the body position, but those <span class="hlt">gradients</span> do not enable unidirectional CSF circulation from the hypothetical site of secretion to the site of absorption in any of them. Thus, our results indicate the existence of new physiological/pathophysiological correlations between intracranial fluids, which opens up the possibility of new therapeutic approaches to intracranial hypertension.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011JThSc..20..430H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011JThSc..20..430H"><span>Effect of <span class="hlt">acoustic</span> resonance phenomenon on fluid flow with light dust</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hamakawa, Hiromitsu; Arshad, Azim B. M.; Ohta, Mitsuo</p> <p>2011-10-01</p> <p>In the present paper, the attention is focused on the characteristics of lightweight materials collection in the duct using <span class="hlt">acoustic</span> resonance phenomena. The <span class="hlt">acoustic</span> resonance was excited by using a controlled speaker at the middle of a test duct. We measured the sound <span class="hlt">pressure</span> level, frequency response characteristics, <span class="hlt">acoustic</span> damping ratio, mode shape, and lightweight materials response to <span class="hlt">acoustic</span> resonance excited by a speaker. As a result, the <span class="hlt">acoustic</span> damping ratio decreased as the mode number of <span class="hlt">acoustic</span> resonance increased. The tissue strips and the lightweight materials were collected at the node of <span class="hlt">acoustic</span> <span class="hlt">pressure</span> when the <span class="hlt">acoustic</span> resonance was excited. It was made clear that it is possible to control lightweight materials using <span class="hlt">acoustic</span> resonance excited by a speaker.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150021421','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150021421"><span>AST Launch Vehicle <span class="hlt">Acoustics</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Houston, Janice; Counter, D.; Giacomoni, D.</p> <p>2015-01-01</p> <p>The liftoff phase induces <span class="hlt">acoustic</span> loading over a broad frequency range for a launch vehicle. These external <span class="hlt">acoustic</span> environments are then used in the prediction of internal vibration responses of the vehicle and components which result in the qualification levels. Thus, predicting these liftoff <span class="hlt">acoustic</span> (LOA) environments is critical to the design requirements of any launch vehicle. If there is a significant amount of uncertainty in the predictions or if <span class="hlt">acoustic</span> mitigation options must be implemented, a subscale <span class="hlt">acoustic</span> test is a feasible pre-launch test option to verify the LOA environments. The NASA Space Launch System (SLS) program initiated the Scale Model <span class="hlt">Acoustic</span> Test (SMAT) to verify the predicted SLS LOA environments and to determine the <span class="hlt">acoustic</span> reduction with an above deck water sound suppression system. The SMAT was conducted at Marshall Space Flight Center and the test article included a 5% scale SLS vehicle model, tower and Mobile Launcher. <span class="hlt">Acoustic</span> and <span class="hlt">pressure</span> data were measured by approximately 250 instruments. The SMAT liftoff <span class="hlt">acoustic</span> results are presented, findings are discussed and a comparison is shown to the Ares I Scale Model <span class="hlt">Acoustic</span> Test (ASMAT) results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140016707','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140016707"><span><span class="hlt">Acoustics</span> Research of Propulsion Systems</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gao, Ximing; Houston, Janice</p> <p>2014-01-01</p> <p>The liftoff phase induces high <span class="hlt">acoustic</span> loading over a broad frequency range for a launch vehicle. These external <span class="hlt">acoustic</span> environments are used in the prediction of the internal vibration responses of the vehicle and components. Present liftoff vehicle <span class="hlt">acoustic</span> environment prediction methods utilize stationary data from previously conducted hold-down tests to generate 1/3 octave band Sound <span class="hlt">Pressure</span> Level (SPL) spectra. In an effort to update the accuracy and quality of liftoff <span class="hlt">acoustic</span> loading predictions, non-stationary flight data from the Ares I-X were processed in PC-Signal in two flight phases: simulated hold-down and liftoff. In conjunction, the Prediction of <span class="hlt">Acoustic</span> Vehicle Environments (PAVE) program was developed in MATLAB to allow for efficient predictions of sound <span class="hlt">pressure</span> levels (SPLs) as a function of station number along the vehicle using semi-empirical methods. This consisted of generating the Dimensionless Spectrum Function (DSF) and Dimensionless Source Location (DSL) curves from the Ares I-X flight data. These are then used in the MATLAB program to generate the 1/3 octave band SPL spectra. Concluding results show major differences in SPLs between the hold-down test data and the processed Ares I-X flight data making the Ares I-X flight data more practical for future vehicle <span class="hlt">acoustic</span> environment predictions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S53B2804K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S53B2804K"><span><span class="hlt">Acoustic</span> Full Waveform Inversion to Characterize Near-surface Chemical Explosions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, K.; Rodgers, A. J.</p> <p>2015-12-01</p> <p>Recent high-quality, atmospheric overpressure data from chemical high-explosive experiments provide a unique opportunity to characterize near-surface explosions, specifically estimating yield and source time function. Typically, yield is estimated from measured signal features, such as peak <span class="hlt">pressure</span>, impulse, duration and/or arrival time of <span class="hlt">acoustic</span> signals. However, the application of full waveform inversion to <span class="hlt">acoustic</span> signals for yield estimation has not been fully explored. In this study, we apply a full waveform inversion method to local overpressure data to extract accurate <span class="hlt">pressure</span>-time histories of <span class="hlt">acoustics</span> sources during chemical explosions. A robust and accurate inversion technique for <span class="hlt">acoustic</span> source is investigated using numerical Green's functions that take into account atmospheric and topographic propagation effects. The inverted <span class="hlt">pressure</span>-time history represents the <span class="hlt">pressure</span> fluctuation at the source region associated with the explosion, and thus, provides a valuable information about <span class="hlt">acoustic</span> source mechanisms and characteristics in greater detail. We compare <span class="hlt">acoustic</span> source properties (i.e., peak overpressure, duration, and non-isotropic shape) of a series of explosions having different emplacement conditions and investigate the relationship of the <span class="hlt">acoustic</span> sources to the yields of explosions. The time histories of <span class="hlt">acoustic</span> sources may refine our knowledge of sound-generation mechanisms of shallow explosions, and thereby allow for accurate yield estimation based on <span class="hlt">acoustic</span> measurements. This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22972446','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22972446"><span>Preretinal partial <span class="hlt">pressure</span> of oxygen <span class="hlt">gradients</span> before and after experimental pars plana vitrectomy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Petropoulos, Ioannis K; Pournaras, Jean-Antoine C; Stangos, Alexandros N; Pournaras, Constantin J</p> <p>2013-01-01</p> <p>To evaluate preretinal partial <span class="hlt">pressure</span> of oxygen (PO2) <span class="hlt">gradients</span> before and after experimental pars plana vitrectomy. Arteriolar, venous, and intervascular preretinal PO2 <span class="hlt">gradients</span> were recorded in 7 minipigs during slow withdrawal of oxygen-sensitive microelectrodes (10-μm tip diameter) from the vitreoretinal interface to 2 mm into the vitreous cavity. Recordings were repeated after pars plana vitrectomy and balanced salt solution (BSS) intraocular perfusion. Arteriolar, venous, and intervascular preretinal PO2 at the vitreoretinal interface were 62.3 ± 13.8, 22.5 ± 3.3, and 17.0 ± 7.5 mmHg, respectively, before vitrectomy; 97.7 ± 19.9, 40.0 ± 21.9, and 56.3 ± 28.4 mmHg, respectively, immediately after vitrectomy; and 59.0 ± 27.4, 25.2 ± 3.0, and 21.5 ± 4.5 mmHg, respectively, 2½ hours after interruption of BSS perfusion. PO2 2 mm from the vitreoretinal interface was 28.4 ± 3.6 mmHg before vitrectomy; 151.8 ± 4.5 mmHg immediately after vitrectomy; and 34.8 ± 4.1 mmHg 2½ hours after interruption of BSS perfusion. PO2 <span class="hlt">gradients</span> were still present after vitrectomy, with the same patterns as before vitrectomy. Preretinal PO2 <span class="hlt">gradients</span> are not eliminated after pars plana vitrectomy. During BSS perfusion, vitreous cavity PO2 is very high. Interruption of BSS perfusion evokes progressive equilibration of vitreous cavity PO2 with concomitant progressive return of preretinal PO2 <span class="hlt">gradients</span> to their previtrectomy patterns. This indicates that preretinal diffusion of oxygen is not altered after vitrectomy. The beneficial effect of vitrectomy in ischemic retinal diseases or macular edema may be related to other mechanisms, such as increased oxygen convection currents or removal of growth factors and cytokines secreted in the vitreous.</p> </li> </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://hdl.handle.net/2060/19780016124','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19780016124"><span><span class="hlt">Acoustic</span> design of the QCSEE propulsion systems</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Loeffler, I. J.; Smith, E. B.; Sowers, H. D.</p> <p>1976-01-01</p> <p><span class="hlt">Acoustic</span> design features and techniques employed in the Quiet Clean Short-Haul Experimental Engine (QCSEE) Program are described. The role of jet/flap noise in selecting the engine fan <span class="hlt">pressure</span> ratio for powered lift propulsion systems is discussed. The QCSEE <span class="hlt">acoustic</span> design features include a hybrid inlet (near-sonic throat velocity with <span class="hlt">acoustic</span> treatment); low fan and core <span class="hlt">pressure</span> ratios; low fan tip speeds; gear-driven fans; high and low frequency stacked core noise treatment; multiple-thickness treatment; bulk absorber treatment; and treatment on the stator vanes. The QCSEE designs represent and anticipated <span class="hlt">acoustic</span> technology improvement of 12 to 16 PNdb relative to the noise levels of the low-noise engines used on current wide-body commercial jet transport aircraft.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvP...9e4009S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvP...9e4009S"><span>Harnessing Multiple Internal Reflections to Design Highly Absorptive <span class="hlt">Acoustic</span> Metasurfaces</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shen, Chen; Cummer, Steven A.</p> <p>2018-05-01</p> <p>The rapid development of metasurfaces has enabled numerous intriguing applications with <span class="hlt">acoustically</span> thin sheets. Here we report the theory and experimental realization of a nonresonant sound-absorbing strategy using metasurfaces by harnessing multiple internal reflections. We theoretically and numerically show that the higher-order diffraction of thin <span class="hlt">gradient</span>-index metasurfaces is tied to multiple internal reflections inside the unit cells. Highly absorbing <span class="hlt">acoustic</span> metasurfaces can be realized by enforcing multiple internal reflections together with a small amount of loss. A reflective <span class="hlt">gradient</span>-index <span class="hlt">acoustic</span> metasurface is designed based on the theory, and we further experimentally verify the performance using a three-dimensional printed prototype. Measurements show over 99% energy absorption at the peak frequency and a 95% energy absorption bandwidth of around 600 Hz. The proposed mechanism provides an alternative route for sound absorption without the necessity of high absorption of the individual unit cells.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007SPIE.6627E..0EV','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007SPIE.6627E..0EV"><span>Robust intravascular optical coherence elastography driven by <span class="hlt">acoustic</span> radiation <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>van Soest, Gijs; Bouchard, Richard R.; Mastik, Frits; de Jong, Nico; van der Steen, Anton F. W.</p> <p>2007-07-01</p> <p>High strain spots in the vessel wall indicate the presence of vulnerable plaques. The majority of acute cardiovascular events are preceded by rupture of such a plaque in a coronary artery. Intracoronary optical coherence tomography (OCT) can be extended, in principle, to an elastography technique, mapping the strain in the vascular wall. However, the susceptibility of OCT to frame-to-frame decorrelation, caused by tissue and catheter motion, inhibits reliable tissue displacement tracking and has to date obstructed the development of OCT-based intravascular elastography. We introduce a new technique for intravascular optical coherence elastography, which is robust against motion artifacts. Using <span class="hlt">acoustic</span> radiation force, we apply a <span class="hlt">pressure</span> to deform the tissue synchronously with the line scan rate of the OCT instrument. Radial tissue displacement can be tracked based on the correlation between adjacent lines, instead of subsequent frames in conventional elastography. The viability of the method is demonstrated with a simulation study. The root mean square (rms) error of the displacement estimate is 0.55 μm, and the rms error of the strain is 0.6%. It is shown that high-strain spots in the vessel wall, such as observed at the sites of vulnerable atherosclerotic lesions, can be detected with the technique. Experiments to realize this new elastographic method are presented. Simultaneous optical and ultrasonic pulse-echo tracking demonstrate that the material can be put in a high-frequency oscillatory motion with an amplitude of several micrometers, more than sufficient for accurate tracking with OCT. The resulting data are used to optimize the <span class="hlt">acoustic</span> pushing sequence and geometry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22463483','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22463483"><span>Thermodynamic and energy efficiency analysis of power generation from natural salinity <span class="hlt">gradients</span> by <span class="hlt">pressure</span> retarded osmosis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yip, Ngai Yin; Elimelech, Menachem</p> <p>2012-05-01</p> <p>The Gibbs free energy of mixing dissipated when fresh river water flows into the sea can be harnessed for sustainable power generation. <span class="hlt">Pressure</span> retarded osmosis (PRO) is one of the methods proposed to generate power from natural salinity <span class="hlt">gradients</span>. In this study, we carry out a thermodynamic and energy efficiency analysis of PRO work extraction. First, we present a reversible thermodynamic model for PRO and verify that the theoretical maximum extractable work in a reversible PRO process is identical to the Gibbs free energy of mixing. Work extraction in an irreversible constant-<span class="hlt">pressure</span> PRO process is then examined. We derive an expression for the maximum extractable work in a constant-<span class="hlt">pressure</span> PRO process and show that it is less than the ideal work (i.e., Gibbs free energy of mixing) due to inefficiencies intrinsic to the process. These inherent inefficiencies are attributed to (i) frictional losses required to overcome hydraulic resistance and drive water permeation and (ii) unutilized energy due to the discontinuation of water permeation when the osmotic <span class="hlt">pressure</span> difference becomes equal to the applied hydraulic <span class="hlt">pressure</span>. The highest extractable work in constant-<span class="hlt">pressure</span> PRO with a seawater draw solution and river water feed solution is 0.75 kWh/m(3) while the free energy of mixing is 0.81 kWh/m(3)-a thermodynamic extraction efficiency of 91.1%. Our analysis further reveals that the operational objective to achieve high power density in a practical PRO process is inconsistent with the goal of maximum energy extraction. This study demonstrates thermodynamic and energetic approaches for PRO and offers insights on actual energy accessible for utilization in PRO power generation through salinity <span class="hlt">gradients</span>. © 2012 American Chemical Society</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/twri/twri3-a17/','USGSPUBS'); return false;" href="https://pubs.usgs.gov/twri/twri3-a17/"><span><span class="hlt">Acoustic</span> velocity meter systems</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Laenen, Antonius</p> <p>1985-01-01</p> <p><span class="hlt">Acoustic</span> velocity meter (AVM) systems operate on the principles that the point-to-point upstream traveltime of an <span class="hlt">acoustic</span> pulse is longer than the downstream traveltime and that this difference in traveltime can be accurately measured by electronic devices. An AVM system is capable of recording water velocity (and discharge) under a wide range of conditions, but some constraints apply: 1. Accuracy is reduced and performance is degraded if the <span class="hlt">acoustic</span> path is not a continuous straight line. The path can be bent by reflection if it is too close to a stream boundary or by refraction if it passes through density <span class="hlt">gradients</span> resulting from variations in either water temperature or salinity. For paths of less than 100 m, a temperature <span class="hlt">gradient</span> of 0.1' per meter causes signal bending less than 0.6 meter at midchannel, and satisfactory velocity results can be obtained. Reflection from stream boundaries can cause signal cancellation if boundaries are too close to signal path. 2. Signal strength is attenuated by particles or bubbles that absorb, spread, or scatter sound. The concentration of particles or bubbles that can be tolerated is a function of the path length and frequency of the <span class="hlt">acoustic</span> signal. 3. Changes in streamline orientation can affect system accuracy if the variability is random. 4. Errors relating to signal resolution are much larger for a single threshold detection scheme than for multiple threshold schemes. This report provides methods for computing the effect of various conditions on the accuracy of a record obtained from an AVM. The equipment must be adapted to the site. Field reconnaissance and preinstallation analysis to detect possible problems are critical for proper installation and operation of an AVM system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5402700','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5402700"><span>Elimination of Trans-coarctation <span class="hlt">Pressure</span> <span class="hlt">Gradients</span> Has No Impact on Left Ventricular Function or Aortic Shear Stress Post Intervention in Patients with Mild Coarctation</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Keshavarz-Motamed, Zahra; Nezami, Farhad Rikhtegar; Partida, Ramon A.; Nakamura, Kenta; Staziaki, Pedro Vinícius; Ben-Assa, Eyal; Ghoshhajra, Brian; Bhatt, Ami B.; Edelman, Elazer R.</p> <p>2017-01-01</p> <p>OBJECTIVES To investigate the impact of transcatheter intervention on left ventricular (LV) function and aortic hemodynamics in patients with mild coarctation of the aorta (COA). BACKGROUND The optimal method and timing of transcatheter intervention for COA remains unclear, especially when the severity of COA is mild (peak-to-peak trans-coarctation <span class="hlt">pressure</span> <span class="hlt">gradient</span>, PKdP < 20 mmHg). Debate rages regarding the risk/benefit ratio of intervention vs. long-term effects of persistent minimal <span class="hlt">gradient</span> in this heterogeneous population with differing blood <span class="hlt">pressures</span>, ventricular function and peripheral perfusion. METHODS We developed a unique computational fluid dynamics and lumped parameter modeling framework based on patient-specific hemodynamic input parameters and validated it against patient-specific clinical outcomes (pre- and post-intervention). We used clinically measured hemodynamic metrics and imaging of the aorta and the LV in thirty-four patients with mild COA to make these correlations. RESULTS Despite dramatic reduction in trans-coarctation <span class="hlt">pressure</span> <span class="hlt">gradient</span> (catheter and Doppler echocardiography <span class="hlt">pressure</span> <span class="hlt">gradients</span> reduced 75% and 47.3%,), there was only modest effect on aortic flow and no significant impact on aortic shear stress (maximum time-averaged wall shear stress in descending aorta was reduced 5.1%). In no patient did transcatheter intervention improve LV function (e.g., stroke work and normalized stroke work were reduced by only 4.48% and 3.9%). CONCLUSIONS Transcatheter intervention which successfully relieves mild COA <span class="hlt">pressure</span> <span class="hlt">gradients</span> does not translate to decrease myocardial strain. The effects of intervention were determined to the greatest degree by ventricular-vascular coupling hemodynamics, and provide a novel valuable mechanism to evaluate patients with COA which may influence clinical practice. PMID:27659574</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940005676&hterms=Acoustic+levitation&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DAcoustic%2Blevitation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940005676&hterms=Acoustic+levitation&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DAcoustic%2Blevitation"><span>Determination of the viscous <span class="hlt">acoustic</span> field for liquid drop positioning/forcing in an <span class="hlt">acoustic</span> levitation chamber in microgravity</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lyell, Margaret J.</p> <p>1992-01-01</p> <p>The development of <span class="hlt">acoustic</span> levitation systems has provided a technology with which to undertake droplet studies as well as do containerless processing experiments in a microgravity environment. <span class="hlt">Acoustic</span> levitation chambers utilize radiation <span class="hlt">pressure</span> forces to position/manipulate the drop. Oscillations can be induced via frequency modulation of the <span class="hlt">acoustic</span> wave, with the modulated <span class="hlt">acoustic</span> radiation vector acting as the driving force. To account for tangential as well as radial forcing, it is necessary that the viscous effects be included in the <span class="hlt">acoustic</span> field. The method of composite expansions is employed in the determination of the <span class="hlt">acoustic</span> field with viscous effects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040161126','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040161126"><span>The Uses and Abuses of the <span class="hlt">Acoustic</span> Analogy in Helicopter Rotor Noise Prediction</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Farassat, F.; Brentner, Kenneth S.</p> <p>1987-01-01</p> <p>This paper is theoretical in nature and addresses applications of the <span class="hlt">acoustic</span> analogy in helicopter rotor noise prediction. It is argued that in many instances the <span class="hlt">acoustic</span> analogy has not been used with care in rotor noise studies. By this it is meant that approximate or inappropriate formulations have been used. By considering various mechanisms of noise generation, such abuses are identified and the remedy is suggested. The mechanisms discussed are thickness, loading, quadrupole, and blade-vortex interaction noise. The quadrupole term of the Ffowcs Williams-Hawkings equation is written in a new form which separates the contributions of regions of high <span class="hlt">gradients</span> such as shock surfaces. It is shown by order of magnitude studies that such regions are capable of producing noise with the same directivity as the thickness noise. The inclusion of this part of quadrupole sources in current <span class="hlt">acoustic</span> codes is quite practical. Some of the difficulties with the use of loading noise formulations of the first author in predictions of blade-vortex interaction noise are discussed. It appears that there is a need for development of new theoretical results based on the <span class="hlt">acoustic</span> analogy in this area. Because of the impulsive character of the blade surface <span class="hlt">pressure</span>, a time scale of integration different from that used in loading and thickness computations must he used in a computer code for prediction of blade-vortex interaction noise.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860019440','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860019440"><span>An analysis of blade vortex interaction aerodynamics and <span class="hlt">acoustics</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lee, D. J.</p> <p>1985-01-01</p> <p>The impulsive noise associated with helicopter flight due to Blade-Vortex Interaction, sometimes called blade slap is analyzed especially for the case of a close encounter of the blade-tip vortex with a following blade. Three parts of the phenomena are considered: the tip-vortex structure generated by the rotating blade, the unsteady <span class="hlt">pressure</span> produced on the following blade during the interaction, and the <span class="hlt">acoustic</span> radiation due to the unsteady <span class="hlt">pressure</span> field. To simplify the problem, the analysis was confined to the situation where the vortex is aligned parallel to the blade span in which case the maximum <span class="hlt">acoustic</span> <span class="hlt">pressure</span> results. <span class="hlt">Acoustic</span> radiation due to the interaction is analyzed in space-fixed coordinates and in the time domain with the unsteady <span class="hlt">pressure</span> on the blade surface as the source of chordwise compact, but spanwise non-compact radiation. Maximum <span class="hlt">acoustic</span> <span class="hlt">pressure</span> is related to the vortex core size and Reynolds number which are in turn functions of the blade-tip aerodynamic parameters. Finally noise reduction and performance are considered.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140016710','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140016710"><span>Mean Flow Augmented <span class="hlt">Acoustics</span> in Rocket Systems</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fischbach, Sean R.</p> <p>2014-01-01</p> <p>Oscillatory motion in solid rocket motors and liquid engines has long been a subject of concern. Many rockets display violent fluctuations in <span class="hlt">pressure</span>, velocity, and temperature originating from the complex interactions between the combustion process and gas dynamics. The customary approach to modeling <span class="hlt">acoustic</span> waves inside a rocket chamber is to apply the classical inhomogeneous wave equation to the combustion gas. The assumption of a linear, non-dissipative wave in a quiescent fluid remains valid while the <span class="hlt">acoustic</span> amplitudes are small and local gas velocities stay below Mach 0.2. The converging section of a rocket nozzle, where <span class="hlt">gradients</span> in <span class="hlt">pressure</span>, density, and velocity become large, is a notable region where this approach is not applicable. The expulsion of unsteady energy through the nozzle of a rocket is identified as the predominate source of <span class="hlt">acoustic</span> damping for most rocket systems. An accurate model of the <span class="hlt">acoustic</span> behavior within this region where <span class="hlt">acoustic</span> modes are influenced by the presence of a steady mean flow is required for reliable stability predictions. Recently, an approach to address nozzle damping with mean flow effects was implemented by French [1]. This new approach extends the work originated by Sigman and Zinn [2] by solving the <span class="hlt">acoustic</span> velocity potential equation (AVPE) formulated by perturbing the Euler equations [3]. The <span class="hlt">acoustic</span> velocity potential (psi) describing the <span class="hlt">acoustic</span> wave motion in the presence of an inhomogeneous steady high-speed flow is defined by, (del squared)(psi) - (lambda/c)(exp 2)(psi) - M(dot)[M(dot)(del)(del(psi))] - 2(lambda(M/c) + (M(dot)del(M))(dot)del(psi)-2(lambda)(psi)[M(dot)del(1/c)]=0 (1) with M as the Mach vector, c as the speed of sound, and lambda as the complex eigenvalue. French apply the finite volume method to solve the steady flow field within the combustion chamber and nozzle with inviscid walls. The complex eigenvalues and eigenvector are determined with the use of the ARPACK eigensolver. The</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20100020896&hterms=monograph&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dmonograph','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20100020896&hterms=monograph&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dmonograph"><span>ATK Launch Vehicle (ALV-X1) Liftoff <span class="hlt">Acoustic</span> Environments: Prediction vs. Measurement</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Houston, J.; Counter, Douglas; Kenny, Jeremy; Murphy, John</p> <p>2010-01-01</p> <p>Launched from the Mid-Atlantic Regional Spaceport (MARS) Pad 01B on August 22, 2008, the ATK Launch Vehicle (ALV-X1) provided an opportunity to measure liftoff <span class="hlt">acoustic</span> noise data. Predicted lift-off <span class="hlt">acoustic</span> environments were developed by both NASA MSFC and ATK engineers. ATK engineers developed predictions for use in determining vibro-<span class="hlt">acoustic</span> loads using the method described in the monograph NASA SP-8072. The MSFC ALV-X1 lift-off <span class="hlt">acoustic</span> prediction was made with the Vehicle <span class="hlt">Acoustic</span> Environment Prediction Program (VAEPP). The VAEPP and SP-8072 methods predict <span class="hlt">acoustic</span> <span class="hlt">pressures</span> of rocket systems generally scaled to existing rocket motor data based upon designed motor or engine characteristics. The predicted <span class="hlt">acoustic</span> <span class="hlt">pressures</span> are sound-<span class="hlt">pressure</span> spectra at specific positions on the vehicle. This paper presents the measured liftoff <span class="hlt">acoustics</span> on the vehicle and tower. This data is useful for the ALV-X1 in validating the pre-launch environments and loads predictions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Cryo...87..103J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Cryo...87..103J"><span>An approach for estimating <span class="hlt">acoustic</span> power in a pulse tube cryocooler</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jiang, Xiao; Qiu, Limin; Duan, Chaoxiang; You, Xiaokuan; Zhi, Xiaoqin</p> <p>2017-10-01</p> <p><span class="hlt">Acoustic</span> power at the cold end of regenerator is the measure of gross cooling capacity for a pulse tube cryocooler (PTC), which cannot be measured directly. Conventionally, the <span class="hlt">acoustic</span> power can only be derived from the measurement of velocity, <span class="hlt">pressure</span> and their phase angle, which is still a challenge for an oscillating flow at cryogenic temperatures. A new method is proposed for estimating the <span class="hlt">acoustic</span> power, which takes use of the easily measurable parameters, such as the <span class="hlt">pressure</span> and temperature, instead of the velocity and phase angle between the <span class="hlt">pressure</span> and velocity at cryogenic temperatures. The ratio of <span class="hlt">acoustic</span> powers at the both ends of isothermal components, like regenerator, heat exchangers, can be conveniently evaluated by using the ratio of <span class="hlt">pressure</span> amplitudes and the local temperatures. The ratio of <span class="hlt">acoustic</span> powers at the both ends of adiabatic components, like transfer line and pulse tube, is obtained by using the ratio of <span class="hlt">pressure</span> amplitudes. Accuracy of the approach for evaluating the <span class="hlt">acoustic</span> power for the regenerator is analyzed by comparing the results with those from REGEN 3.3 and references. For the cold end temperature range of 40-80 K, the deviation is less than 5% if the phase angle at the cold end of regenerator is around -30°. The simple method benefits estimating the <span class="hlt">acoustic</span> power and optimizing the PTC performance without interfering the cryogenic flow field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27624160','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27624160"><span>Laser-Induced <span class="hlt">Acoustic</span> Desorption Atmospheric <span class="hlt">Pressure</span> Photoionization via VUV-Generating Microplasmas.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Benham, Kevin; Hodyss, Robert; Fernández, Facundo M; Orlando, Thomas M</p> <p>2016-11-01</p> <p>We demonstrate the first application of laser-induced <span class="hlt">acoustic</span> desorption (LIAD) and atmospheric <span class="hlt">pressure</span> photoionization (APPI) as a mass spectrometric method for detecting low-polarity organics. This was accomplished using a Lyman-α (10.2 eV) photon generating microhollow cathode discharge (MHCD) microplasma photon source in conjunction with the addition of a gas-phase molecular dopant. This combination provided a soft desorption and a relatively soft ionization technique. Selected compounds analyzed include α-tocopherol, perylene, cholesterol, phenanthrene, phylloquinone, and squalene. Detectable surface concentrations as low as a few pmol per spot sampled were achievable using test molecules. The combination of LIAD and APPI provided a soft desorption and ionization technique that can allow detection of labile, low-polarity, structurally complex molecules over a wide mass range with minimal fragmentation. Graphical Abstract ᅟ.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ConPh..56..338V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ConPh..56..338V"><span>Pattern-formation under <span class="hlt">acoustic</span> driving forces</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Valverde, Jose Manuel</p> <p>2015-07-01</p> <p>Chemical and metallurgical processes enhanced by high intensity <span class="hlt">acoustic</span> waves, thermoacoustic engines and refrigerators, fuel rods in nuclear reactors, heat exchanger tubes, offshore and vibrating structures, solar thermal collectors, <span class="hlt">acoustic</span> levitators, microfluidic devices, cycling, musical <span class="hlt">acoustics</span>, blood flow through veins/arteries, hearing in the mammalian ear, carbon nanotube loudspeakers, etc. The evolution of a myriad of processes involving the oscillation of viscous fluids in the presence of solid boundaries is up to a certain extent influenced by <span class="hlt">acoustic</span> streaming. In addition to the sound field, viscous energy dissipation at the fluid-solid boundary causes a time-independent fluid circulation, which can lead to a significant enhancement of heat, mass and momentum transfer at large oscillation amplitudes. A particularly relevant phenomenon that can be notably affected by <span class="hlt">acoustic</span> streaming is the promotion of sound waves by temperature <span class="hlt">gradients</span> or viceversa (thermoacoustics), which is at the basis of potentially efficient and environmental friendly engines and refrigerators that have attracted a renewed interest in the last years. In the present manuscript, historical developments and the underlying basic physics behind <span class="hlt">acoustic</span> streaming and thermoacoustics are reviewed from an unifying perspective.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1616861M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1616861M"><span>Fluid displacement fronts in porous media: pore scale interfacial jumps, <span class="hlt">pressure</span> bursts and <span class="hlt">acoustic</span> emissions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moebius, Franziska; Or, Dani</p> <p>2014-05-01</p> <p>The macroscopically smooth and regular motion of fluid fronts in porous media is composed of numerous rapid pore-scale interfacial jumps and <span class="hlt">pressure</span> bursts that involve intense interfacial energy release in the form of <span class="hlt">acoustic</span> emissions. The characteristics of these pore scale events affect residual phase entrapment and transport properties behind the front. We present experimental studies using <span class="hlt">acoustic</span> emission technique (AE), rapid imaging, and liquid <span class="hlt">pressure</span> measurements to characterize these processes during drainage and imbibition in simple porous media. Imbibition and drainage produce different AE signatures (AE amplitudes obey a power law). For rapid drainage, AE signals persist long after cessation of front motion reflecting fluid redistribution and interfacial relaxation. Imaging revealed that the velocity of interfacial jumps often exceeds front velocity by more than 50 fold and is highly inertial component (Re>1000). Pore invasion volumes reduced deduced from <span class="hlt">pressure</span> fluctuations waiting times (for constant withdrawal rates) show remarkable agreement with geometrically-deduced pore volumes. Discrepancies between invaded volumes and geometrical pores increase with increasing capillary numbers due to constraints on evacuation opportunity times and simultaneous invasion events. A mechanistic model for interfacial motions in a pore-throat network was developed to investigate interfacial dynamics focusing on the role of inertia. Results suggest that while pore scale dynamics were sensitive to variations in pore geometry and boundary conditions, inertia exerted only a minor effect on phase entrapment. The study on pore scale invasion events paints a complex picture of rapid and inertial motions and provides new insights on mechanisms at displacement fronts that are essential for improved macroscopic description of multiphase flows in porous media.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19750000232','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19750000232"><span>Levitation of objects using <span class="hlt">acoustic</span> energy</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Whymark, R. R.</p> <p>1975-01-01</p> <p>Activated sound source establishes standing-wave pattern in gap between source and <span class="hlt">acoustic</span> reflector. Solid or liquid material introduced in region will move to one of the low <span class="hlt">pressure</span> areas produced at antinodes and remain suspended as long as <span class="hlt">acoustic</span> signal is present.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDG17002W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDG17002W"><span>Effects of surface roughness on an adverse-<span class="hlt">pressure-gradient</span> separating turbulent boundary layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wu, Wen; Piomelli, Ugo; Turbulence Simulation; Modelling Laboratory Team</p> <p>2017-11-01</p> <p>Separating turbulent boundary layers over smooth and rough flat plates are investigated by large-eddy simulations. A suction-blowing velocity distribution is imposed at the top boundary to produce an adverse-to-favourable <span class="hlt">pressure</span> <span class="hlt">gradient</span> and a closed separation bubble. Sandgrain roughness in the fully-rough regime is modelled by an immersed boundary method. In the rough-wall case, streamline detachment occurs earlier and the separation region is substantially larger due to the momentum deficit caused by the roughness. The adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> decreases the form drag and causes a thin reversed-flow region below the roughness crest, so that Cf = 0 does not coincide with the detachment of the flow from the surface. The wake regions behind roughness elements affect the intermittency of the near-wall flow, so that upstream of the detachment point the flow can be reversed half of the time, but its average is positive. The separated shear layer exhibits higher turbulent kinetic energy (TKE); the growth of the TKE there begins earlier relative to the separation point, and the peak TKE occurs close to the separation point. The momentum deficit caused by the roughness, again, plays a critical role in these changes. The authors acknowledge the support from Hydro-Québec and the NSERC Collaborative Research & Development program (CRDPJ 418786-11). The simulations were performed at CAC Queen't site. UP also thanks the support of Canada Research Chair Program.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016Cryo...80....1H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016Cryo...80....1H"><span><span class="hlt">Acoustic</span> field modulation in regenerators</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hu, J. Y.; Wang, W.; Luo, E. C.; Chen, Y. Y.</p> <p>2016-12-01</p> <p>The regenerator is a key component that transfers energy between heat and work. The conversion efficiency is significantly influenced by the <span class="hlt">acoustic</span> field in the regenerator. Much effort has been spent to quantitatively determine this influence, but few comprehensive experimental verifications have been performed because of difficulties in modulating and measuring the <span class="hlt">acoustic</span> field. In this paper, a method requiring two compressors is introduced and theoretically investigated that achieves <span class="hlt">acoustic</span> field modulation in the regenerator. One compressor outputs the <span class="hlt">acoustic</span> power for the regenerator; the other acts as a phase shifter. A RC load dissipates the <span class="hlt">acoustic</span> power out of both the regenerator and the latter compressor. The <span class="hlt">acoustic</span> field can be modulated by adjusting the current in the two compressors and opening the RC load. The <span class="hlt">acoustic</span> field is measured with <span class="hlt">pressure</span> sensors instead of flow-field imaging equipment, thereby greatly simplifying the experiment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790008479','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790008479"><span>Preliminary characterization of a one-axis <span class="hlt">acoustic</span> system. [<span class="hlt">acoustic</span> levitation for space processing</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Oran, W. A.; Reiss, D. A.; Berge, L. H.; Parker, H. W.</p> <p>1979-01-01</p> <p>The <span class="hlt">acoustic</span> fields and levitation forces produced along the axis of a single-axis resonance system were measured. The system consisted of a St. Clair generator and a planar reflector. The levitation force was measured for bodies of various sizes and geometries (i.e., spheres, cylinders, and discs). The force was found to be roughly proportional to the volume of the body until the characteristic body radius reaches approximately 2/k (k = wave number). The <span class="hlt">acoustic</span> <span class="hlt">pressures</span> along the axis were modeled using Huygens principle and a method of imaging to approximate multiple reflections. The modeled <span class="hlt">pressures</span> were found to be in reasonable agreement with those measured with a calibrated microphone.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25502599','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25502599"><span>Characterization of the startup transient electrokinetic flow in rectangular channels of arbitrary dimensions, zeta potential distribution, and time-varying <span class="hlt">pressure</span> <span class="hlt">gradient</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Miller, Andrew; Villegas, Arturo; Diez, F Javier</p> <p>2015-03-01</p> <p>The solution to the startup transient EOF in an arbitrary rectangular microchannel is derived analytically and validated experimentally. This full 2D transient solution describes the evolution of the flow through five distinct periods until reaching a final steady state. The derived analytical velocity solution is validated experimentally for different channel sizes and aspect ratios under time-varying <span class="hlt">pressure</span> <span class="hlt">gradients</span>. The experiments used a time resolved micro particle image velocimetry technique to calculate the startup transient velocity profiles. The measurements captured the effect of time-varying <span class="hlt">pressure</span> <span class="hlt">gradient</span> fields derived in the analytical solutions. This is tested by using small reservoirs at both ends of the channel which allowed a time-varying <span class="hlt">pressure</span> <span class="hlt">gradient</span> to develop with a time scale on the order of the transient EOF. Results showed that under these common conditions, the effect of the <span class="hlt">pressure</span> build up in the reservoirs on the temporal development of the transient startup EOF in the channels cannot be neglected. The measurements also captured the analytical predictions for channel walls made of different materials (i.e., zeta potentials). This was tested in channels that had three PDMS and one quartz wall, resulting in a flow with an asymmetric velocity profile due to variations in the zeta potential between the walls. © 2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> </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/1993PhDT........28G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1993PhDT........28G"><span>Combustion response to <span class="hlt">acoustic</span> perturbation in liquid rocket engines</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ghafourian, Akbar</p> <p></p> <p>An experimental study of the effect of <span class="hlt">acoustic</span> perturbations on combustion behavior of a model liquid propellant rocket engine has been carried out. A pair of compression drivers were used to excite transverse and longitudinal <span class="hlt">acoustic</span> fields at strengths of up to 156.6 dB and 159.5 dB respectively in the combustion chamber of the experimental rocket engine. Propellant simulants were injected into the combustion chamber through a single element shear coaxial injector. Water and air were used in cold flow studies and ethanol and oxygen-enriched air were used as fuel and oxidizer in reacting hot flow studies. In cold flow studies an imposed transverse <span class="hlt">acoustic</span> field had a more pronounced effect on the spray pattern than a longitudinal <span class="hlt">acoustic</span> fields. A transverse <span class="hlt">acoustic</span> field widened the spray by as much as 33 percent and the plane of impingement of the spray with chamber walls moved up closer to the injection plane. The behavior was strongly influenced by the gas phase velocity but was less sensitive to changes in the liquid phase velocity. In reacting hot flow studies the effects of changes in equivalence ratio, excitation amplitude, excitation frequency, liquid and gas phase velocity and chamber <span class="hlt">pressure</span> on the response of the injector to imposed high frequency transverse <span class="hlt">acoustic</span> excitation were measured. Reducing the equivalence ratio from 7.4 to 3.8 increased the chamber <span class="hlt">pressure</span> response to the imposed excitation at 3000 Hz. Increasing the excitation amplitude from 147 dB to 155.6 dB at 3000 Hz increased the chamber <span class="hlt">pressure</span> response to the excitation. In the frequency range of 1240 Hz to 3220 Hz, an excitation frequency of 3000 Hz resulted in the largest response of the chamber <span class="hlt">pressure</span> indicating the importance of fluid dynamic coupling. Increasing the liquid phase velocity from 9.2 m/sec to 22.7 m/sec, did not change the amplitude of the chamber <span class="hlt">pressure</span> response to excitation. This implied the importance of local equivalence ratio and not the overall</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhCS1001a2001A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS1001a2001A"><span>Reynolds stress structures in a self-similar adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> turbulent boundary layer at the verge of separation.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Atkinson, C.; Sekimoto, A.; Jiménez, J.; Soria, J.</p> <p>2018-04-01</p> <p>Mean Reynolds stress profiles and instantaneous Reynolds stress structures are investigated in a self-similar adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> turbulent boundary layer (APG-TBL) at the verge of separation using data from direct numerical simulations. The use of a self-similar APG-TBL provides a flow domain in which the flow gradually approaches a constant non-dimensional <span class="hlt">pressure</span> <span class="hlt">gradient</span>, resulting in a flow in which the relative contribution of each term in the governing equations is independent of streamwise position over a domain larger than two boundary layer thickness. This allows the flow structures to undergo a development that is less dependent on the upstream flow history when compared to more rapidly decelerated boundary layers. This APG-TBL maintains an almost constant shape factor of H = 2.3 to 2.35 over a momentum thickness based Reynolds number range of Re δ 2 = 8420 to 12400. In the APG-TBL the production of turbulent kinetic energy is still mostly due to the correlation of streamwise and wall-normal fluctuations, 〈uv〉, however the contribution form the other components of the Reynolds stress tensor are no longer negligible. Statistical properties associated with the scale and location of sweeps and ejections in this APG-TBL are compared with those of a zero <span class="hlt">pressure</span> <span class="hlt">gradient</span> turbulent boundary layer developing from the same inlet profile, resulting in momentum thickness based range of Re δ 2 = 3400 to 3770. In the APG-TBL the peak in both the mean Reynolds stress and the production of turbulent kinetic energy move from the near wall region out to a point consistent with the displacement thickness height. This is associated with a narrower distribution of the Reynolds stress and a 1.6 times higher relative number of wall-detached negative uv structures. These structures occupy 5 times less of the boundary layer volume and show a similar reduction in their streamwise extent with respect to the boundary layer thickness. A significantly lower percentage</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JAG...150..314S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JAG...150..314S"><span><span class="hlt">Acoustic</span> propagation operators for <span class="hlt">pressure</span> waves on an arbitrarily curved surface in a homogeneous medium</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sun, Yimin; Verschuur, Eric; van Borselen, Roald</p> <p>2018-03-01</p> <p>The Rayleigh integral solution of the <span class="hlt">acoustic</span> Helmholtz equation in a homogeneous medium can only be applied when the integral surface is a planar surface, while in reality almost all surfaces where <span class="hlt">pressure</span> waves are measured exhibit some curvature. In this paper we derive a theoretically rigorous way of building propagation operators for <span class="hlt">pressure</span> waves on an arbitrarily curved surface. Our theory is still based upon the Rayleigh integral, but it resorts to matrix inversion to overcome the limitations faced by the Rayleigh integral. Three examples are used to demonstrate the correctness of our theory - propagation of <span class="hlt">pressure</span> waves acquired on an arbitrarily curved surface to a planar surface, on an arbitrarily curved surface to another arbitrarily curved surface, and on a spherical cap to a planar surface, and results agree well with the analytical solutions. The generalization of our method for particle velocities and the calculation cost of our method are also discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvE..96c3114S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvE..96c3114S"><span>Luminescence from cavitation bubbles deformed in uniform <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Supponen, Outi; Obreschkow, Danail; Kobel, Philippe; Farhat, Mohamed</p> <p>2017-09-01</p> <p>Presented here are observations that demonstrate how the deformation of millimetric cavitation bubbles by a uniform <span class="hlt">pressure</span> <span class="hlt">gradient</span> quenches single-collapse luminescence. Our innovative measurement system captures a broad luminescence spectrum (wavelength range, 300-900 nm) from the individual collapses of laser-induced bubbles in water. By varying the bubble size, driving <span class="hlt">pressure</span>, and perceived gravity level aboard parabolic flights, we probed the limit from aspherical to highly spherical bubble collapses. Luminescence was detected for bubbles of maximum radii within the previously uncovered range, R0=1.5 -6 mm, for laser-induced bubbles. The relative luminescence energy was found to rapidly decrease as a function of the bubble asymmetry quantified by the anisotropy parameter ζ , which is the dimensionless equivalent of the Kelvin impulse. As established previously, ζ also dictates the characteristic parameters of bubble-driven microjets. The threshold of ζ beyond which no luminescence is observed in our experiment closely coincides with the threshold where the microjets visibly pierce the bubble and drive a vapor jet during the rebound. The individual fitted blackbody temperatures range between Tlum=7000 and Tlum=11 500 K but do not show any clear trend as a function of ζ . Time-resolved measurements using a high-speed photodetector disclose multiple luminescence events at each bubble collapse. The averaged full width at half-maximum of the pulse is found to scale with R0 and to range between 10 and 20 ns.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140011603','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140011603"><span><span class="hlt">Acoustics</span> Research of Propulsion Systems</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gao, Ximing; Houston, Janice D.</p> <p>2014-01-01</p> <p>The liftoff phase induces some of the highest <span class="hlt">acoustic</span> loading over a broad frequency for a launch vehicle. These external <span class="hlt">acoustic</span> environments are used in the prediction of the internal vibration responses of the vehicle and components. Thus, predicting these liftoff <span class="hlt">acoustic</span> environments is critical to the design requirements of any launch vehicle but there are challenges. Present liftoff vehicle <span class="hlt">acoustic</span> environment prediction methods utilize stationary data from previously conducted hold-down tests; i.e. static firings conducted in the 1960's, to generate 1/3 octave band Sound <span class="hlt">Pressure</span> Level (SPL) spectra. These data sets are used to predict the liftoff <span class="hlt">acoustic</span> environments for launch vehicles. To facilitate the accuracy and quality of <span class="hlt">acoustic</span> loading, predictions at liftoff for future launch vehicles such as the Space Launch System (SLS), non-stationary flight data from the Ares I-X were processed in PC-Signal in two forms which included a simulated hold-down phase and the entire launch phase. In conjunction, the Prediction of <span class="hlt">Acoustic</span> Vehicle Environments (PAVE) program was developed in MATLAB to allow for efficient predictions of sound <span class="hlt">pressure</span> levels (SPLs) as a function of station number along the vehicle using semiempirical methods. This consisted, initially, of generating the Dimensionless Spectrum Function (DSF) and Dimensionless Source Location (DSL) curves from the Ares I-X flight data. These are then used in the MATLAB program to generate the 1/3 octave band SPL spectra. Concluding results show major differences in SPLs between the hold-down test data and the processed Ares IX flight data making the Ares I-X flight data more practical for future vehicle <span class="hlt">acoustic</span> environment predictions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090013386','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090013386"><span>Aeroelastic-<span class="hlt">Acoustics</span> Simulation of Flight Systems</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gupta, kajal K.; Choi, S.; Ibrahim, A.</p> <p>2009-01-01</p> <p>This paper describes the details of a numerical finite element (FE) based analysis procedure and a resulting code for the simulation of the <span class="hlt">acoustics</span> phenomenon arising from aeroelastic interactions. Both CFD and structural simulations are based on FE discretization employing unstructured grids. The sound <span class="hlt">pressure</span> level (SPL) on structural surfaces is calculated from the root mean square (RMS) of the unsteady <span class="hlt">pressure</span> and the <span class="hlt">acoustic</span> wave frequencies are computed from a fast Fourier transform (FFT) of the unsteady <span class="hlt">pressure</span> distribution as a function of time. The resulting tool proves to be unique as it is designed to analyze complex practical problems, involving large scale computations, in a routine fashion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26520322','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26520322"><span>Experimental and numerical investigations of resonant <span class="hlt">acoustic</span> waves in near-critical carbon dioxide.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hasan, Nusair; Farouk, Bakhtier</p> <p>2015-10-01</p> <p>Flow and transport induced by resonant <span class="hlt">acoustic</span> waves in a near-critical fluid filled cylindrical enclosure is investigated both experimentally and numerically. Supercritical carbon dioxide (near the critical or the pseudo-critical states) in a confined resonator is subjected to <span class="hlt">acoustic</span> field created by an electro-mechanical <span class="hlt">acoustic</span> transducer and the induced <span class="hlt">pressure</span> waves are measured by a fast response <span class="hlt">pressure</span> field microphone. The frequency of the <span class="hlt">acoustic</span> transducer is chosen such that the lowest <span class="hlt">acoustic</span> mode propagates along the enclosure. For numerical simulations, a real-fluid computational fluid dynamics model representing the thermo-physical and transport properties of the supercritical fluid is considered. The simulated <span class="hlt">acoustic</span> field in the resonator is compared with measurements. The formation of <span class="hlt">acoustic</span> streaming structures in the highly compressible medium is revealed by time-averaging the numerical solutions over a given period. Due to diverging thermo-physical properties of supercritical fluid near the critical point, large scale oscillations are generated even for small sound field intensity. The strength of the <span class="hlt">acoustic</span> wave field is found to be in direct relation with the thermodynamic state of the fluid. The effects of near-critical property variations and the operating <span class="hlt">pressure</span> on the formation process of the streaming structures are also investigated. Irregular streaming patterns with significantly higher streaming velocities are observed for near-pseudo-critical states at operating <span class="hlt">pressures</span> close to the critical <span class="hlt">pressure</span>. However, these structures quickly re-orient to the typical Rayleigh streaming patterns with the increase operating <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/864660','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/864660"><span><span class="hlt">Acoustical</span> heat pumping engine</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Wheatley, John C.; Swift, Gregory W.; Migliori, Albert</p> <p>1983-08-16</p> <p>The disclosure is directed to an <span class="hlt">acoustical</span> heat pumping engine without moving seals. A tubular housing holds a compressible fluid capable of supporting an <span class="hlt">acoustical</span> standing wave. An <span class="hlt">acoustical</span> driver is disposed at one end of the housing and the other end is capped. A second thermodynamic medium is disposed in the housing near to but spaced from the capped end. Heat is pumped along the second thermodynamic medium toward the capped end as a consequence both of the <span class="hlt">pressure</span> oscillation due to the driver and imperfect thermal contact between the fluid and the second thermodynamic medium.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/7008256','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/7008256"><span><span class="hlt">Acoustical</span> heat pumping engine</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Wheatley, J.C.; Swift, G.W.; Migliori, A.</p> <p>1983-08-16</p> <p>The disclosure is directed to an <span class="hlt">acoustical</span> heat pumping engine without moving seals. A tubular housing holds a compressible fluid capable of supporting an <span class="hlt">acoustical</span> standing wave. An <span class="hlt">acoustical</span> driver is disposed at one end of the housing and the other end is capped. A second thermodynamic medium is disposed in the housing near to but spaced from the capped end. Heat is pumped along the second thermodynamic medium toward the capped end as a consequence both of the <span class="hlt">pressure</span> oscillation due to the driver and imperfect thermal contact between the fluid and the second thermodynamic medium. 2 figs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DPPT11093S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DPPT11093S"><span>Investigation of energetic particle induced geodesic <span class="hlt">acoustic</span> mode</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schneller, Mirjam; Fu, Guoyong; Chavdarovski, Ilija; Wang, Weixing; Lauber, Philipp; Lu, Zhixin</p> <p>2017-10-01</p> <p>Energetic particles are ubiquitous in present and future tokamaks due to heating systems and fusion reactions. Anisotropy in the distribution function of the energetic particle population is able to excite oscillations from the continuous spectrum of geodesic <span class="hlt">acoustic</span> modes (GAMs), which cannot be driven by plasma <span class="hlt">pressure</span> <span class="hlt">gradients</span> due to their toroidally and nearly poloidally symmetric structures. These oscillations are known as energetic particle-induced geodesic <span class="hlt">acoustic</span> modes (EGAMs) [G.Y. Fu'08] and have been observed in recent experiments [R. Nazikian'08]. EGAMs are particularly attractive in the framework of turbulence regulation, since they lead to an oscillatory radial electric shear which can potentially saturate the turbulence. For the presented work, the nonlinear gyrokinetic, electrostatic, particle-in-cell code GTS [W.X. Wang'06] has been extended to include an energetic particle population following either bump-on-tail Maxwellian or slowing-down [Stix'76] distribution function. With this new tool, we study growth rate, frequency and mode structure of the EGAM in an ASDEX Upgrade-like scenario. A detailed understanding of EGAM excitation reveals essential for future studies of EGAM interaction with micro-turbulence. Funded by the Max Planck Princeton Research Center. Computational resources of MPCDF and NERSC are greatefully acknowledged.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790054016&hterms=1043&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3D%2526%25231043','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790054016&hterms=1043&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3D%2526%25231043"><span>Gap heating with <span class="hlt">pressure</span> <span class="hlt">gradients</span>. [for Shuttle Orbiter thermal protection system tiles</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Scott, C. D.; Maraia, R. J.</p> <p>1979-01-01</p> <p>The heating rate distribution and temperature response on the gap walls of insulating tiles is analyzed to determine significant phenomena and parameters in flows where there is an external surface <span class="hlt">pressure</span> <span class="hlt">gradient</span>. Convective heating due to gap flow, modeled as fully developed pipe flow, is coupled with a two-dimensional thermal model of the tiles that includes conduction and radiative heat transfer. To account for geometry and important environmental parameters, scale factors are obtained by curve-fitting measured temperatures to analytical solutions. These scale factors are then used to predict the time-dependent gap heat flux and temperature response of tile gaps on the Space Shuttle Orbiter during entry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930004210','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930004210"><span><span class="hlt">Acoustic</span> modes in fluid networks</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Michalopoulos, C. D.; Clark, Robert W., Jr.; Doiron, Harold H.</p> <p>1992-01-01</p> <p><span class="hlt">Pressure</span> and flow rate eigenvalue problems for one-dimensional flow of a fluid in a network of pipes are derived from the familiar transmission line equations. These equations are linearized by assuming small velocity and <span class="hlt">pressure</span> oscillations about mean flow conditions. It is shown that the flow rate eigenvalues are the same as the <span class="hlt">pressure</span> eigenvalues and the relationship between line <span class="hlt">pressure</span> modes and flow rate modes is established. A volume at the end of each branch is employed which allows any combination of boundary conditions, from open to closed, to be used. The Jacobi iterative method is used to compute undamped natural frequencies and associated <span class="hlt">pressure</span>/flow modes. Several numerical examples are presented which include <span class="hlt">acoustic</span> modes for the Helium Supply System of the Space Shuttle Orbiter Main Propulsion System. It should be noted that the method presented herein can be applied to any one-dimensional <span class="hlt">acoustic</span> system involving an arbitrary number of branches.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApPhL.112i3503L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApPhL.112i3503L"><span>Broadband <span class="hlt">acoustic</span> phased array with subwavelength active tube array</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Xiao-Yan; Yang, Zhang-Zhao; Zhu, Yi-Fan; Zou, Xin-Ye; Cheng, Jian-Chun</p> <p>2018-02-01</p> <p><span class="hlt">Acoustic</span> metasurfaces provide a way to manipulate wavefronts at anomalous reflection or refraction angles through subwavelength structures. Here, based on the generalized Snell's refraction law for <span class="hlt">acoustic</span> metasurfaces and the classical <span class="hlt">acoustic</span> phased array (PA) theory, a broadband <span class="hlt">acoustic</span> PA with a subwavelength active tube array has been proposed to form a special <span class="hlt">acoustic</span> beam and to determine the directivity characteristics of the <span class="hlt">acoustic</span> source. Theoretical analysis shows that the dispersionless wavefront manipulation can be realized by the <span class="hlt">gradient</span> model of the active tube array, and a wide working frequency band can be obtained in practical applications from the simulated and experimental results. The numerical results of forming a special <span class="hlt">acoustic</span> beam and establishing an <span class="hlt">acoustic</span> focus model with an arbitrary focal position are consistent with the theoretical predictions. The experimental results agree well with the simulated results in the model of forming the <span class="hlt">acoustic</span> beam of 45 ° . By combining <span class="hlt">acoustic</span> metamaterials and conventional <span class="hlt">acoustic</span> PA, the model of the active tube array paves a way to design a composite <span class="hlt">acoustic</span> PA with high radiation efficiency and system robustness without the need for any complex circuit control system. This design concept is expected to be used in the design of ultrasonic therapy devices and high-efficiency transducers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980201049','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980201049"><span>A Comparison of Signal Enhancement Methods for Extracting Tonal <span class="hlt">Acoustic</span> Signals</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jones, Michael G.</p> <p>1998-01-01</p> <p>The measurement of pure tone <span class="hlt">acoustic</span> <span class="hlt">pressure</span> signals in the presence of masking noise, often generated by mean flow, is a continual problem in the field of passive liner duct <span class="hlt">acoustics</span> research. In support of the Advanced Subsonic Technology Noise Reduction Program, methods were investigated for conducting measurements of advanced duct liner concepts in harsh, aeroacoustic environments. This report presents the results of a comparison study of three signal extraction methods for acquiring quality <span class="hlt">acoustic</span> <span class="hlt">pressure</span> measurements in the presence of broadband noise (used to simulate the effects of mean flow). The performance of each method was compared to a baseline measurement of a pure tone <span class="hlt">acoustic</span> <span class="hlt">pressure</span> 3 dB above a uniform, broadband noise background.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24449879','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24449879"><span><span class="hlt">Acoustic</span> droplet vaporization is initiated by superharmonic focusing.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shpak, Oleksandr; Verweij, Martin; Vos, Hendrik J; de Jong, Nico; Lohse, Detlef; Versluis, Michel</p> <p>2014-02-04</p> <p><span class="hlt">Acoustically</span> sensitive emulsion droplets composed of a liquid perfluorocarbon have the potential to be a highly efficient system for local drug delivery, embolotherapy, or for tumor imaging. The physical mechanisms underlying the <span class="hlt">acoustic</span> activation of these phase-change emulsions into a bubbly dispersion, termed <span class="hlt">acoustic</span> droplet vaporization, have not been well understood. The droplets have a very high activation threshold; its frequency dependence does not comply with homogeneous nucleation theory and localized nucleation spots have been observed. Here we show that <span class="hlt">acoustic</span> droplet vaporization is initiated by a combination of two phenomena: highly nonlinear distortion of the <span class="hlt">acoustic</span> wave before it hits the droplet and focusing of the distorted wave by the droplet itself. At high excitation <span class="hlt">pressures</span>, nonlinear distortion causes significant superharmonics with wavelengths of the order of the droplet size. These superharmonics strongly contribute to the focusing effect; therefore, the proposed mechanism also explains the observed <span class="hlt">pressure</span> thresholding effect. Our interpretation is validated with experimental data captured with an ultrahigh-speed camera on the positions of the nucleation spots, where we find excellent agreement with the theoretical prediction. Moreover, the presented mechanism explains the hitherto counterintuitive dependence of the nucleation threshold on the ultrasound frequency. The physical insight allows for the optimization of <span class="hlt">acoustic</span> droplet vaporization for therapeutic applications, in particular with respect to the <span class="hlt">acoustic</span> <span class="hlt">pressures</span> required for activation, thereby minimizing the negative bioeffects associated with the use of high-intensity ultrasound.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3918756','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3918756"><span><span class="hlt">Acoustic</span> droplet vaporization is initiated by superharmonic focusing</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Shpak, Oleksandr; Verweij, Martin; Vos, Hendrik J.; de Jong, Nico; Lohse, Detlef; Versluis, Michel</p> <p>2014-01-01</p> <p><span class="hlt">Acoustically</span> sensitive emulsion droplets composed of a liquid perfluorocarbon have the potential to be a highly efficient system for local drug delivery, embolotherapy, or for tumor imaging. The physical mechanisms underlying the <span class="hlt">acoustic</span> activation of these phase-change emulsions into a bubbly dispersion, termed <span class="hlt">acoustic</span> droplet vaporization, have not been well understood. The droplets have a very high activation threshold; its frequency dependence does not comply with homogeneous nucleation theory and localized nucleation spots have been observed. Here we show that <span class="hlt">acoustic</span> droplet vaporization is initiated by a combination of two phenomena: highly nonlinear distortion of the <span class="hlt">acoustic</span> wave before it hits the droplet and focusing of the distorted wave by the droplet itself. At high excitation <span class="hlt">pressures</span>, nonlinear distortion causes significant superharmonics with wavelengths of the order of the droplet size. These superharmonics strongly contribute to the focusing effect; therefore, the proposed mechanism also explains the observed <span class="hlt">pressure</span> thresholding effect. Our interpretation is validated with experimental data captured with an ultrahigh-speed camera on the positions of the nucleation spots, where we find excellent agreement with the theoretical prediction. Moreover, the presented mechanism explains the hitherto counterintuitive dependence of the nucleation threshold on the ultrasound frequency. The physical insight allows for the optimization of <span class="hlt">acoustic</span> droplet vaporization for therapeutic applications, in particular with respect to the <span class="hlt">acoustic</span> <span class="hlt">pressures</span> required for activation, thereby minimizing the negative bioeffects associated with the use of high-intensity ultrasound. PMID:24449879</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140017046','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140017046"><span><span class="hlt">Acoustic</span> Test Results of Melamine Foam with Application to Payload Fairing <span class="hlt">Acoustic</span> Attenuation Systems</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hughes, William O.; McNelis, Anne M.</p> <p>2014-01-01</p> <p>A spacecraft at launch is subjected to a harsh <span class="hlt">acoustic</span> and vibration environment resulting from the passage of <span class="hlt">acoustic</span> energy, created during the liftoff of a launch vehicle, through the vehicle's payload fairing. In order to ensure the mission success of the spacecraft it is often necessary to reduce the resulting internal <span class="hlt">acoustic</span> sound <span class="hlt">pressure</span> levels through the usage of <span class="hlt">acoustic</span> attenuation systems. Melamine foam, lining the interior walls of the payload fairing, is often utilized as the main component of such a system. In order to better understand the <span class="hlt">acoustic</span> properties of melamine foam, with the goal of developing improved <span class="hlt">acoustic</span> attenuation systems, NASA has recently performed panel level testing on numerous configurations of melamine foam <span class="hlt">acoustic</span> treatments at the Riverbank <span class="hlt">Acoustical</span> Laboratory. Parameters assessed included the foam's thickness and density, as well as the effects of a top outer cover sheet material and mass barriers embedded within the foam. This testing followed the ASTM C423 standard for absorption and the ASTM E90 standard for transmission loss. The <span class="hlt">acoustic</span> test data obtained and subsequent conclusions are the subjects of this paper.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008JFST....3..805H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008JFST....3..805H"><span><span class="hlt">Acoustic</span> Resonance and Vortex Shedding from Tube Banks of Boiler Plant</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hamakawa, Hiromitsu; Matsue, Hiroto; Nishida, Eiichi; Fukano, Tohru</p> <p></p> <p>This paper focuses on the relationship between <span class="hlt">acoustic</span> resonance and vortex shedding from the tube banks of a boiler plant. We have built a model similar to the actual boiler plant to clarify the characteristics of <span class="hlt">acoustic</span> resonance phenomena and vortex shedding. The model used in-line tube banks with a small tube pitch ratio. We examined the relationship between the <span class="hlt">acoustic</span> resonance of the actual plant and that of the model, and measured the sound <span class="hlt">pressure</span> level, <span class="hlt">acoustic</span> <span class="hlt">pressure</span> mode shape, spectrum of velocity fluctuation, and gap velocity. Gap velocity was defined as the mean velocity in the smallest gaps between two neighboring tubes in the transverse direction. As a result, the resonant frequencies and mode shapes of the <span class="hlt">acoustic</span> resonances in the actual boiler plant agreed well with those in the similar model. We found many peak frequencies in the sound <span class="hlt">pressure</span> level spectrum when <span class="hlt">acoustic</span> resonances occurred. The typical Strouhal numbers at the onset velocity of <span class="hlt">acoustic</span> resonances were about 0.19, 0.26 and 0.52. Periodic velocity fluctuation caused by vortex shedding was observed inside the tube banks without <span class="hlt">acoustic</span> resonance. The Strouhal number measured for vortex shedding was 0.15. <span class="hlt">Acoustic</span> resonances of higher-order modes were generated in this plant.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE10025E..0ZL','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE10025E..0ZL"><span>High-sensitivity fiber optic <span class="hlt">acoustic</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>Lu, Ping; Liu, Deming; Liao, Hao</p> <p>2016-11-01</p> <p>Due to the overwhelming advantages compared with traditional electronicsensors, fiber-optic <span class="hlt">acoustic</span> sensors have arisen enormous interest in multiple disciplines. In this paper we present the recent research achievements of our group on fiber-optic <span class="hlt">acoustic</span> sensors. The main point of our research is high sensitivity interferometric <span class="hlt">acoustic</span> sensors, including Michelson, Sagnac, and Fabry-Pérot interferometers. In addition, some advanced technologies have been proposed for <span class="hlt">acoustic</span> or <span class="hlt">acoustic</span> <span class="hlt">pressure</span> sensing such as single-mode/multimode fiber coupler, dual FBGs and multi-longitudinal mode fiber laser based <span class="hlt">acoustic</span> sensors. Moreover, our attention we have also been paid on signal demodulation schemes. The intensity-based quadrature point (Q-point) demodulation, two-wavelength quadrature demodulation and symmetric 3×3 coupler methodare discussed and compared in this paper.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930000660&hterms=gas+pump&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dgas%2Bpump','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930000660&hterms=gas+pump&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dgas%2Bpump"><span><span class="hlt">Acoustic</span> Pump</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Heyman, Joseph S.</p> <p>1993-01-01</p> <p>Pump uses <span class="hlt">acoustic</span>-radiation forces. Momentum transferred from sound waves to sound-propagating material in way resulting in net pumping action on material. <span class="hlt">Acoustic</span> pump is solid-state pump. Requires no moving parts, entirely miniaturized, and does not invade pumped environment. Silent, with no conventional vibration. Used as pump for liquid, suspension, gas, or any other medium interacting with radiation <span class="hlt">pressure</span>. Also used where solid-state pump needed for reliability and controllability. In microgravity environment, device offers unusual control for low flow rates. For medical or other applications in which contamination cannot be allowed, offers noninvasive pumping force.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_18 --> <div id="page_19" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="361"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDQ23009K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDQ23009K"><span>Transverse <span class="hlt">acoustic</span> forcing of a round hydrodynamically self-excited jet</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kushwaha, Abhijit Kumar; Mazur, Marek; Worth, Nicholas; Dawson, James; Li, Larry K. B.</p> <p>2017-11-01</p> <p>Hydrodynamically self-excited jets can readily synchronize with longitudinal <span class="hlt">acoustic</span> forcing, but their response to transverse <span class="hlt">acoustic</span> forcing is less clear. In this experimental study, we apply transverse <span class="hlt">acoustic</span> forcing to an axisymmetric low-density jet at frequencies around its natural global frequency. We place the jet in a rectangular box containing two loudspeakers, one at each end, producing nominally one-dimensional standing <span class="hlt">pressure</span> waves. By traversing the jet across this box, we subject it to a range of <span class="hlt">acoustic</span> modes, from purely longitudinal (streamwise) modes at the <span class="hlt">pressure</span> anti-node to purely transverse (cross-stream) modes at the <span class="hlt">pressure</span> node. Using time-resolved Background-Oriented Schlieren (BOS) imaging and hot-wire anemometry, we characterize the jet response for different forcing frequencies, amplitudes and mode shapes, providing new insight into the way transverse <span class="hlt">acoustic</span> oscillations interact with axisymmetric hydrodynamic oscillations. This work was supported by the Research Grants Council of Hong Kong (Project No. 16235716 and 26202815).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/867668','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/867668"><span>Methods and apparatus for moving and separating materials exhibiting different physical properties</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Peterson, Stephen C.; Brimhall, Owen D.; McLaughlin, Thomas J.; Baker, Charles D.; Sparks, Sam L.</p> <p>1991-01-01</p> <p>Methods and apparatus for controlling the movement of materials having different physical properties when one of the materials is a fluid. The invention does not rely on flocculation, sedimentation, centrifugation, the buoyancy of the materials, or any other gravity dependent characteristic, in order to achieve its desired results. The methods of the present invention provide that a first <span class="hlt">acoustic</span> wave is propagated through a vessel containing the materials. A second <span class="hlt">acoustic</span> wave, at a frequency different than the first <span class="hlt">acoustic</span> wave, is also propagated through the vessel so that the two <span class="hlt">acoustic</span> waves are superimposed upon each other. The superimposition of the two waves creates a beat frequency wave. The beat frequency wave comprises <span class="hlt">pressure</span> <span class="hlt">gradients</span> dividing regions of maximum and minimum <span class="hlt">pressure</span>. The <span class="hlt">pressure</span> <span class="hlt">gradients</span> and the regions of maximum and minimum <span class="hlt">pressure</span> move through space and time at a group velocity. The moving <span class="hlt">pressure</span> <span class="hlt">gradients</span> and regions of maximum and minimum <span class="hlt">pressure</span> act upon the materials so as to move one of the materials towards a predetermined location in the vessel. The present invention provides that the materials may be controllably moved toward a location, aggregated at a particular location, or physically separated from each other.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/866654','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/866654"><span>Methods and apparatus for moving and separating materials exhibiting different physical properties</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Peterson, Stephen C.; Brimhall, Owen D.; McLaughlin, Thomas J.; Baker, Charles D.; Sparks, Sam L.</p> <p>1988-01-01</p> <p>Methods and apparatus for controlling the movement of materials having different physical properties when one of the materials is a fluid. The invention does not rely on flocculation, sedimentation, centrifugation, the buoyancy of the materials, or any other gravity dependent characteristic, in order to achieve its desired results. The methods of the present invention provide that a first <span class="hlt">acoustic</span> wave is progpagated through a vessel containing the materials. A second <span class="hlt">acoustic</span> wave, at a frequency different than the first <span class="hlt">acoustic</span> wave, is also propagated through the vessel so that the two <span class="hlt">acoustic</span> waves are superimposed upon each other. The superimposition of the two waves creates a beat frequency wave. The beat frequency wave comprises <span class="hlt">pressure</span> <span class="hlt">gradients</span> dividing regions of maximum and minimum <span class="hlt">pressure</span>. The <span class="hlt">pressure</span> <span class="hlt">gradients</span> and the regions of maximum and minimum <span class="hlt">pressure</span> move through space and time at a group velocity. The moving <span class="hlt">pressure</span> <span class="hlt">gradients</span> and regions of maximum and minimum <span class="hlt">pressure</span> act upon the marterials so as to move one of the materials towards a predetermined location in the vessel. The present invention provides that the materials may be controllably moved toward a location, aggreated at a particular location, or physically separated from each other.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JAP...123l4501S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JAP...123l4501S"><span><span class="hlt">Acoustic</span> metacages for sound shielding with steady air flow</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shen, Chen; Xie, Yangbo; Li, Junfei; Cummer, Steven A.; Jing, Yun</p> <p>2018-03-01</p> <p>Conventional sound shielding structures typically prevent fluid transport between the exterior and interior. A design of a two-dimensional <span class="hlt">acoustic</span> metacage with subwavelength thickness which can shield <span class="hlt">acoustic</span> waves from all directions while allowing steady fluid flow is presented in this paper. The structure is designed based on <span class="hlt">acoustic</span> <span class="hlt">gradient</span>-index metasurfaces composed of open channels and shunted Helmholtz resonators. In-plane sound at an arbitrary angle of incidence is reflected due to the strong parallel momentum on the metacage surface, which leads to low sound transmission through the metacage. The performance of the proposed metacage is verified by numerical simulations and measurements on a three-dimensional printed prototype. The <span class="hlt">acoustic</span> metacage has potential applications in sound insulation where steady fluid flow is necessary or advantageous.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004ASAJ..115R2419M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004ASAJ..115R2419M"><span>Shape oscillations of <span class="hlt">acoustically</span> levitated drops in water: Early research with Bob Apfel on modulated radiation <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>Marston, Philip L.</p> <p>2004-05-01</p> <p>In 1976, research in collaboration with Bob Apfel demonstrated that low-frequency shape oscillations of hydrocarbon drops levitated in water could be driven using modulated radiation <span class="hlt">pressure</span>. While that response to modulated ultrasound was subsequently extended to a range of systems, the emphasis here is to recall the initial stages of development in Bob Apfel's laboratory leading to some publications [P. L. Marston and R. E. Apfel, J. Colloid Interface Sci. 68, 280-286 (1979); J. <span class="hlt">Acoust</span>. Soc. Am. 67, 27-37 (1980)]. The levitation technology used at that time was such that it was helpful to develop a sensitive method for detecting weak oscillations using the interference pattern in laser light scattered by levitated drops. The initial experiments to verify this scattering method used shape oscillations induced by modulated electric fields within the <span class="hlt">acoustic</span> levitator. Light scattering was subsequently used to detect shape oscillations induced by amplitude modulating a carrier having a high frequency (around 680 kHz) at a resonance of the transducer. Methods were also developed for quantitative measurements of the drop's response and with improved <span class="hlt">acoustic</span> coupling drop fission was observed. The connection with research currently supported by NASA will also be noted.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25506260','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25506260"><span>Changes in intracranial <span class="hlt">pressure</span> <span class="hlt">gradients</span> between the cerebral hemispheres in patients with intracerebral hematomas in one cerebral hemisphere.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Qiu, Wusi; Jiang, Qizhou; Xiao, Guoming; Wang, Weiming; Shen, Hong</p> <p>2014-01-01</p> <p>Intracranial-<span class="hlt">pressure</span> (ICP) monitoring is useful for patients with increased ICP following hemorrhagic stroke. In this study, the changes in <span class="hlt">pressure</span> <span class="hlt">gradients</span> between the two cerebral hemispheres were investigated after hemorrhagic stroke of one side, and after a craniotomy. Twenty-four patients with acute cerebral hemorrhages and intracerebral hematomas who exhibited mass effect and midline shift to the contralateral side on computed tomography were selected for this study. After admission, both sides of the cranium were drilled, and optical fiber sensors were implanted to monitor the brain parenchyma <span class="hlt">pressure</span> (BPP) in both cerebral hemispheres. All patients underwent surgical hematoma evacuations. The preoperative and postoperative BPP data from both cerebral hemispheres were collected at various time points and compared pairwise. There were statistically significant differences (P < 0.01) in the preoperative BPP values between the two hemispheres at three different time points. Differences in the BPP values between the two hemispheres at the time of surgery, and 24 and 48 h after surgery, were not statistically significant (P > 0.05). The posteroperative BPPs of both hemispheres were statistically significantly lower than preoperative recordings. BPP sensors should be applied to the injured cerebral hemisphere, because this becomes the source of increased ICP. Hematoma evacuation surgery effectively decreases ICP and eliminates <span class="hlt">pressure</span> <span class="hlt">gradients</span> between the two cerebral hemispheres, consequently enabling brain shift correction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MSSP...98..324S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MSSP...98..324S"><span>Vibro-<span class="hlt">acoustic</span> modeling and analysis of a coupled <span class="hlt">acoustic</span> system comprising a partially opened cavity coupled with a flexible plate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shi, Shuangxia; Su, Zhu; Jin, Guoyong; Liu, Zhigang</p> <p>2018-01-01</p> <p>This paper is concerned with the modeling and solution method of a three-dimensional (3D) coupled <span class="hlt">acoustic</span> system comprising a partially opened cavity coupled with a flexible plate and an exterior field of semi-infinite size, which is ubiquitously encountered in architectural <span class="hlt">acoustics</span> and is a reasonable representation of many engineering occasions. A general solution method is presented to predict the dynamic behaviors of the three-dimensional (3D) <span class="hlt">acoustic</span> coupled system, in which the displacement of the plate and the sound <span class="hlt">pressure</span> in the cavity are respectively constructed in the form of the two-dimensional and three-dimensional modified Fourier series with several auxiliary functions introduced to ensure the uniform convergence of the solution over the entire solution domain. The effect of the opening is taken into account via the work done by the sound <span class="hlt">pressure</span> acting at the coupling aperture that is contributed from the vibration of particles on the <span class="hlt">acoustic</span> coupling interface and on the structural-<span class="hlt">acoustic</span> coupling interface. Both the <span class="hlt">acoustic</span> coupling between finite cavity and exterior field and the structural-<span class="hlt">acoustic</span> coupling between flexible plate and interior <span class="hlt">acoustic</span> field are considered in the vibro-<span class="hlt">acoustic</span> modeling of the three-dimensional <span class="hlt">acoustic</span> coupled <span class="hlt">acoustic</span> system. The dynamic responses of the coupled structural-<span class="hlt">acoustic</span> system are obtained using the Rayleigh-Ritz procedure based on the energy expressions for the coupled system. The accuracy and effectiveness of the proposed method are validated through numerical examples and comparison with results obtained by the boundary element analysis. Furthermore, the influence of the opening and the cavity volume on the <span class="hlt">acoustic</span> behaviors of opened cavity system is studied.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27185055','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27185055"><span>Intrinsic advantages of packed capillaries over narrow-bore columns in very high-<span class="hlt">pressure</span> <span class="hlt">gradient</span> liquid chromatography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gritti, Fabrice; McDonald, Thomas; Gilar, Martin</p> <p>2016-06-17</p> <p>250μm×100mm fused silica glass capillaries were packed with 1.8μm high-strength silica (HSS) fully porous particles. They were prepared without bulky stainless steel endfittings and metal frits, which both generate significant sample dispersion. The isocratic efficiencies and <span class="hlt">gradient</span> peak capacities of these prototype capillary columns were measured for small molecules (n-alkanophenones) using a home-made ultra-low dispersive micro-HPLC instrument. Their resolution power was compared to that of standard 2.1mm×100mm very high-<span class="hlt">pressure</span> liquid chromatography (vHPLC) narrow-bore columns packed with the same particles. The results show that, for the same column efficiency (25000 plates) and <span class="hlt">gradient</span> steepness (0.04min(-1)), the peak capacity of the 250μm i.d. capillary columns is systematically 15-20% higher than that of the 2.1mm i.d. narrow-bore columns. A validated model of <span class="hlt">gradient</span> chromatography enabled one to predict accurately the observed peak capacities of the capillary columns for non-linear solvation strength retention behavior and under isothermal conditions. Thermodynamics applied to the eluent quantified the temperature difference for the thermal <span class="hlt">gradients</span> in both capillary and narrow-bore columns. Experimental data revealed that the <span class="hlt">gradient</span> peak capacity is more affected by viscous heating than the column efficiency. Unlike across 2.1mm i.d. columns, the changes in eluent composition across the 250μm i.d. columns during the <span class="hlt">gradient</span> is rapidly relaxed by transverse dispersion. The combination of (1) the absence of viscous heating and (2) the high uniformity of the eluent composition across the diameter of capillary columns explains the intrinsic advantage of capillary over narrow-bore columns in <span class="hlt">gradient</span> vHPLC. Copyright © 2016 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26611052','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26611052"><span>Parvulescu Revisited: Small Tank <span class="hlt">Acoustics</span> for Bioacousticians.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rogers, Peter H; Hawkins, Anthony D; Popper, Arthur N; Fay, Richard R; Gray, Michael D</p> <p>2016-01-01</p> <p>Researchers often perform hearing studies on fish in small tanks. The <span class="hlt">acoustic</span> field in such a tank is considerably different from the <span class="hlt">acoustic</span> field that occurs in the animal's natural environment. The significance of these differences is magnified by the nature of the fish's auditory system where either <span class="hlt">acoustic</span> <span class="hlt">pressure</span> (a scalar), <span class="hlt">acoustic</span> particle velocity (a vector), or both may serve as the stimulus. It is essential for the underwater acoustician to understand the <span class="hlt">acoustics</span> of small tanks to be able to carry out valid auditory research in the laboratory and to properly compare and interpret the results of others.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27652563','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27652563"><span>Holograms for <span class="hlt">acoustics</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Melde, Kai; Mark, Andrew G; Qiu, Tian; Fischer, Peer</p> <p>2016-09-22</p> <p>Holographic techniques are fundamental to applications such as volumetric displays, high-density data storage and optical tweezers that require spatial control of intricate optical or <span class="hlt">acoustic</span> fields within a three-dimensional volume. The basis of holography is spatial storage of the phase and/or amplitude profile of the desired wavefront in a manner that allows that wavefront to be reconstructed by interference when the hologram is illuminated with a suitable coherent source. Modern computer-generated holography skips the process of recording a hologram from a physical scene, and instead calculates the required phase profile before rendering it for reconstruction. In ultrasound applications, the phase profile is typically generated by discrete and independently driven ultrasound sources; however, these can only be used in small numbers, which limits the complexity or degrees of freedom that can be attained in the wavefront. Here we introduce monolithic <span class="hlt">acoustic</span> holograms, which can reconstruct diffraction-limited <span class="hlt">acoustic</span> <span class="hlt">pressure</span> fields and thus arbitrary ultrasound beams. We use rapid fabrication to craft the holograms and achieve reconstruction degrees of freedom two orders of magnitude higher than commercial phased array sources. The technique is inexpensive, appropriate for both transmission and reflection elements, and scales well to higher information content, larger aperture size and higher power. The complex three-dimensional <span class="hlt">pressure</span> and phase distributions produced by these <span class="hlt">acoustic</span> holograms allow us to demonstrate new approaches to controlled ultrasonic manipulation of solids in water, and of liquids and solids in air. We expect that <span class="hlt">acoustic</span> holograms will enable new capabilities in beam-steering and the contactless transfer of power, improve medical imaging, and drive new applications of ultrasound.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950012515','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950012515"><span><span class="hlt">Acoustic</span> properties and durability of liner materials at non-standard atmospheric conditions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ahuja, K. K.; Gaeta, R. J., Jr.; Hsu, J. S.</p> <p>1994-01-01</p> <p>This report documents the results of an experimental study on how <span class="hlt">acoustic</span> properties of certain absorbing liner materials are affected by nonstandard atmospheric conditions. This study was motivated by the need to assess risks associated with incorporating <span class="hlt">acoustic</span> testing capability in wind tunnels with semicryogenic high Reynolds number aerodynamic and/or low <span class="hlt">pressure</span> capabilities. The study consisted of three phases: 1) measurement of <span class="hlt">acoustic</span> properties of selected liner materials at subatmospheric <span class="hlt">pressure</span> conditions, 2) periodic cold soak and high <span class="hlt">pressure</span> exposure of liner materials for 250 cycles, and 3) determination of the effect of periodic cold soak on the <span class="hlt">acoustic</span> properties of the liner materials at subatmospheric conditions and the effect on mechanical resiliency. The selected liner materials were Pyrell foam, Fiberglass, and Kevlar. A vacuum facility was used to create the subatmospheric environment in which an impedance tube was placed to measure <span class="hlt">acoustic</span> properties of the test materials. An automated cryogenic cooling system was used to simulate periodic cold soak and high <span class="hlt">pressure</span> exposure. It was found that lower ambient <span class="hlt">pressure</span> reduced the absorption effectiveness of the liner materials to varying degrees. Also no significant change in the <span class="hlt">acoustic</span> properties occurred after the periodic cold soak. Furthermore, mechanical resiliency tests indicated no noticeable change.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1175891','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1175891"><span>Passive tire <span class="hlt">pressure</span> sensor and method</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Pfeifer, Kent Bryant; Williams, Robert Leslie; Waldschmidt, Robert Lee; Morgan, Catherine Hook</p> <p>2006-08-29</p> <p>A surface <span class="hlt">acoustic</span> wave device includes a micro-machined <span class="hlt">pressure</span> transducer for monitoring tire <span class="hlt">pressure</span>. The device is configured having a micro-machined cavity that is sealed with a flexible conductive membrane. When an external tire <span class="hlt">pressure</span> equivalent to the cavity <span class="hlt">pressure</span> is detected, the membrane makes contact with ridges on the backside of the surface <span class="hlt">acoustic</span> wave device. The ridges are electrically connected to conductive fingers of the device. When the detected <span class="hlt">pressure</span> is correct, selected fingers on the device will be grounded producing patterned <span class="hlt">acoustic</span> reflections to an impulse RF signal. When the external tire <span class="hlt">pressure</span> is less than the cavity reference <span class="hlt">pressure</span>, a reduced reflected signal to the receiver results. The sensor may further be constructed so as to identify itself by a unique reflected identification pulse series.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/914716','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/914716"><span>Passive tire <span class="hlt">pressure</span> sensor and method</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Pfeifer, Kent Bryant; Williams, Robert Leslie; Waldschmidt, Robert Lee; Morgan, Catherine Hook</p> <p>2007-09-04</p> <p>A surface <span class="hlt">acoustic</span> wave device includes a micro-machined <span class="hlt">pressure</span> transducer for monitoring tire <span class="hlt">pressure</span>. The device is configured having a micro-machined cavity that is sealed with a flexible conductive membrane. When an external tire <span class="hlt">pressure</span> equivalent to the cavity <span class="hlt">pressure</span> is detected, the membrane makes contact with ridges on the backside of the surface <span class="hlt">acoustic</span> wave device. The ridges are electrically connected to conductive fingers of the device. When the detected <span class="hlt">pressure</span> is correct, selected fingers on the device will be grounded producing patterned <span class="hlt">acoustic</span> reflections to an impulse RF signal. When the external tire <span class="hlt">pressure</span> is less than the cavity reference <span class="hlt">pressure</span>, a reduced reflected signal to the receiver results. The sensor may further be constructed so as to identify itself by a unique reflected identification pulse series.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050220576','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050220576"><span>Electrochemical Processes Enhanced by <span class="hlt">Acoustic</span> Liquid Manipulation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Oeftering, Richard C.</p> <p>2004-01-01</p> <p><span class="hlt">Acoustic</span> liquid manipulation is a family of techniques that employ the nonlinear <span class="hlt">acoustic</span> effects of <span class="hlt">acoustic</span> radiation <span class="hlt">pressure</span> and <span class="hlt">acoustic</span> streaming to manipulate the behavior of liquids. Researchers at the NASA Glenn Research Center are exploring new methods of manipulating liquids for a variety of space applications, and we have found that <span class="hlt">acoustic</span> techniques may also be used in the normal Earth gravity environment to enhance the performance of existing fluid processes. Working in concert with the NASA Commercial Technology Office, the Great Lakes Industrial Technology Center, and Alchemitron Corporation (Elgin, IL), researchers at Glenn have applied nonlinear <span class="hlt">acoustic</span> principles to industrial applications. Collaborating with Alchemitron Corporation, we have adapted the devices to create <span class="hlt">acoustic</span> streaming in a conventional electroplating process.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24296292','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24296292"><span>Very high <span class="hlt">pressure</span> liquid chromatography using fully porous particles: quantitative analysis of fast <span class="hlt">gradient</span> separations without post-run times.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Stankovich, Joseph J; Gritti, Fabrice; Stevenson, Paul G; Beaver, Lois Ann; Guiochon, Georges</p> <p>2014-01-10</p> <p>Using a column packed with fully porous particles, four methods for controlling the flow rates at which <span class="hlt">gradient</span> elution runs are conducted in very high <span class="hlt">pressure</span> liquid chromatography (VHPLC) were tested to determine whether reproducible thermal conditions could be achieved, such that subsequent analyses would proceed at nearly the same initial temperature. In VHPLC high flow rates are achieved, producing fast analyses but requiring high inlet <span class="hlt">pressures</span>. The combination of high flow rates and high inlet <span class="hlt">pressures</span> generates local heat, leading to temperature changes in the column. Usually in this case a post-run time is input into the analytical method to allow the return of the column temperature to its initial state. An alternative strategy involves operating the column without a post-run equilibration period and maintaining constant temperature variations for subsequent analysis after conducting one or a few separations to bring the column to a reproducible starting temperature. A liquid chromatography instrument equipped with a <span class="hlt">pressure</span> controller was used to perform constant <span class="hlt">pressure</span> and constant flow rate VHPLC separations. Six replicate <span class="hlt">gradient</span> separations of a nine component mixture consisting of acetophenone, propiophenone, butyrophenone, valerophenone, hexanophenone, heptanophenone, octanophenone, benzophenone, and acetanilide dissolved in water/acetonitrile (65:35, v/v) were performed under various experimental conditions: constant flow rate, two sets of constant <span class="hlt">pressure</span>, and constant <span class="hlt">pressure</span> operation with a programmed flow rate. The relative standard deviations of the response factors for all the analytes are lower than 5% across the methods. Programming the flow rate to maintain a fairly constant <span class="hlt">pressure</span> instead of using instrument controlled constant <span class="hlt">pressure</span> improves the reproducibility of the retention times by a factor of 5, when plotting the chromatograms in time. Copyright © 2013 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70034727','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70034727"><span><span class="hlt">Pressure-gradient</span>-driven nearshore circulation on a beach influenced by a large inlet-tidal shoal system</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Shi, F.; Hanes, D.M.; Kirby, J.T.; Erikson, L.; Barnard, P.; Eshleman, J.</p> <p>2011-01-01</p> <p>The nearshore circulation induced by a focused pattern of surface gravity waves is studied at a beach adjacent to a major inlet with a large ebb tidal shoal. Using a coupled wave and wave-averaged nearshore circulation model, it is found that the nearshore circulation is significantly affected by the heterogeneous wave patterns caused by wave refraction over the ebb tidal shoal. The model is used to predict waves and currents during field experiments conducted near the mouth of San Francisco Bay and nearby Ocean Beach. The field measurements indicate strong spatial variations in current magnitude and direction and in wave height and direction along Ocean Beach and across the ebb tidal shoal. Numerical simulations suggest that wave refraction over the ebb tidal shoal causes wave focusing toward a narrow region at Ocean Beach. Due to the resulting spatial variation in nearshore wave height, wave-induced setup exhibits a strong alongshore nonuniformity, resulting in a dramatic change in the <span class="hlt">pressure</span> field compared to a simulation with only tidal forcing. The analysis of momentum balances inside the surf zone shows that, under wave conditions with intensive wave focusing, the alongshore <span class="hlt">pressure</span> <span class="hlt">gradient</span> associated with alongshore nonuniform wave setup can be a dominant force driving circulation, inducing heterogeneous alongshore currents. <span class="hlt">Pressure-gradient</span>- forced alongshore currents can exhibit flow reversals and flow convergence or divergence, in contrast to the uniform alongshore currents typically caused by tides or homogeneous waves.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4822701','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4822701"><span>Conditionally Increased <span class="hlt">Acoustic</span> <span class="hlt">Pressures</span> in Nonfetal Diagnostic Ultrasound Examinations Without Contrast Agents: A Preliminary Assessment</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Nightingale, Kathryn R.; Church, Charles C.; Harris, Gerald; Wear, Keith A.; Bailey, Michael R.; Carson, Paul L.; Jiang, Hui; Sandstrom, Kurt L.; Szabo, Thomas L.; Ziskin, Marvin C.</p> <p>2016-01-01</p> <p>The mechanical index (MI) has been used by the US Food and Drug Administration (FDA) since 1992 for regulatory decisions regarding the <span class="hlt">acoustic</span> output of diagnostic ultrasound equipment. Its formula is based on predictions of <span class="hlt">acoustic</span> cavitation under specific conditions. Since its implementation over 2 decades ago, new imaging modes have been developed that employ unique beam sequences exploiting higher-order <span class="hlt">acoustic</span> phenomena, and, concurrently, studies of the bioeffects of ultrasound under a range of imaging scenarios have been conducted. In 2012, the American Institute of Ultrasound in Medicine Technical Standards Committee convened a working group of its Output Standards Subcommittee to examine and report on the potential risks and benefits of the use of conditionally increased <span class="hlt">acoustic</span> <span class="hlt">pressures</span> (CIP) under specific diagnostic imaging scenarios. The term “conditionally” is included to indicate that CIP would be considered on a per-patient basis for the duration required to obtain the necessary diagnostic information. This document is a result of that effort. In summary, a fundamental assumption in the MI calculation is the presence of a preexisting gas body. For tissues not known to contain preexisting gas bodies, based on theoretical predications and experimentally reported cavitation thresholds, we find this assumption to be invalid. We thus conclude that exceeding the recommended maximum MI level given in the FDA guidance could be warranted without concern for increased risk of cavitation in these tissues. However, there is limited literature assessing the potential clinical benefit of exceeding the MI guidelines in these tissues. The report proposes a 3-tiered approach for CIP that follows the model for employing elevated output in magnetic resonance imaging and concludes with summary recommendations to facilitate Institutional Review Board (IRB)-monitored clinical studies investigating CIP in specific tissues. PMID:26112617</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26112617','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26112617"><span>Conditionally Increased <span class="hlt">Acoustic</span> <span class="hlt">Pressures</span> in Nonfetal Diagnostic Ultrasound Examinations Without Contrast Agents: A Preliminary Assessment.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nightingale, Kathryn R; Church, Charles C; Harris, Gerald; Wear, Keith A; Bailey, Michael R; Carson, Paul L; Jiang, Hui; Sandstrom, Kurt L; Szabo, Thomas L; Ziskin, Marvin C</p> <p>2015-07-01</p> <p>The mechanical index (MI) has been used by the US Food and Drug Administration (FDA) since 1992 for regulatory decisions regarding the <span class="hlt">acoustic</span> output of diagnostic ultrasound equipment. Its formula is based on predictions of <span class="hlt">acoustic</span> cavitation under specific conditions. Since its implementation over 2 decades ago, new imaging modes have been developed that employ unique beam sequences exploiting higher-order <span class="hlt">acoustic</span> phenomena, and, concurrently, studies of the bioeffects of ultrasound under a range of imaging scenarios have been conducted. In 2012, the American Institute of Ultrasound in Medicine Technical Standards Committee convened a working group of its Output Standards Subcommittee to examine and report on the potential risks and benefits of the use of conditionally increased <span class="hlt">acoustic</span> <span class="hlt">pressures</span> (CIP) under specific diagnostic imaging scenarios. The term "conditionally" is included to indicate that CIP would be considered on a per-patient basis for the duration required to obtain the necessary diagnostic information. This document is a result of that effort. In summary, a fundamental assumption in the MI calculation is the presence of a preexisting gas body. For tissues not known to contain preexisting gas bodies, based on theoretical predications and experimentally reported cavitation thresholds, we find this assumption to be invalid. We thus conclude that exceeding the recommended maximum MI level given in the FDA guidance could be warranted without concern for increased risk of cavitation in these tissues. However, there is limited literature assessing the potential clinical benefit of exceeding the MI guidelines in these tissues. The report proposes a 3-tiered approach for CIP that follows the model for employing elevated output in magnetic resonance imaging and concludes with summary recommendations to facilitate Institutional Review Board (IRB)-monitored clinical studies investigating CIP in specific tissues. © 2015 by the American Institute of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApPhL.112r3503S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApPhL.112r3503S"><span>A surface impedance-based three-channel <span class="hlt">acoustic</span> metasurface retroreflector</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shen, Chen; Díaz-Rubio, Ana; Li, Junfei; Cummer, Steven A.</p> <p>2018-04-01</p> <p>We propose the design and measurement of an <span class="hlt">acoustic</span> metasurface retroreflector that works at three discrete incident angles. An impedance model is developed such that for <span class="hlt">acoustic</span> waves impinging at -60°, the reflected wave is defined by the surface impedance of the metasurface, which is realized by a periodic grating. At 0° and 60°, the retroreflection condition can be fulfilled by the diffraction of the surface. The thickness of the metasurface is about half of the operating wavelength and the retroreflector functions without parasitic diffraction associated with conventional <span class="hlt">gradient</span>-index metasurfaces. Such highly efficient and compact retroreflectors open up possibilities in metamaterial-based <span class="hlt">acoustic</span> sensing and communications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005ApPhL..87r4107L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005ApPhL..87r4107L"><span>Observation of ice nucleation in <span class="hlt">acoustically</span> levitated water drops</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lü, Y. J.; Xie, W. J.; Wei, B.</p> <p>2005-10-01</p> <p>The supercooling and nucleation of <span class="hlt">acoustically</span> levitated water drops were investigated at two different sound <span class="hlt">pressure</span> levels (SPL). These water drops were supercooled by 13to16K at the low SPL of 160.6dB, whereas their supercoolings varied from 5to11K at the high SPL of 164.4dB. The maximum supercooling obtained in the experiments is 32K. Statistical analyses based on the classical nucleation theory reveal that the occurrence of ice nucleation in water drops is mainly confined to the surface region under <span class="hlt">acoustic</span> levitation conditions and the enlargement of drop surface area caused by the <span class="hlt">acoustic</span> radiation <span class="hlt">pressure</span> reduces water supercoolability remarkably. A comparison of the nucleation rates at the two SPLs indicates that the sound <span class="hlt">pressure</span> can strengthen the surface-dominated nucleation of water drops. The <span class="hlt">acoustic</span> stream around levitated water drops and the cavitation effect associated with ultrasonic field are the main factors that induce surface-dominated nucleation.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_19 --> <div id="page_20" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="381"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22494742-acoustic-travel-time-gauges-situ-determination-pressure-temperature-multi-anvil-apparatus','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22494742-acoustic-travel-time-gauges-situ-determination-pressure-temperature-multi-anvil-apparatus"><span><span class="hlt">Acoustic</span> travel time gauges for in-situ determination of <span class="hlt">pressure</span> and temperature in multi-anvil apparatus</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, Xuebing; Chen, Ting; Qi, Xintong</p> <p></p> <p>In this study, we developed a new method for in-situ <span class="hlt">pressure</span> determination in multi-anvil, high-<span class="hlt">pressure</span> apparatus using an <span class="hlt">acoustic</span> travel time approach within the framework of acoustoelasticity. The ultrasonic travel times of polycrystalline Al{sub 2}O{sub 3} were calibrated against NaCl <span class="hlt">pressure</span> scale up to 15 GPa and 900 °C in a Kawai-type double-stage multi-anvil apparatus in conjunction with synchrotron X-radiation, thereby providing a convenient and reliable gauge for <span class="hlt">pressure</span> determination at ambient and high temperatures. The <span class="hlt">pressures</span> derived from this new travel time method are in excellent agreement with those from the fixed-point methods. Application of this new <span class="hlt">pressure</span> gauge in anmore » offline experiment revealed a remarkable agreement of the densities of coesite with those from the previous single crystal compression studies under hydrostatic conditions, thus providing strong validation for the current travel time <span class="hlt">pressure</span> scale. The travel time approach not only can be used for continuous in-situ <span class="hlt">pressure</span> determination at room temperature, high temperatures, during compression and decompression, but also bears a unique capability that none of the previous scales can deliver, i.e., simultaneous <span class="hlt">pressure</span> and temperature determination with a high accuracy (±0.16 GPa in <span class="hlt">pressure</span> and ±17 °C in temperature). Therefore, the new in-situ Al{sub 2}O{sub 3} <span class="hlt">pressure</span> gauge is expected to enable new and expanded opportunities for offline laboratory studies of solid and liquid materials under high <span class="hlt">pressure</span> and high temperature in multi-anvil apparatus.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19830005115','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19830005115"><span>Analysis of an existing experiment on the interaction of <span class="hlt">acoustic</span> waves with a laminar boundary layer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schopper, M. R.</p> <p>1982-01-01</p> <p>The hot-wire anemometer amplitude data contained in the 1977 report of P. J. Shapiro entitled, ""The Influence of Sound Upon Laminar Boundary'' were reevaluated. Because the low-Reynolds number boundary layer disturbance data were misinterpreted, an effort was made to improve the corresponding disturbance growth rate curves. The data are modeled as the sum of upstream and downstream propagating <span class="hlt">acoustic</span> waves and a wave representing the Tollmien-Schlichting (TS) wave. The amplitude and phase velocity of the latter wave were then adjusted so that the total signal reasonably matched the amplitude and phase angle hot-wire data along the plate laminar boundary layer. The revised rates show growth occurring further upstream than Shapiro found. It appears that the premature growth is due to the adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> created by the shape of the plate. Basic elements of sound propagation in ducts and the experimental and theoretical <span class="hlt">acoustic</span>-stability literature are reviewed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhPl...25b4502M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhPl...25b4502M"><span>Degenerate <span class="hlt">pressure</span> driven modified nucleus-<span class="hlt">acoustic</span> waves in degenerate plasmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mamun, A. A.</p> <p>2018-02-01</p> <p>The existence of degenerate <span class="hlt">pressure</span> driven modified nucleus-<span class="hlt">acoustic</span> (DPDMNA) waves propagating in a cold degenerate quantum plasma (DQP) system [containing cold inertialess degenerate electron species (DES), cold inertial non-degenerate light nucleus species (LNS), and stationary heavy nucleus species (HNS)] is predicted for the first time. The DPDMNA waves (in which the mass density of the cold LNS provides the inertia and the cold inertialess DES gives rise to the restoring force) are new since they completely disappear if the degenerate <span class="hlt">pressure</span> of the cold DES is neglected. It is found that the phase speed (Vp) of the DPDMNA waves decreases with the rise of the charge number density of the stationary HNS for both non-relativistic and ultra-relativistic DES, and that the ultra-relativistic DES does not have any effect on Vp when β = 1, where β = Λc/Λe with Λ e = ne 0 - 1 / 3 being the average inter-electron distance in the DQP system and Λc being the constant (˜10-10 cm) for the DES. However, the ultra-relativistic DES does have quite a significant effect on Vp for β ≫ 1 and β ≪ 1, and the ultra-relativistic effect significantly enhances (reduces) Vp for β ≫ 1 (β ≪ 1). The DPDMNA waves and their dispersion properties are expected to be useful in understanding the basic features of the electrostatic perturbation mode in space and laboratory DQP systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1066816','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1066816"><span>Ultrasonic <span class="hlt">Acoustic</span> Emissions from the Sapwood of Thuja occidentalis Measured inside a <span class="hlt">Pressure</span> Bomb 1</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Tyree, Melvin T.; Dixon, Michael A.; Thompson, Robert G.</p> <p>1984-01-01</p> <p>An improved method of counting <span class="hlt">acoustic</span> emission (AE) events from water-stressed stems of cedar (Thuja occidentalis L.) is presented. Amplified AEs are analyzed on a real time basis by a microcomputer. The instrumentation counts AE events in a fashion nearly analogous to scintillation counting of radioactive materials. The technique was applied to measuring ultrasonic AEs from the stems of cedar inside a <span class="hlt">pressure</span> bomb. The shoots were originally fully hydrated. When the shoots are dehydrated in the bomb by application of an overpressure very few AEs were detected. When the bomb <span class="hlt">pressure</span> is reduced after dehydration of the shoot, AE events could be detected. We conclude that ultrasonic AEs are caused by cavitation events (= structural breakdown of water columns in the tracheids of cedar) and not by the breaking of cellulose fibers in the wood. PMID:16663501</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JSV...329.2276D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JSV...329.2276D"><span>Prediction of the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> above periodically uneven facings in industrial workplaces</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ducourneau, J.; Bos, L.; Planeau, V.; Faiz, Adil; Skali Lami, Salah; Nejade, A.</p> <p>2010-05-01</p> <p>The aim of this work is to predict sound <span class="hlt">pressure</span> in front of wall facings based on periodic sound scattering surface profiles. The method involves investigating plane wave reflections randomly incident upon an uneven surface. The waveguide approach is well suited to the geometries usually encountered in industrial workplaces. This method simplifies the profile geometry by using elementary rectangular volumes. The <span class="hlt">acoustic</span> field in the profile interstices can then be expressed as the superposition of waveguide modes. In past work, walls considered are of infinite dimensions and are subjected to a periodic surface profile in only one direction. We therefore generalise this approach by extending its applicability to "double-periodic" wall facings. Free-field measurements have been taken and the observed agreement between numerical and experimental results supports the validity of the waveguide method.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950018487','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950018487"><span>Numerical simulation of the nonlinear response of composite plates under combined thermal and <span class="hlt">acoustic</span> loading</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mei, Chuh; Moorthy, Jayashree</p> <p>1995-01-01</p> <p>A time-domain study of the random response of a laminated plate subjected to combined <span class="hlt">acoustic</span> and thermal loads is carried out. The features of this problem also include given uniform static inplane forces. The formulation takes into consideration a possible initial imperfection in the flatness of the plate. High decibel sound <span class="hlt">pressure</span> levels along with high thermal <span class="hlt">gradients</span> across thickness drive the plate response into nonlinear regimes. This calls for the analysis to use von Karman large deflection strain-displacement relationships. A finite element model that combines the von Karman strains with the first-order shear deformation plate theory is developed. The development of the analytical model can accommodate an anisotropic composite laminate built up of uniformly thick layers of orthotropic, linearly elastic laminae. The global system of finite element equations is then reduced to a modal system of equations. Numerical simulation using a single-step algorithm in the time-domain is then carried out to solve for the modal coordinates. Nonlinear algebraic equations within each time-step are solved by the Newton-Raphson method. The random gaussian filtered white noise load is generated using Monte Carlo simulation. The <span class="hlt">acoustic</span> <span class="hlt">pressure</span> distribution over the plate is capable of accounting for a grazing incidence wavefront. Numerical results are presented to study a variety of cases.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29137774','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29137774"><span>Influence of reactions heats on variation of radius, temperature, <span class="hlt">pressure</span> and chemical species amounts within a single <span class="hlt">acoustic</span> cavitation bubble.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kerboua, Kaouther; Hamdaoui, Oualid</p> <p>2018-03-01</p> <p>The scientific interest toward the study of <span class="hlt">acoustic</span> bubble is mainly explained by its practical benefit in providing a reactional media favorable to the rapid evolution of chemical mechanism. The evolution of this mechanism is related to the simultaneous and dependent variation of the volume, temperature and <span class="hlt">pressure</span> within the bubble, retrieved by the resolution of a differential equations system, including among others the thermal balance. This last one is subject to different assumptions, some authors deem simply that the temperature varies adiabatically during the collapsing phase, without considering the reactions heat of the studied mechanism. This paper aims to evaluate the pertinence of neglecting reactions heats in the thermal balance, by analyzing their effect on the variation of radius, temperature, <span class="hlt">pressure</span> and chemical species amounts. The results show that the introduction of reactions heats conducts to a decrease of the temperature, an increase of the <span class="hlt">pressure</span> and a reduction of the bubble volume. As a consequence, this leads to a drop of the quantities of free radicals produced by the chemical mechanism evolving within the bubble. This paper also proved that the impact of the consideration of reactions heats is dependent of the frequency and the <span class="hlt">acoustic</span> amplitude of the ultrasonic wave. Copyright © 2017 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014NatCo...5E4316Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014NatCo...5E4316Z"><span>Generation of <span class="hlt">acoustic</span> self-bending and bottle beams by phase engineering</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Peng; Li, Tongcang; Zhu, Jie; Zhu, Xuefeng; Yang, Sui; Wang, Yuan; Yin, Xiaobo; Zhang, Xiang</p> <p>2014-07-01</p> <p>Directing <span class="hlt">acoustic</span> waves along curved paths is critical for applications such as ultrasound imaging, surgery and <span class="hlt">acoustic</span> cloaking. Metamaterials can direct waves by spatially varying the material properties through which the wave propagates. However, this approach is not always feasible, particularly for <span class="hlt">acoustic</span> applications. Here we demonstrate the generation of <span class="hlt">acoustic</span> bottle beams in homogeneous space without using metamaterials. Instead, the sound energy flows through a three-dimensional curved shell in air leaving a close-to-zero <span class="hlt">pressure</span> region in the middle, exhibiting the capability of circumventing obstacles. By designing the initial phase, we develop a general recipe for creating self-bending wave packets, which can set <span class="hlt">acoustic</span> beams propagating along arbitrary prescribed convex trajectories. The measured <span class="hlt">acoustic</span> pulling force experienced by a rigid ball placed inside such a beam confirms the <span class="hlt">pressure</span> field of the bottle. The demonstrated <span class="hlt">acoustic</span> bottle and self-bending beams have potential applications in medical ultrasound imaging, therapeutic ultrasound, as well as <span class="hlt">acoustic</span> levitations and isolations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850039818&hterms=stress+relationship&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dstress%2Brelationship','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850039818&hterms=stress+relationship&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dstress%2Brelationship"><span><span class="hlt">Acoustic</span>-radiation stress in solids. I - Theory</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cantrell, J. H., Jr.</p> <p>1984-01-01</p> <p>The general case of <span class="hlt">acoustic</span>-radiation stress associated with quasi-compressional and quasi-shear waves propagating in infinite and semiinfinite lossless solids of arbitrary crystalline symmetry is studied. The Boussinesq radiation stress is defined and found to depend directly on an <span class="hlt">acoustic</span> nonlinearity parameter which characterizes the radiation-induced static strain, a stress-generalized nonlinearity parameter which characterizes the stress nonlinearity, and the energy density of the propagating wave. Application of the Boltzmann-Ehrenfest principle of adiabatic invariance to a self-constrained system described by the nonlinear equations of motion allows the <span class="hlt">acoustic</span>-radiation-induced static strain to be identified with a self-constrained variation in the time-averaged product of the internal energy density and displacement <span class="hlt">gradient</span>. The time-averaged product is scaled by the <span class="hlt">acoustic</span> nonlinearity parameter and represents the first-order nonlinearity in the virial theorem. Finally, the relationship between the Boussinesq and the Cauchy radiation stress is obtained in a closed three-dimensional form.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DFD.R1002S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DFD.R1002S"><span>Dynamics of encapsulated microbubbles for contrast ultrasound imaging and drug delivery: from <span class="hlt">pressure</span> dependent subharmonic to collapsing jet and <span class="hlt">acoustic</span> streaming</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sarkar, Kausik</p> <p>2016-11-01</p> <p>Intravenously injected microbubbles used as ultrasound contrast enhancing agents are encapsulated by a nanometer-thick layer of lipids, proteins or polymers to stabilize them against premature dissolution. Over the years, we have developed interfacial rheological models for the encapsulation and used them to characterize several contrast agents by <span class="hlt">acoustic</span> means. We will present an overview of our research emphasizing recent efforts in two directions. The first is on using subharmonic signals from the contrast microbubbles for non-invasive <span class="hlt">pressure</span> estimation. Experimental measurement and modeling show that the subharmonic signal can both increase or decrease with <span class="hlt">pressure</span> depending on frequency. Secondly, we will discuss boundary element (BEM) simulation of the collapse of an encapsulated microbubbles forming a jet near a blood vessel wall. Different rheology models of the encapsulation have been rigorously implemented in the BEM formulation. We will discuss the resulting stresses and the <span class="hlt">acoustic</span> streaming near the wall leading to sonoporation and other bioeffects. Partially supported by Natinal Science Foundation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29764373','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29764373"><span>A subclinical high tricuspid regurgitation <span class="hlt">pressure</span> <span class="hlt">gradient</span> independent of the mean pulmonary artery <span class="hlt">pressure</span> is a risk factor for the survival after living donor liver transplantation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Saragai, Yosuke; Takaki, Akinobu; Umeda, Yuzo; Matsusaki, Takashi; Yasunaka, Tetsuya; Oyama, Atsushi; Kaku, Ryuji; Nakamura, Kazufumi; Yoshida, Ryuichi; Nobuoka, Daisuke; Kuise, Takashi; Takagi, Kosei; Adachi, Takuya; Wada, Nozomu; Takeuchi, Yasuto; Koike, Kazuko; Ikeda, Fusao; Onishi, Hideki; Shiraha, Hidenori; Nakamura, Shinichiro; Morimatsu, Hiroshi; Ito, Hiroshi; Fujiwara, Toshiyoshi; Yagi, Takahito; Okada, Hiroyuki</p> <p>2018-05-15</p> <p>Portopulmonary hypertension (POPH) is characterized by pulmonary vasoconstriction, while hepatopulmonary syndrome (HPS) is characterized by vasodilation. Definite POPH is a risk factor for the survival after orthotopic liver transplantation (OLT), as the congestive <span class="hlt">pressure</span> affects the grafted liver, while subclinical pulmonary hypertension (PH) has been acknowledged as a non-risk factor for deceased donor OLT. Given that PH measurement requires cardiac catheterization, the tricuspid regurgitation <span class="hlt">pressure</span> <span class="hlt">gradient</span> (TRPG) measured by echocardiography is used to screen for PH and congestive <span class="hlt">pressure</span> to the liver. We investigated the impact of a subclinical high TRPG on the survival of small grafted living donor liver transplantation (LDLT). We retrospectively analyzed 84 LDLT candidates. Patients exhibiting a TRPG ≥25 mmHg on echocardiography were categorized as potentially having liver congestion (subclinical high TRPG; n = 34). The mean pulmonary artery <span class="hlt">pressure</span> (mPAP) measured after general anesthesia with FIO 2 0.6 (mPAP-FIO 2 0.6) was also assessed. Patients exhibiting pO 2  < 80 mmHg and an alveolar-arterial oxygen <span class="hlt">gradient</span> (AaDO 2 ) ≥ 15 mmHg were categorized as potentially having HPS (subclinical HPS; n = 29). The clinical course after LDLT was investigated according to subclinical high TRPG. A subclinical high TRPG (p = 0.012) and older donor age (p = 0.008) were correlated with a poor 40-month survival. Although a higher mPAP-FIO 2 0.6 was expected to correlate with a worse survival, a high mPAP-FIO 2 0.6 with a low TRPG was associated with high frequency complicating subclinical HPS and a good survival, suggesting a reduction in the PH <span class="hlt">pressure</span> via pulmonary shunt. In cirrhosis patients, mPAP-FIO 2 0.6 may not accurately reflect the congestive <span class="hlt">pressure</span> to the liver, as the <span class="hlt">pressure</span> might escape via pulmonary shunt. A subclinical high TRPG is an important marker for predicting a worse survival after LDLT, possibly reflecting</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910054344&hterms=Acoustic+levitation&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DAcoustic%2Blevitation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910054344&hterms=Acoustic+levitation&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DAcoustic%2Blevitation"><span><span class="hlt">Acoustic</span> levitation for high temperature containerless processing in space</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rey, C. A.; Sisler, R.; Merkley, D. R.; Danley, T. J.</p> <p>1990-01-01</p> <p>New facilities for high-temperature containerless processing in space are described, including the <span class="hlt">acoustic</span> levitation furnace (ALF), the high-temperature <span class="hlt">acoustic</span> levitator (HAL), and the high-<span class="hlt">pressure</span> <span class="hlt">acoustic</span> levitator (HPAL). In the current ALF development, the maximum temperature capabilities of the levitation furnaces are 1750 C, and in the HAL development with a cold wall furnace they will exceed 2000-2500 C. The HPAL demonstrated feasibility of precursor space flight experiments on the ground in a 1 g <span class="hlt">pressurized</span>-gas environment. Testing of lower density materials up to 1300 C has also been accomplished. It is suggested that advances in <span class="hlt">acoustic</span> levitation techniques will result in the production of new materials such as ceramics, alloys, and optical and electronic materials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3880383','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3880383"><span>A <span class="hlt">pressure-gradient</span> mechanism for vortex shedding in constricted channels</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Boghosian, M. E.; Cassel, K. W.</p> <p>2013-01-01</p> <p>Numerical simulations of the unsteady, two-dimensional, incompressible Navier–Stokes equations are performed for a Newtonian fluid in a channel having a symmetric constriction modeled by a two-parameter Gaussian distribution on both channel walls. The Reynolds number based on inlet half-channel height and mean inlet velocity ranges from 1 to 3000. Constriction ratios based on the half-channel height of 0.25, 0.5, and 0.75 are considered. The results show that both the Reynolds number and constriction geometry have a significant effect on the behavior of the post-constriction flow field. The Navier–Stokes solutions are observed to experience a number of bifurcations: steady attached flow, steady separated flow (symmetric and asymmetric), and unsteady vortex shedding downstream of the constriction depending on the Reynolds number and constriction ratio. A sequence of events is described showing how a sustained spatially growing flow instability, reminiscent of a convective instability, leads to the vortex shedding phenomenon via a proposed streamwise <span class="hlt">pressure-gradient</span> mechanism. PMID:24399860</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6548360-assessment-stenosis-severity-correlation-angiography-t1-scintigraphy-intracoronary-pressure-gradients','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6548360-assessment-stenosis-severity-correlation-angiography-t1-scintigraphy-intracoronary-pressure-gradients"><span>Assessment of stenosis severity: Correlation of angiography, T1-201 scintigraphy, and intracoronary <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Bateman, T.; Raymond, M.; Czer, L.</p> <p>1984-01-01</p> <p>To clarify the relationship between angiographic and hemodynamic stenosis severity and the appearance during stress-redistribution myocardial T1-201 scintigraphy (Ex-T1) of a visual (V) or quantitative (Q) perfusion defect (PD) or washout (WO) abnormality, 24 pts with CAD underwent intracoronary <span class="hlt">pressure</span> <span class="hlt">gradient</span> study at bypass surgery (CABG). All had pre-CABG Ex-T1 without interval deterioration. The mean diastolic <span class="hlt">pressure</span> <span class="hlt">gradient</span> (MDG) measured at reproducible hyperemic flow rates was determined for 34 stenoses (13 LAD, 7 LCX, 14 RCA) and compared with the results of Ex-T1 in subtended myocardial regions (LAD=anterior; LCX=posterolateral; RCA=inferior). Fourteen stenoses (50-99% diameter narrowing) were unassociated with VPD despitemore » maximal exercise: MDG was 9 +- 5mmHg, with MDG/mean aortic diastolic <span class="hlt">pressure</span> (ADP) ratio of 0.12 +- 0.07. QPD and QWO analysis detected 8 of these. Thirteen stenoses (90-100% severity) led to reversible VPD: MDG was 36 +- 11 mm Hg, MDG/ADP ratio was 0.52 +- 0.17, and Q analysis was abnormal in 12/13. Seven stenoses (90-100% severity) subtended infarcted myocardium: MDG was 42 +- 21 mm Hg, MDG/ADP ratio was 0.52 +- 0.18, and V and Q analyses were abnormal in all. From this study, the authors derive the following conclusion: 1) Ex-T1 correlates better with hemodynamic severity of stenoses than does angiography; 2) V abnormalities identify stenoses of major angiographic and hemodynamic severity, while Q analysis detects some (57% in this study) stenoses of lesser severity; and 3) stenoses causing reversible Ex-T1 abnormalities present similar hemodynamic impediments to those causing myocardial infarcts.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24606249','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24606249"><span>Experimental study on inter-particle <span class="hlt">acoustic</span> forces.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Garcia-Sabaté, Anna; Castro, Angélica; Hoyos, Mauricio; González-Cinca, Ricard</p> <p>2014-03-01</p> <p>A method for the experimental measurement of inter-particle forces (secondary Bjerknes force) generated by the action of an <span class="hlt">acoustic</span> field in a resonator micro-channel is presented. The <span class="hlt">acoustic</span> radiation force created by an ultrasonic standing wave moves suspended particles towards the <span class="hlt">pressure</span> nodes and the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> induces particle volume oscillations. Once particles are in the levitation plane, transverse and secondary Bjerknes forces become important. Experiments were carried out in a resonator filled with a suspension composed of water and latex particles of different size (5-15 μm) at different concentrations. Ultrasound was generated by means of a 2.5 MHz nominal frequency transducer. For the first time the <span class="hlt">acoustic</span> force generated by oscillating particles acting on other particles has been measured, and the critical interaction distance in various cases has been determined. Inter-particle forces on the order of 10(-14) N have been measured by using this method.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730012553','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730012553"><span>The behavior of a compressible turbulent boundary layer in a shock-wave-induced adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span>. Ph.D. Thesis - Washington Univ., Seattle, Aug. 1972</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rose, W. C.</p> <p>1973-01-01</p> <p>The results of an experimental investigation of the mean- and fluctuating-flow properties of a compressible turbulent boundary layer in a shock-wave-induced adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> are presented. The turbulent boundary layer developed on the wall of an axially symmetric nozzle and test section whose nominal free-stream Mach number and boundary-layer thickness Reynolds number were 4 and 100,000, respectively. The adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> was induced by an externally generated conical shock wave. Mean and time-averaged fluctuating-flow data, including the complete experimental Reynolds stress tensor and experimental turbulent mass- and heat-transfer rates are presented for the boundary layer and external flow, upstream, within and downstream of the <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The mean-flow data include distributions of total temperature throughout the region of interest. The turbulent mixing properties of the flow were determined experimentally with a hot-wire anemometer. The calibration of the wires and the interpretation of the data are discussed. From the results of the investigation, it is concluded that the shock-wave - boundary-layer interaction significantly alters the turbulent mixing characteristics of the boundary layer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25920860','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25920860"><span>Analyzing panel <span class="hlt">acoustic</span> contributions toward the sound field inside the passenger compartment of a full-size automobile.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wu, Sean F; Moondra, Manmohan; Beniwal, Ravi</p> <p>2015-04-01</p> <p>The Helmholtz equation least squares (HELS)-based nearfield <span class="hlt">acoustical</span> holography (NAH) is utilized to analyze panel <span class="hlt">acoustic</span> contributions toward the <span class="hlt">acoustic</span> field inside the interior region of an automobile. Specifically, the <span class="hlt">acoustic</span> power flows from individual panels are reconstructed, and relative contributions to sound <span class="hlt">pressure</span> level and spectrum at any point of interest are calculated. Results demonstrate that by correlating the <span class="hlt">acoustic</span> power flows from individual panels to the field <span class="hlt">acoustic</span> <span class="hlt">pressure</span>, one can correctly locate the panel allowing the most <span class="hlt">acoustic</span> energy transmission into the vehicle interior. The panel on which the surface <span class="hlt">acoustic</span> <span class="hlt">pressure</span> amplitude is the highest should not be used as indicative of the panel responsible for the sound field in the vehicle passenger compartment. Another significant advantage of this HELS-based NAH is that measurements of the input data only need to be taken once by using a conformal array of microphones in the near field, and ranking of panel <span class="hlt">acoustic</span> contributions to any field point can be readily performed. The transfer functions between individual panels of any vibrating structure to the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> anywhere in space are calculated not measured, thus significantly reducing the time and effort involved in panel <span class="hlt">acoustic</span> contributions analyses.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1207283','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1207283"><span>Microfluidic device for <span class="hlt">acoustic</span> cell lysis</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>Branch, Darren W.; Cooley, Erika Jane; Smith, Gennifer Tanabe</p> <p>2015-08-04</p> <p>A microfluidic <span class="hlt">acoustic</span>-based cell lysing device that can be integrated with on-chip nucleic acid extraction. Using a bulk <span class="hlt">acoustic</span> wave (BAW) transducer array, <span class="hlt">acoustic</span> waves can be coupled into microfluidic cartridges resulting in the lysis of cells contained therein by localized <span class="hlt">acoustic</span> <span class="hlt">pressure</span>. Cellular materials can then be extracted from the lysed cells. For example, nucleic acids can be extracted from the lysate using silica-based sol-gel filled microchannels, nucleic acid binding magnetic beads, or Nafion-coated electrodes. Integration of cell lysis and nucleic acid extraction on-chip enables a small, portable system that allows for rapid analysis in the field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22617069','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22617069"><span>[Diagnostic importance of the alveolar-arterial oxygen <span class="hlt">gradient</span>].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Weinans, Marije A E; Drost-de Klerck, Amanda M; ter Maaten, Jan C</p> <p>2012-01-01</p> <p>The alveolar-arterial (A-a) oxygen <span class="hlt">gradient</span> is the difference between the partial <span class="hlt">pressure</span> of oxygen in the alveoli and the partial <span class="hlt">pressure</span> of arterial oxygen and can be elevated in the case of pulmonary disease. We describe a 41-year-old patient with pneumonia who presented with abdominal pain, in whom calculation of the A-a <span class="hlt">gradient</span> could have led to earlier diagnosis. The A-a oxygen <span class="hlt">gradient</span> is mainly of diagnostic importance and the presented nomogram allows easy and quick interpretation. This might lead to a more frequent use of the A-a oxygen <span class="hlt">gradient</span> in the future.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JSV...333.3585H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JSV...333.3585H"><span>Suppression of Helmholtz resonance using inside <span class="hlt">acoustic</span> liner</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hong, Zhiliang; Dai, Xiwen; Zhou, Nianfa; Sun, Xiaofeng; Jing, Xiaodong</p> <p>2014-08-01</p> <p>When a Helmholtz resonator is exposed to grazing flow, an unstable shear layer at the opening can cause the occurrence of <span class="hlt">acoustic</span> resonance under appropriate conditions. In this paper, in order to suppress the flow-induced resonance, the effects of inside <span class="hlt">acoustic</span> liners placed on the side wall or the bottom of a Helmholtz resonator are investigated. Based on the one-dimensional sound propagation theory, the time domain impedance model of a Helmholtz resonator with inside <span class="hlt">acoustic</span> liner is derived, and then combined with a discrete vortex model the resonant behavior of the resonator under grazing flow is simulated. Besides, an experiment is conducted to validate the present model, showing significant reduction of the peak sound <span class="hlt">pressure</span> level achieved by the use of the side-wall liners. And the simulation results match reasonably well with the experimental data. The present results reveal that the inside <span class="hlt">acoustic</span> liner can not only absorb the resonant sound <span class="hlt">pressure</span>, but also suppress the fluctuation motion of the shear layer over the opening of the resonator. In all, the impact of the <span class="hlt">acoustic</span> liners is to dampen the instability of the flow-<span class="hlt">acoustic</span> coupled system. This demonstrates that it is a convenient and effective method for suppressing Helmholtz resonance by using inside <span class="hlt">acoustic</span> liner.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_20 --> <div id="page_21" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="401"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19880012911','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19880012911"><span>Enhanced viscous flow drag reduction using <span class="hlt">acoustic</span> excitation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nagel, R. T.</p> <p>1988-01-01</p> <p>Large eddy break up devices (LEBUs) constitute a promising method of obtaining drag reduction in a turbulent boundary layer. Enhancement of the LEBU effectiveness by exciting its trailing edge with <span class="hlt">acoustic</span> waves phase locked to the large scale structure influencing the momentum transfer to the wall is sought. An initial estimate of the required sound <span class="hlt">pressure</span> level for an effective pulse was obtained by considering the magnitude of the <span class="hlt">pressure</span> perturbations at the near wake of a thin plate in inviscid flow. Detailed skin friction measurments were obtained in the flow region downstream of a LEBU excited with <span class="hlt">acoustic</span> waves. The data are compared with skin friction measurements of a simply manipulated flow, without <span class="hlt">acoustic</span> excitation and with a plain flow configuration. The properties and the scales of motion in the flow regime downstream of the <span class="hlt">acoustically</span> excited LEBU are studied. A parametric study based upon the characteristics of the <span class="hlt">acoustic</span> input was pursued in addition to the careful mapping of the drag reduction phenomenon within the <span class="hlt">acoustically</span> manipulated boundary layer. This study of boundary layer manipulation has lead to improved skin friction drag reduction and further understanding of the turbulent boundary layer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900014354','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900014354"><span>Aerodynamic <span class="hlt">pressure</span> and heating-rate distributions in tile gaps around chine regions with <span class="hlt">pressure</span> <span class="hlt">gradients</span> at a Mach number of 6.6</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hunt, L. Roane; Notestine, Kristopher K.</p> <p>1990-01-01</p> <p>Surface and gap <span class="hlt">pressures</span> and heating-rate distributions were obtained for simulated Thermal Protection System (TPS) tile arrays on the curved surface test apparatus of the Langley 8-Foot High Temperature Tunnel at Mach 6.6. The results indicated that the chine gap <span class="hlt">pressures</span> varied inversely with gap width because larger gap widths allowed greater venting from the gap to the lower model side <span class="hlt">pressures</span>. Lower gap <span class="hlt">pressures</span> caused greater flow ingress from the surface and increased gap heating. Generally, gap heating was greater in the longitudinal gaps than in the circumferential gaps. Gap heating decreased with increasing gap depth. Circumferential gap heating at the mid-depth was generally less than about 10 percent of the external surface value. Gap heating was most severe at local T-gap junctions and tile-to-tile forward-facing steps that caused the greatest heating from flow impingement. The use of flow stoppers at discrete locations reduced heating from flow impingement. The use of flow stoppers at discrete locations reduced heating in most gaps but increased heating in others. Limited use of flow stoppers or gap filler in longitudinal gaps could reduce gap heating in open circumferential gaps in regions of high surface <span class="hlt">pressure</span> <span class="hlt">gradients</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3635164','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3635164"><span>Investigating Individual- and Area-Level Socioeconomic <span class="hlt">Gradients</span> of Pulse <span class="hlt">Pressure</span> among Normotensive and Hypertensive Participants</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Matricciani, Lisa A.; Paquet, Catherine; Howard, Natasha J.; Adams, Robert; Coffee, Neil T.; Taylor, Anne W.; Daniel, Mark</p> <p>2013-01-01</p> <p>Socioeconomic status is a strong predictor of cardiovascular disease. Pulse <span class="hlt">pressure</span>, the difference between systolic and diastolic blood <span class="hlt">pressure</span>, has been identified as an important predictor of cardiovascular risk even after accounting for absolute measures of blood <span class="hlt">pressure</span>. However, little is known about the social determinants of pulse <span class="hlt">pressure</span>. The aim of this study was to examine individual- and area-level socioeconomic <span class="hlt">gradients</span> of pulse <span class="hlt">pressure</span> in a sample of 2,789 Australian adults. Using data from the North West Adelaide Health Study we estimated the association between pulse <span class="hlt">pressure</span> and three indices of socioeconomic status (education, income and employment status) at the area and individual level for hypertensive and normotensive participants, using Generalized Estimating Equations. In normotensive individuals, area-level education (estimate: −0.106; 95% CI: −0.172, −0.041) and individual-level income (estimate: −1.204; 95% CI: −2.357, −0.050) and employment status (estimate: −1.971; 95% CI: −2.894, −1.048) were significant predictors of pulse <span class="hlt">pressure</span>, even after accounting for the use of medication and lifestyle behaviors. In hypertensive individuals, only individual-level measures of socioeconomic status were significant predictors of pulse <span class="hlt">pressure</span> (education estimate: −2.618; 95% CI: −4.878, −0.357; income estimate: −1.683, 95% CI: −3.743, 0.377; employment estimate: −2.023; 95% CI: −3.721, −0.326). Further research is needed to better understand how individual- and area-level socioeconomic status influences pulse <span class="hlt">pressure</span> in normotensive and hypertensive individuals. PMID:23380912</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2753615','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2753615"><span>Reconstruction of Vectorial <span class="hlt">Acoustic</span> Sources in Time-Domain Tomography</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Xia, Rongmin; Li, Xu; He, Bin</p> <p>2009-01-01</p> <p>A new theory is proposed for the reconstruction of curl-free vector field, whose divergence serves as <span class="hlt">acoustic</span> source. The theory is applied to reconstruct vector <span class="hlt">acoustic</span> sources from the scalar <span class="hlt">acoustic</span> signals measured on a surface enclosing the source area. It is shown that, under certain conditions, the scalar <span class="hlt">acoustic</span> measurements can be vectorized according to the known measurement geometry and subsequently be used to reconstruct the original vector field. Theoretically, this method extends the application domain of the existing <span class="hlt">acoustic</span> reciprocity principle from a scalar field to a vector field, indicating that the stimulating vectorial source and the transmitted <span class="hlt">acoustic</span> <span class="hlt">pressure</span> vector (<span class="hlt">acoustic</span> <span class="hlt">pressure</span> vectorized according to certain measurement geometry) are interchangeable. Computer simulation studies were conducted to evaluate the proposed theory, and the numerical results suggest that reconstruction of a vector field using the proposed theory is not sensitive to variation in the detecting distance. The present theory may be applied to magnetoacoustic tomography with magnetic induction (MAT-MI) for reconstructing current distribution from <span class="hlt">acoustic</span> measurements. A simulation on MAT-MI shows that, compared to existing methods, the present method can give an accurate estimation on the source current distribution and a better conductivity reconstruction. PMID:19211344</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003ASAJ..113..167L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003ASAJ..113..167L"><span><span class="hlt">Acoustic</span> near-field characteristics of a conical, premixed flame</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, Doh-Hyoung; Lieuwen, Tim C.</p> <p>2003-01-01</p> <p>The occurrence of self-excited <span class="hlt">pressure</span> oscillations routinely plagues the development of combustion systems. These oscillations are often driven by interactions between the flame and <span class="hlt">acoustic</span> perturbations. This study was performed to characterize the structure of the <span class="hlt">acoustic</span> field in the near field of the flame and the manner in which it is influenced by oscillation frequency, combustor geometry, flame length and temperature ratio. The results of these calculations indicate that the <span class="hlt">acoustic</span> velocity has primarily one- and two-dimensional features near the flame tip and base, respectively. The magnitude of the radial velocity components increases with temperature ratio across the flame, while their axial extent increases with frequency. However, the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> has primarily one-dimensional characteristics. They also show that the <span class="hlt">acoustic</span> field structure exhibits only moderate dependencies upon area expansion and flame temperature ratio for values typical of practical systems. Finally, they show that the local characteristics of the <span class="hlt">acoustic</span> field, as well as the overall plane-wave reflection coefficient, exhibit a decreasing dependence upon the flame length as the area expansion ratio increases.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12558257','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12558257"><span><span class="hlt">Acoustic</span> near-field characteristics of a conical, premixed flame.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lee, Doh-Hyoung; Lieuwen, Tim C</p> <p>2003-01-01</p> <p>The occurrence of self-excited <span class="hlt">pressure</span> oscillations routinely plagues the development of combustion systems. These oscillations are often driven by interactions between the flame and <span class="hlt">acoustic</span> perturbations. This study was performed to characterize the structure of the <span class="hlt">acoustic</span> field in the near field of the flame and the manner in which it is influenced by oscillation frequency, combustor geometry, flame length and temperature ratio. The results of these calculations indicate that the <span class="hlt">acoustic</span> velocity has primarily one- and two-dimensional features near the flame tip and base, respectively. The magnitude of the radial velocity components increases with temperature ratio across the flame, while their axial extent increases with frequency. However, the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> has primarily one-dimensional characteristics. They also show that the <span class="hlt">acoustic</span> field structure exhibits only moderate dependencies upon area expansion and flame temperature ratio for values typical of practical systems. Finally, they show that the local characteristics of the <span class="hlt">acoustic</span> field, as well as the overall plane-wave reflection coefficient, exhibit a decreasing dependence upon the flame length as the area expansion ratio increases.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2485241','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2485241"><span>Compensation of <span class="hlt">Gradient</span>-Induced Magnetic Field Perturbations</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Nixon, Terence W.; McIntyre, Scott; Rothman, Douglas L.; de Graaf, Robin A.</p> <p>2008-01-01</p> <p>Pulsed magnetic field <span class="hlt">gradients</span> are essential for MR imaging and localized spectroscopy applications. However, besides the desired linear field <span class="hlt">gradients</span>, pulsed currents in a strong external magnetic field also generate unwanted effects like eddy currents, <span class="hlt">gradient</span> coil vibrations and <span class="hlt">acoustic</span> noise. While the temporal magnetic field perturbations associated with eddy currents lead to spectral line shape distortions and signal loss, the vibration-related modulations lead to anti-symmetrical sidebands of any large signal (i.e. water), thereby obliterating the signals from smaller signals (i.e. metabolites). Here the measurement, characterization and compensation of vibrations-related magnetic field perturbations is presented. Following a quantitative evaluation of the various temporal components of the main magnetic field, a digital B0 magnetic field waveform is generated which reduces all temporal variations of the main magnetic field to within the spectral noise level. PMID:18329304</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002APS..DFD.JJ002W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002APS..DFD.JJ002W"><span>A Method for Large Eddy Simulation of <span class="hlt">Acoustic</span> Combustion Instabilities</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wall, Clifton; Pierce, Charles; Moin, Parviz</p> <p>2002-11-01</p> <p>A method for performing Large Eddy Simulation of <span class="hlt">acoustic</span> combustion instabilities is presented. By extending the low Mach number <span class="hlt">pressure</span> correction method to the case of compressible flow, a numerical method is developed in which the Poisson equation for <span class="hlt">pressure</span> is replaced by a Helmholtz equation. The method avoids the <span class="hlt">acoustic</span> CFL condition by using implicit time advancement, leading to large efficiency gains at low Mach number. The method also avoids artificial damping of <span class="hlt">acoustic</span> waves. The numerical method is attractive for the simulation of <span class="hlt">acoustic</span> combustion instabilities, since these flows are typically at low Mach number, and the <span class="hlt">acoustic</span> frequencies of interest are usually low. Both of these characteristics suggest the use of larger time steps than those allowed by an <span class="hlt">acoustic</span> CFL condition. The turbulent combustion model used is the Combined Conserved Scalar/Level Set Flamelet model of Duchamp de Lageneste and Pitsch for partially premixed combustion. Comparison of LES results to the experiments of Besson et al will be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28983969','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28983969"><span>A high-performance <span class="hlt">gradient</span> insert for rapid and short-T2 imaging at full duty cycle.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Weiger, Markus; Overweg, Johan; Rösler, Manuela Barbara; Froidevaux, Romain; Hennel, Franciszek; Wilm, Bertram Jakob; Penn, Alexander; Sturzenegger, Urs; Schuth, Wout; Mathlener, Menno; Borgo, Martino; Börnert, Peter; Leussler, Christoph; Luechinger, Roger; Dietrich, Benjamin Emanuel; Reber, Jonas; Brunner, David Otto; Schmid, Thomas; Vionnet, Laetitia; Pruessmann, Klaas P</p> <p>2018-06-01</p> <p>The goal of this study was to devise a <span class="hlt">gradient</span> system for MRI in humans that reconciles cutting-edge <span class="hlt">gradient</span> strength with rapid switching and brings up the duty cycle to 100% at full continuous amplitude. Aiming to advance neuroimaging and short-T 2 techniques, the hardware design focused on the head and the extremities as target anatomies. A boundary element method with minimization of power dissipation and stored magnetic energy was used to design anatomy-targeted <span class="hlt">gradient</span> coils with maximally relaxed geometry constraints. The design relies on hollow conductors for high-performance cooling and split coils to enable dual-mode <span class="hlt">gradient</span> amplifier operation. With this approach, strength and slew rate specifications of either 100 mT/m with 1200 mT/m/ms or 200 mT/m with 600 mT/m/ms were reached at 100% duty cycle, assuming a standard <span class="hlt">gradient</span> amplifier and cooling unit. After manufacturing, the specified values for maximum <span class="hlt">gradient</span> strength, maximum switching rate, and field geometry were verified experimentally. In temperature measurements, maximum local values of 63°C were observed, confirming that the device can be operated continuously at full amplitude. Testing for peripheral nerve stimulation showed nearly unrestricted applicability in humans at full <span class="hlt">gradient</span> performance. In measurements of <span class="hlt">acoustic</span> noise, a maximum average sound <span class="hlt">pressure</span> level of 132 dB(A) was determined. In vivo capability was demonstrated by head and knee imaging. Full <span class="hlt">gradient</span> performance was employed with echo planar and zero echo time readouts. Combining extreme <span class="hlt">gradient</span> strength and switching speed without duty cycle limitations, the described system offers unprecedented options for rapid and short-T 2 imaging. Magn Reson Med 79:3256-3266, 2018. © 2017 International Society for Magnetic Resonance in Medicine. © 2017 International Society for Magnetic Resonance in Medicine.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4684573','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4684573"><span>Procedures for ambient-<span class="hlt">pressure</span> and tympanometric tests of aural <span class="hlt">acoustic</span> reflectance and admittance in human infants and adults</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Keefe, Douglas H.; Hunter, Lisa L.; Feeney, M. Patrick; Fitzpatrick, Denis F.</p> <p>2015-01-01</p> <p>Procedures are described to measure <span class="hlt">acoustic</span> reflectance and admittance in human adult and infant ears at frequencies from 0.2 to 8 kHz. Transfer functions were measured at ambient <span class="hlt">pressure</span> in the ear canal, and as down- or up-swept tympanograms. <span class="hlt">Acoustically</span> estimated ear-canal area was used to calculate ear reflectance, which was parameterized by absorbance and group delay over all frequencies (and <span class="hlt">pressures</span>), with substantial data reduction for tympanograms. Admittance measured at the probe tip in adults was transformed into an equivalent admittance at the eardrum using a transmission-line model for an ear canal with specified area and ear-canal length. Ear-canal length was estimated from group delay around the frequency above 2 kHz of minimum absorbance. Illustrative measurements in ears with normal function are described for an adult, and two infants at 1 month of age with normal hearing and a conductive hearing loss. The sensitivity of this equivalent eardrum admittance was calculated for varying estimates of area and length. Infant-ear patterns of absorbance peaks aligned in frequency with dips in group delay were explained by a model of resonant canal-wall mobility. Procedures will be applied in a large study of wideband clinical diagnosis and monitoring of middle-ear and cochlear function. PMID:26723319</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4437633','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4437633"><span>Ex-Vivo Lymphatic Perfusion System for Independently Controlling <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> and Transmural <span class="hlt">Pressure</span> in Isolated Vessels</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kornuta, Jeffrey A.; Dixon, J. Brandon</p> <p>2015-01-01</p> <p>In addition to external forces, collecting lymphatic vessels intrinsically contract to transport lymph from the extremities to the venous circulation. As a result, the lymphatic endothelium is routinely exposed to a wide range of dynamic mechanical forces, primarily fluid shear stress and circumferential stress, which have both been shown to affect lymphatic pumping activity. Although various ex-vivo perfusion systems exist to study this innate pumping activity in response to mechanical stimuli, none are capable of independently controlling the two primary mechanical forces affecting lymphatic contractility: transaxial <span class="hlt">pressure</span> <span class="hlt">gradient</span>, ΔP, which governs fluid shear stress; and average transmural <span class="hlt">pressure</span>, Pavg, which governs circumferential stress. Hence, the authors describe a novel ex-vivo lymphatic perfusion system (ELPS) capable of independently controlling these two outputs using a linear, explicit model predictive control (MPC) algorithm. The ELPS is capable of reproducing arbitrary waveforms within the frequency range observed in the lymphatics in vivo, including a time-varying ΔP with a constant Pavg, time-varying ΔP and Pavg, and a constant ΔP with a time-varying Pavg. In addition, due to its implementation of syringes to actuate the working fluid, a post-hoc method of estimating both the flow rate through the vessel and fluid wall shear stress over multiple, long (5 sec) time windows is also described. PMID:24809724</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900018149','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900018149"><span>The validation and application of a rotor <span class="hlt">acoustic</span> prediction computer program</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gallman, Judith M.</p> <p>1990-01-01</p> <p>An essential prerequisite to reducing the <span class="hlt">acoustic</span> detectability of military rotorcraft is a better understanding of main rotor noise which is the major contributor to the overall noise. A simple, yet accurate, Rotor <span class="hlt">Acoustic</span> Prediction Program (RAPP) was developed to advance the understanding of main rotor noise. This prediction program uses the Ffowcs Williams and Hawkings (FW-H) equation. The particular form of the FW-H equation used is well suited for the coupling of the measured blade surface <span class="hlt">pressure</span> to the prediction of <span class="hlt">acoustic</span> <span class="hlt">pressure</span>. The FW-H equation is an inhomogeneous wave equation that is valid in all space and governs <span class="hlt">acoustic</span> <span class="hlt">pressure</span> generated by thin moving bodies. The nonhomogeneous terms describe mass displacement due to surface motion and forces due to local surface stresses, such as viscous stress and <span class="hlt">pressure</span> distribution on the surface. This paper examines two of the four types of main rotor noise: BVI noise and low-frequency noise. Blade-vortex interaction noise occurs when a tip vortex, previously shed by a rotor blade, passes close enough to a rotor blade to cause large variations in the blade surface <span class="hlt">pressures</span>. This event is most disturbing when it happens on the advancing side of the rotor disk. Low-frequency noise includes hover and low to moderate speed forward flight. For these flight conditions, the low frequency components of the <span class="hlt">acoustic</span> signal dominate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25138664','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25138664"><span>The role of jet eccentricity in generating disproportionately elevated transaortic <span class="hlt">pressure</span> <span class="hlt">gradients</span> in patients with aortic stenosis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Abbas, Amr E; Franey, Laura M; Lester, Steven; Raff, Gilbert; Gallagher, Michael J; Hanzel, George; Safian, Robert D; Pibarot, Philippe</p> <p>2015-02-01</p> <p>In patients with aortic stenosis (AS) and eccentric transaortic flow, greater <span class="hlt">pressure</span> loss occurs as the jet collides with the aortic wall together with delayed and diminished <span class="hlt">pressure</span> recovery. This leads to the elevated transaortic valve <span class="hlt">pressure</span> <span class="hlt">gradients</span> noted on both Doppler and cardiac catheterization. Such situations may present a diagnostic dilemma where traditional measures of stenosis severity indicate severe AS, while imaging modalities of the aortic valve geometric aortic valve area (GOA) suggest less than severe stenosis. In this study, we present a series of cases exemplifying this clinical dilemma and demonstrate how color M-mode, 2D and 3D transthoracic (TTE) and transesophageal (TEE) echocardiography, cardiac computed tomography angiography (CTA), and magnetic resonance imaging (MRI), may be used to resolve such discrepancies. © 2014, Wiley Periodicals, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27743249','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27743249"><span>The association between the pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> at the cranio-cervical junction derived from phase-contrast magnetic resonance imaging and invasively measured pulsatile intracranial <span class="hlt">pressure</span> in symptomatic patients with Chiari malformation type 1.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Frič, Radek; Lindstrøm, Erika Kristina; Ringstad, Geir Andre; Mardal, Kent-André; Eide, Per Kristian</p> <p>2016-12-01</p> <p>In symptomatic Chiari malformation type 1 (CMI), impaired intracranial compliance (ICC) is associated with an increased cranio-spinal pulsatile <span class="hlt">pressure</span> <span class="hlt">gradient</span>. Phase-contrast magnetic resonance imaging (MRI) represents a non-invasive modality for the assessment of the pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> at the cranio-cervical junction (CCJ). We wished to explore how the MRI-derived pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> (MRI-dP) compares with invasively measured pulsatile intracranial <span class="hlt">pressure</span> (ICP) in CMI, and with healthy controls. From phase-contrast MRI of CMI patients and healthy controls, we computed cerebrospinal fluid (CSF) flow velocities and MRI-dP at the CCJ. We assessed bidirectional flow and compared the flow between the anterior and the posterior subarachnoid space at the CCJ. We computed total intracranial volume (ICV), ventricular CSF volume (VV), and posterior cranial fossa volume (PCFV). We analyzed the static and pulsatile ICP scores from overnight monitoring in CMI patients. Five CMI patients and four healthy subjects were included. The CMI group had a significantly larger extent of tonsillar ectopia, smaller PCFV, and a smaller area of CSF in the FM. The pulsatile ICP (mean ICP wave amplitude, MWA) was abnormally increased in 4/5 CMI patients and correlated positively with MRI-dP. However, the MRI-dP as well as the CSF flow velocities did not differ significantly between CMI and healthy subjects. Moreover, bidirectional flow was observed in both CMI as well as healthy subjects, with no significant difference. In symptomatic CMI patients, we found a significant association between the pulse <span class="hlt">pressure</span> <span class="hlt">gradient</span> at the CCJ derived from phase-contrast MRI and the pulsatile ICP (MWA) measured invasively. However, the MRI-dP was close to identical in CMI patients and healthy subjects. Moreover, the CSF flow velocities at the CCJ and the occurrence of bidirectional flow were not different in CMI patients and healthy individuals. Further studies are required to determine the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19780041998&hterms=Electromagnetic+Pulse&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DElectromagnetic%2BPulse','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19780041998&hterms=Electromagnetic+Pulse&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DElectromagnetic%2BPulse"><span>Interaction of electromagnetic and <span class="hlt">acoustic</span> waves in a stochastic atmosphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bhatnagar, N.; Frankel, M. S.; Peterson, A. M.</p> <p>1977-01-01</p> <p>This paper considers the interaction of electromagnetic and <span class="hlt">acoustic</span> waves where a Radio <span class="hlt">Acoustic</span> Sounding System (RASS) is operated in a stochastic environment characterized by turbulence, winds and mean-temperature <span class="hlt">gradients</span>. It has been shown that for a RASS operating at <span class="hlt">acoustic</span> frequencies below a few kilohertz propagating under typical atmospheric conditions, turbulence has little effect on the strength of the received radio signal scattered from the pulse at heights up to a few kilometers. This result implies that the received RF signal level (power) is primarily a function of sound intensity which decreases as x exp minus 2 where x is the altitude.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19840015581','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840015581"><span>Investigation of the effects of <span class="hlt">pressure</span> <span class="hlt">gradient</span>, temperature and wall temperature ratio on the stagnation point heat transfer for circular cylinders and gas turbine vanes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nagamatsu, H. T.; Duffy, R. E.</p> <p>1984-01-01</p> <p>Low and high <span class="hlt">pressure</span> shock tubes were designed and constructed for the purpose of obtaining heat transfer data over a temperature range of 390 to 2500 K, <span class="hlt">pressures</span> of 0.3 to 42 atm, and Mach numbers of 0.15 to 1.5 with and without <span class="hlt">pressure</span> <span class="hlt">gradient</span>. A square test section with adjustable top and bottom walls was constructed to produce the favorable and adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span> over the flat plate with heat gages. A water cooled gas turbine nozzle cascade which is attached to the high <span class="hlt">pressure</span> shock tube was obtained to measuse the heat flux over <span class="hlt">pressure</span> and suction surfaces. Thin-film platinum heat gages with a response time of a few microseconds were developed and used to measure the heat flux for laminar, transition, and turbulent boundary layers. The laminar boundary heat flux on the shock tube wall agreed with Mirel's flat plate theory. Stagnation point heat transfer for circular cylinders at low temperature compared with the theoretical prediction, but for a gas temperature of 922 K the heat fluxes were higher than the predicted values. Preliminary flat plate heat transfer data were measured for laminar, transition, and turbulent boundary layers with and without <span class="hlt">pressure</span> <span class="hlt">gradients</span> for free-stream temperatures of 350 to 2575 K and flow Mach numbers of 0.11 to 1.9. The experimental heat flux data were correlated with the laminar and turbulent theories and the agreement was good at low temperatures which was not the case for higher temperatures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16657786','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16657786"><span>Water potential <span class="hlt">gradient</span> in a tall sequoiadendron.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tobiessen, P</p> <p>1971-09-01</p> <p>With an elevator installed in a 90-meter tall Sequoiadendron to collect the samples, xylem <span class="hlt">pressure</span> potential measurements were made approximately every 15 meters along 60 meters of the tree's height. The measured <span class="hlt">gradient</span> was about -0.8 bar per 10 meters of height, i.e., less than the hydrostatic <span class="hlt">gradient</span>. Correction of the xylem <span class="hlt">pressure</span> potential data by calibration against a thermocouple psychrometer confirmed this result. Similar <span class="hlt">gradients</span> are described in the literature in tall conifers at times of low transpiration, although a different sampling technique was used. If the data in the present study and those supporting it are typical, they imply a re-evaluation of either the use of the <span class="hlt">pressure</span> chamber to estimate water potential or the present theories describing water transport in tall trees.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=396854','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=396854"><span>Water Potential <span class="hlt">Gradient</span> in a Tall Sequoiadendron</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Tobiessen, Peter; Rundel, Philip W.; Stecker, R. E.</p> <p>1971-01-01</p> <p>With an elevator installed in a 90-meter tall Sequoiadendron to collect the samples, xylem <span class="hlt">pressure</span> potential measurements were made approximately every 15 meters along 60 meters of the tree's height. The measured <span class="hlt">gradient</span> was about −0.8 bar per 10 meters of height, i.e., less than the hydrostatic <span class="hlt">gradient</span>. Correction of the xylem <span class="hlt">pressure</span> potential data by calibration against a thermocouple psychrometer confirmed this result. Similar <span class="hlt">gradients</span> are described in the literature in tall conifers at times of low transpiration, although a different sampling technique was used. If the data in the present study and those supporting it are typical, they imply a re-evaluation of either the use of the <span class="hlt">pressure</span> chamber to estimate water potential or the present theories describing water transport in tall trees. PMID:16657786</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19740025322','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19740025322"><span>Boundary-layer transition on a plate subjected to simultaneous spanwise and chordwise <span class="hlt">pressure</span> <span class="hlt">gradients</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Boldman, D. R.; Brinich, P. F.</p> <p>1974-01-01</p> <p>The boundary-layer transition on a short plate was studied by means of the china-clay visual technique. The plate model was mounted in a wind tunnel so that it was subjected to small simultaneous spanwise and chordwise <span class="hlt">pressure</span> <span class="hlt">gradients</span>. Results of the experimental study, which was performed at three subsonic velocities, indicated that the transition pattern was appreciably curved in the spanwise direction but quite smooth and well behaved. Reasonable comparisons between predictions of transition and experiment were obtained from two finite-difference two-dimensional boundary-layer calculation methods which incorporated transition models based on the concept of a transition intermittency factor.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhDT.......146A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhDT.......146A"><span>Design and development of second order MEMS sound <span class="hlt">pressure</span> <span class="hlt">gradient</span> sensor</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Albahri, Shehab</p> <p></p> <p>The design and development of a second order MEMS sound <span class="hlt">pressure</span> <span class="hlt">gradient</span> sensor is presented in this dissertation. Inspired by the directional hearing ability of the parasitoid fly, Ormia ochracea, a novel first order directional microphone that mimics the mechanical structure of the fly's ears and detects the sound <span class="hlt">pressure</span> <span class="hlt">gradient</span> has been developed. While the first order directional microphones can be very beneficial in a large number of applications, there is great potential for remarkable improvements in performance through the use of second order systems. The second order directional microphone is able to provide a theoretical improvement in Sound to Noise ratio (SNR) of 9.5dB, compared to the first-order system that has its maximum SNR of 6dB. Although second order microphone is more sensitive to sound angle of incidence, the nature of the design and fabrication process imposes different factors that could lead to deterioration in its performance. The first Ormia ochracea second order directional microphone was designed in 2004 and fabricated in 2006 at Binghamton University. The results of the tested parts indicate that the Ormia ochracea second order directional microphone performs mostly as an Omni directional microphone. In this work, the previous design is reexamined and analyzed to explain the unexpected results. A more sophisticated tool implementing a finite element package ANSYS is used to examine the previous design response. This new tool is used to study different factors that used to be ignored in the previous design, mainly; response mismatch and fabrication uncertainty. A continuous model using Hamilton's principle is introduced to verify the results using the new method. Both models agree well, and propose a new way for optimizing the second order directional microphone using geometrical manipulation. In this work we also introduce a new fabrication process flow to increase the fabrication yield. The newly suggested method uses the shell</p> </li> </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/29429710','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29429710"><span>Numerical simulation of single bubble dynamics under <span class="hlt">acoustic</span> travelling waves.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ma, Xiaojian; Huang, Biao; Li, Yikai; Chang, Qing; Qiu, Sicong; Su, Zheng; Fu, Xiaoying; Wang, Guoyu</p> <p>2018-04-01</p> <p>The objective of this paper is to apply CLSVOF method to investigate the single bubble dynamics in <span class="hlt">acoustic</span> travelling waves. The Naiver-Stokes equation considering the <span class="hlt">acoustic</span> radiation force is proposed and validated to capture the bubble behaviors. And the CLSVOF method, which can capture the continuous geometric properties and satisfies mass conservation, is applied in present work. Firstly, the regime map, depending on the dimensionless <span class="hlt">acoustic</span> <span class="hlt">pressure</span> amplitude and <span class="hlt">acoustic</span> wave number, is constructed to present different bubble behaviors. Then, the time evolution of the bubble oscillation is investigated and analyzed. Finally, the effect of the direction and the damping coefficient of <span class="hlt">acoustic</span> wave propagation on the bubble behavior are also considered. The numerical results show that the bubble presents distinct oscillation types in <span class="hlt">acoustic</span> travelling waves, namely, volume oscillation, shape oscillation, and splitting oscillation. For the splitting oscillation, the formation of jet, splitting of bubble, and the rebound of sub-bubbles may lead to substantial increase in <span class="hlt">pressure</span> fluctuations on the boundary. For the shape oscillation, the nodes and antinodes of the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> wave contribute to the formation of the "cross shape" of the bubble. It should be noted that the direction of the bubble translation and bubble jet are always towards the direction of wave propagation. In addition, the damping coefficient causes bubble in shape oscillation to be of asymmetry in shape and inequality in size, and delays the splitting process. Copyright © 2017 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014E%26ES...22e2007C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014E%26ES...22e2007C"><span>Detection of cavitation vortex in hydraulic turbines using <span class="hlt">acoustic</span> techniques</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Candel, I.; Bunea, F.; Dunca, G.; Bucur, D. M.; Ioana, C.; Reeb, B.; Ciocan, G. D.</p> <p>2014-03-01</p> <p>Cavitation phenomena are known for their destructive capacity in hydraulic machineries and are caused by the <span class="hlt">pressure</span> decrease followed by an implosion when the cavitation bubbles find an adverse <span class="hlt">pressure</span> <span class="hlt">gradient</span>. A helical vortex appears in the turbine diffuser cone at partial flow rate operation and can be cavitating in its core. Cavity volumes and vortex frequencies vary with the under-<span class="hlt">pressure</span> level. If the vortex frequency comes close to one of the eigen frequencies of the turbine, a resonance phenomenon may occur, the unsteady fluctuations can be amplified and lead to important turbine and hydraulic circuit damage. Conventional cavitation vortex detection techniques are based on passive devices (<span class="hlt">pressure</span> sensors or accelerometers). Limited sensor bandwidths and low frequency response limit the vortex detection and characterization information provided by the passive techniques. In order to go beyond these techniques and develop a new active one that will remove these drawbacks, previous work in the field has shown that techniques based on <span class="hlt">acoustic</span> signals using adapted signal content to a particular hydraulic situation, can be more robust and accurate. The cavitation vortex effects in the water flow profile downstream hydraulic turbines runner are responsible for signal content modifications. Basic signal techniques use narrow band signals traveling inside the flow from an emitting transducer to a receiving one (active sensors). Emissions of wide band signals in the flow during the apparition and development of the vortex embeds changes in the received signals. Signal processing methods are used to estimate the cavitation apparition and evolution. Tests done in a reduced scale facility showed that due to the increasing flow rate, the signal -- vortex interaction is seen as modifications on the received signal's high order statistics and bandwidth. Wide band <span class="hlt">acoustic</span> transducers have a higher dynamic range over mechanical elements; the system's reaction time</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19720006029','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19720006029"><span>An investigation of transient <span class="hlt">pressure</span> and plasma properties in a pinched plasma column. M.S. Thesis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Stover, E. K.; York, T. M.</p> <p>1971-01-01</p> <p>The transient pinched plasma column generated in a linear Z-pinch was studied experimentally and analytically. The plasma column was investigated experimentally with the following plasma diagnostics: a special rapid response <span class="hlt">pressure</span> transducer, a magnetic field probe, a voltage probe and discharge luminosity. Axial <span class="hlt">pressure</span> profiles on the discharge chamber axis were used to identify three characteristic regions of plasma column behavior; they were in temporal sequence: strong axial <span class="hlt">pressure</span> asymmetry noted early in plasma column lifetime followed by plasma heating in which there is a rapid rise in static <span class="hlt">pressure</span> and a slight decrease static <span class="hlt">pressure</span> before plasma column breakup. Plasma column lifetime was approximately 5 microseconds. The axial <span class="hlt">pressure</span> asymmetry was attributed to nonsimultaneous pinching of the imploding current sheet along the discharge chamber axis. The rapid heating is attributed in part to viscous effects introduced by radial <span class="hlt">gradients</span> in the axial streaming velocity. Turbulent heating arising from discharge current excitation of the ion <span class="hlt">acoustic</span> wave instability is also considered a possible heating mechanism.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19830024244','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19830024244"><span><span class="hlt">Acoustic</span> system for material transport</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Barmatz, M. B.; Trinh, E. H.; Wang, T. G.; Elleman, D. D.; Jacobi, N. (Inventor)</p> <p>1983-01-01</p> <p>An object within a chamber is <span class="hlt">acoustically</span> moved by applying wavelengths of different modes to the chamber to move the object between <span class="hlt">pressure</span> wells formed by the modes. In one system, the object is placed in one end of the chamber while a resonant mode, applied along the length of the chamber, produces a <span class="hlt">pressure</span> well at the location. The frequency is then switched to a second mode that produces a <span class="hlt">pressure</span> well at the center of the chamber, to draw the object. When the object reaches the second <span class="hlt">pressure</span> well and is still traveling towards the second end of the chamber, the <span class="hlt">acoustic</span> frequency is again shifted to a third mode (which may equal the first model) that has a <span class="hlt">pressure</span> well in the second end portion of the chamber, to draw the object. A heat source may be located near the second end of the chamber to heat the sample, and after the sample is heated it can be cooled by moving it in a corresponding manner back to the first end of the chamber. The transducers for levitating and moving the object may be all located at the cool first end of the chamber.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010057034','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010057034"><span>Comparison of Two <span class="hlt">Acoustic</span> Waveguide Methods for Determining Liner Impedance</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jones, Michael G.; Watson, Willie R.; Tracy, Maureen B.; Parrott, Tony L.</p> <p>2001-01-01</p> <p><span class="hlt">Acoustic</span> measurements taken in a flow impedance tube are used to assess the relative accuracy of two waveguide methods for impedance eduction in the presence of grazing flow. The aeroacoustic environment is assumed to contain forward and backward-traveling <span class="hlt">acoustic</span> waves, consisting of multiple modes, and uniform mean flow. Both methods require a measurement of the complex <span class="hlt">acoustic</span> <span class="hlt">pressure</span> profile over the length of the test liner. The Single Mode Method assumes that the sound <span class="hlt">pressure</span> level and phase decay-rates of a single progressive mode can be extracted from this measured complex <span class="hlt">acoustic</span> <span class="hlt">pressure</span> profile. No a priori assumptions are made in the Finite Element. Method regarding the modal or reflection content in the measured <span class="hlt">acoustic</span> <span class="hlt">pressure</span> profile. The integrity of each method is initially demonstrated by how well their no-flow impedances match those acquired in a normal incidence impedance tube. These tests were conducted using ceramic tubular and conventional perforate liners. Ceramic tubular liners were included because of their impedance insensitivity to mean flow effects. Conversely, the conventional perforate liner was included because its impedance is known to be sensitive to mean flow velocity effects. Excellent comparisons between impedance values educed with the two waveguide methods in the absence of mean flow and the corresponding values educed with the normal incident impedance tube were observed. The two methods are then compared for mean flow Mach numbers up to 0.5, and are shown to give consistent results for both types of test liners. The quality of the results indicates that the Single Mode Method should be used when the measured <span class="hlt">acoustic</span> <span class="hlt">pressure</span> profile is clearly dominated by a single progressive mode, and the Finite Element Method should be used for all other cases.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22778438','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22778438"><span>Redox systematics of a magma ocean with variable <span class="hlt">pressure</span>-temperature <span class="hlt">gradients</span> and composition.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Righter, K; Ghiorso, M S</p> <p>2012-07-24</p> <p>Oxygen fugacity in metal-bearing systems controls some fundamental aspects of the geochemistry of the early Earth, such as the FeO and siderophile trace element content of the mantle, volatile species that influence atmospheric composition, and conditions for organic compounds synthesis. Redox and metal-silicate equilibria in the early Earth are sensitive to oxygen fugacity (fO(2)), yet are poorly constrained in modeling and experimentation. High <span class="hlt">pressure</span> and temperature experimentation and modeling in metal-silicate systems usually employs an approximation approach for estimating fO(2) that is based on the ratio of Fe and FeO [called "ΔIW (ratio)" hereafter]. We present a new approach that utilizes free energy and activity modeling of the equilibrium: Fe + SiO(2) + O(2) = Fe(2)SiO(4) to calculate absolute fO(2) and relative to the iron-wüstite (IW) buffer at <span class="hlt">pressure</span> and temperature [ΔIW (P,T)]. This equilibrium is considered across a wide range of <span class="hlt">pressures</span> and temperatures, including up to the liquidus temperature of peridotite (4,000 K at 50 GPa). Application of ΔIW (ratio) to metal-silicate experiments can be three or four orders of magnitude different from ΔIW (P,T) values calculated using free energy and activity modeling. We will also use this approach to consider the variation in oxygen fugacity in a magma ocean scenario for various thermal structures for the early Earth: hot liquidus <span class="hlt">gradient</span>, 100 °C below the liquidus, hot and cool adiabatic <span class="hlt">gradients</span>, and a cool subsolidus adiabat. The results are used to assess the effect of increasing P and T, changing silicate composition during accretion, and related to current models for accretion and core formation in the Earth. The fO(2) in a deep magma ocean scenario may become lower relative to the IW buffer at hotter and deeper conditions, which could include metal entrainment scenarios. Therefore, fO(2) may evolve from high to low fO(2) during Earth (and other differentiated bodies) accretion. Any</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3409746','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3409746"><span>Redox systematics of a magma ocean with variable <span class="hlt">pressure</span>-temperature <span class="hlt">gradients</span> and composition</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Righter, K.; Ghiorso, M. S.</p> <p>2012-01-01</p> <p>Oxygen fugacity in metal-bearing systems controls some fundamental aspects of the geochemistry of the early Earth, such as the FeO and siderophile trace element content of the mantle, volatile species that influence atmospheric composition, and conditions for organic compounds synthesis. Redox and metal-silicate equilibria in the early Earth are sensitive to oxygen fugacity (fO2), yet are poorly constrained in modeling and experimentation. High <span class="hlt">pressure</span> and temperature experimentation and modeling in metal-silicate systems usually employs an approximation approach for estimating fO2 that is based on the ratio of Fe and FeO [called “ΔIW (ratio)” hereafter]. We present a new approach that utilizes free energy and activity modeling of the equilibrium: Fe + SiO2 + O2 = Fe2SiO4 to calculate absolute fO2 and relative to the iron-wüstite (IW) buffer at <span class="hlt">pressure</span> and temperature [ΔIW (P,T)]. This equilibrium is considered across a wide range of <span class="hlt">pressures</span> and temperatures, including up to the liquidus temperature of peridotite (4,000 K at 50 GPa). Application of ΔIW (ratio) to metal-silicate experiments can be three or four orders of magnitude different from ΔIW (P,T) values calculated using free energy and activity modeling. We will also use this approach to consider the variation in oxygen fugacity in a magma ocean scenario for various thermal structures for the early Earth: hot liquidus <span class="hlt">gradient</span>, 100 °C below the liquidus, hot and cool adiabatic <span class="hlt">gradients</span>, and a cool subsolidus adiabat. The results are used to assess the effect of increasing P and T, changing silicate composition during accretion, and related to current models for accretion and core formation in the Earth. The fO2 in a deep magma ocean scenario may become lower relative to the IW buffer at hotter and deeper conditions, which could include metal entrainment scenarios. Therefore, fO2 may evolve from high to low fO2 during Earth (and other differentiated bodies) accretion. Any modeling of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150023002','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150023002"><span>Implicit Large-Eddy Simulations of Zero-<span class="hlt">Pressure</span> <span class="hlt">Gradient</span>, Turbulent Boundary Layer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sekhar, Susheel; Mansour, Nagi N.</p> <p>2015-01-01</p> <p>A set of direct simulations of zero-<span class="hlt">pressure</span> <span class="hlt">gradient</span>, turbulent boundary layer flows are conducted using various span widths (62-630 wall units), to document their influence on the generated turbulence. The FDL3DI code that solves compressible Navier-Stokes equations using high-order compact-difference scheme and filter, with the standard recycling/rescaling method of turbulence generation, is used. Results are analyzed at two different Re values (500 and 1,400), and compared with spectral DNS data. They show that a minimum span width is required for the mere initiation of numerical turbulence. Narrower domains ((is) less than 100 w.u.) result in relaminarization. Wider spans ((is) greater than 600 w.u.) are required for the turbulent statistics to match reference DNS. The upper-wall boundary condition for this setup spawns marginal deviations in the mean velocity and Reynolds stress profiles, particularly in the buffer region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22492622-acoustic-streaming-jets-scaling-dimensional-analysis','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22492622-acoustic-streaming-jets-scaling-dimensional-analysis"><span><span class="hlt">Acoustic</span> streaming jets: A scaling and dimensional analysis</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>Botton, V., E-mail: valery.botton@insa-lyon.fr; Henry, D.; Millet, S.</p> <p>2015-10-28</p> <p>We present our work on <span class="hlt">acoustic</span> streaming free jets driven by ultrasonic beams in liquids. These jets are steady flows generated far from walls by progressive <span class="hlt">acoustic</span> waves. As can be seen on figure 1, our set-up, denominated AStrID for <span class="hlt">Acoustic</span> Streaming Investigation Device, is made of a water tank in which a 29 mm plane source emits continuous ultrasonic waves at typically 2 MHz. Our approach combines an experimental characterization of both the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> field (hydrophone) and the obtained <span class="hlt">acoustic</span> streaming velocity field (PIV visualization) on one hand, with CFD using an incompressible Navier-Stokes solver on the other hand.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22398945-towards-direct-realisation-si-unit-sound-pressure-audible-hearing-range-based-optical-free-field-acoustic-particle-measurements','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22398945-towards-direct-realisation-si-unit-sound-pressure-audible-hearing-range-based-optical-free-field-acoustic-particle-measurements"><span>Towards direct realisation of the SI unit of sound <span class="hlt">pressure</span> in the audible hearing range based on optical free-field <span class="hlt">acoustic</span> particle 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>Koukoulas, Triantafillos, E-mail: triantafillos.koukoulas@npl.co.uk; Piper, Ben</p> <p></p> <p>Since the introduction of the International System of Units (the SI system) in 1960, weights, measures, standardised approaches, procedures, and protocols have been introduced, adapted, and extensively used. A major international effort and activity concentrate on the definition and traceability of the seven base SI units in terms of fundamental constants, and consequently those units that are derived from the base units. In airborne <span class="hlt">acoustical</span> metrology and for the audible range of frequencies up to 20 kHz, the SI unit of sound <span class="hlt">pressure</span>, the pascal, is realised indirectly and without any knowledge or measurement of the sound field. Though themore » principle of reciprocity was originally formulated by Lord Rayleigh nearly two centuries ago, it was devised in the 1940s and eventually became a calibration standard in the 1960s; however, it can only accommodate a limited number of <span class="hlt">acoustic</span> sensors of specific types and dimensions. International standards determine the device sensitivity either through coupler or through free-field reciprocity but rely on the continuous availability of specific <span class="hlt">acoustical</span> artefacts. Here, we show an optical method based on gated photon correlation spectroscopy that can measure sound <span class="hlt">pressures</span> directly and absolutely in fully anechoic conditions, remotely, and without disturbing the propagating sound field. It neither relies on the availability or performance of any measurement artefact nor makes any assumptions of the device geometry and sound field characteristics. Most importantly, the required units of sound <span class="hlt">pressure</span> and microphone sensitivity may now be experimentally realised, thus providing direct traceability to SI base units.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvE..97a0901G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvE..97a0901G"><span>Synchronized oscillations and <span class="hlt">acoustic</span> fluidization in confined granular materials</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Giacco, F.; de Arcangelis, L.; Ciamarra, M. Pica; Lippiello, E.</p> <p>2018-01-01</p> <p>According to the <span class="hlt">acoustic</span> fluidization hypothesis, elastic waves at a characteristic frequency form inside seismic faults even in the absence of an external perturbation. These waves are able to generate a normal stress which contrasts the confining <span class="hlt">pressure</span> and promotes failure. Here, we study the mechanisms responsible for this wave activation via numerical simulations of a granular fault model. We observe the particles belonging to the percolating backbone, which sustains the stress, to perform synchronized oscillations over ellipticlike trajectories in the fault plane. These oscillations occur at the characteristic frequency of <span class="hlt">acoustic</span> fluidization. As the applied shear stress increases, these oscillations become perpendicular to the fault plane just before the system fails, opposing the confining <span class="hlt">pressure</span>, consistently with the <span class="hlt">acoustic</span> fluidization scenario. The same change of orientation can be induced by external perturbations at the <span class="hlt">acoustic</span> fluidization frequency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930000622&hterms=biometrics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dbiometrics','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930000622&hterms=biometrics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dbiometrics"><span>Improved Calibration Of <span class="hlt">Acoustic</span> Plethysmographic Sensors</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zuckerwar, Allan J.; Davis, David C.</p> <p>1993-01-01</p> <p>Improved method of calibration of <span class="hlt">acoustic</span> plethysmographic sensors involves <span class="hlt">acoustic</span>-impedance test conditions like those encountered in use. Clamped aluminum tube holds source of sound (hydrophone) inside balloon. Test and reference sensors attached to outside of balloon. Sensors used to measure blood flow, blood <span class="hlt">pressure</span>, heart rate, breathing sounds, and other vital signs from surfaces of human bodies. Attached to torsos or limbs by straps or adhesives.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24815258','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24815258"><span>A geospatial model of ambient sound <span class="hlt">pressure</span> levels in the contiguous United States.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mennitt, Daniel; Sherrill, Kirk; Fristrup, Kurt</p> <p>2014-05-01</p> <p>This paper presents a model that predicts measured sound <span class="hlt">pressure</span> levels using geospatial features such as topography, climate, hydrology, and anthropogenic activity. The model utilizes random forest, a tree-based machine learning algorithm, which does not incorporate a priori knowledge of source characteristics or propagation mechanics. The response data encompasses 270 000 h of <span class="hlt">acoustical</span> measurements from 190 sites located in National Parks across the contiguous United States. The explanatory variables were derived from national geospatial data layers and cross validation procedures were used to evaluate model performance and identify variables with predictive power. Using the model, the effects of individual explanatory variables on sound <span class="hlt">pressure</span> level were isolated and quantified to reveal systematic trends across environmental <span class="hlt">gradients</span>. Model performance varies by the <span class="hlt">acoustical</span> metric of interest; the seasonal L50 can be predicted with a median absolute deviation of approximately 3 dB. The primary application for this model is to generalize point measurements to maps expressing spatial variation in ambient sound levels. An example of this mapping capability is presented for Zion National Park and Cedar Breaks National Monument in southwestern Utah.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19970000433','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19970000433"><span>Stabilization and Low-Frequency Oscillation of Capillary Bridges with Modulated <span class="hlt">Acoustic</span> Radiation <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>Marston, Philip L.; Marr-Lyon, Mark J.; Morse, S. F.; Thiessen, David B.</p> <p>1996-01-01</p> <p>In the work reported here it is demonstrated that <span class="hlt">acoustic</span> radiation <span class="hlt">pressure</span> may be used in simulated low gravity to produce stable bridges significantly beyond the Rayleigh limit with S as large as 3.6. The bridge (PDMS mixed with a dense liquid) has the same density as the surrounding water bath containing an ultrasonic standing wave. Modulation was first used to excite specific bridge modes. In the most recent work reported here the shape of the bridge is optically sensed and the ultrasonic drive is electronically adjusted such that the radiation stress distribution dynamically quenches the most unstable mode. This active control simulates passive stabilization suggested for low gravity. Feedback increases the mode frequency in the naturally stable region since the effective stiffness of the mode is increased.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130000609','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130000609"><span>Verification of Ares I Liftoff <span class="hlt">Acoustic</span> Environments via the Ares Scale Model <span class="hlt">Acoustic</span> Test</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Counter, Douglas D.; Houston, Janice D.</p> <p>2012-01-01</p> <p>Launch environments, such as Liftoff <span class="hlt">Acoustic</span> (LOA) and Ignition Overpressure (IOP), are important design factors for any vehicle and are dependent upon the design of both the vehicle and the ground systems. The NASA Constellation Program had several risks to the development of the Ares I vehicle linked to LOA which are used in the development of the vibro-<span class="hlt">acoustic</span> environments. The risks included cost, schedule and technical impacts for component qualification due to high predicted vibro-<span class="hlt">acoustic</span> environments. One solution is to mitigate the environment at the component level. However, where the environment is too severe to mitigate at the component level, reduction of the launch environments is required. The Ares I Scale Model <span class="hlt">Acoustic</span> Test (ASMAT) program was implemented to verify the predicted Ares I launch environments and to determine the <span class="hlt">acoustic</span> reduction for the LOA environment with an above deck water sound suppression system. The test article included a 5% scale Ares I vehicle model, tower and Mobile Launcher. <span class="hlt">Acoustic</span> and <span class="hlt">pressure</span> data were measured by approximately 200 instruments. The ASMAT results are compared to the Ares I LOA predictions and water suppression effectiveness results are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090042611','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090042611"><span>Optimal Disturbances in Boundary Layers Subject to Streamwise <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tumin, Anatoli; Ashpis, David E.</p> <p>2003-01-01</p> <p>Laminar-turbulent transition in shear flows is still an enigma in the area of fluid mechanics. The conventional explanation of the phenomenon is based on the instability of the shear flow with respect to infinitesimal disturbances. The conventional hydrodynamic stability theory deals with the analysis of normal modes that might be unstable. The latter circumstance is accompanied by an exponential growth of the disturbances that might lead to laminar-turbulent transition. Nevertheless, in many cases, the transition scenario bypasses the exponential growth stage associated with the normal modes. This type of transition is called bypass transition. An understanding of the phenomenon has eluded us to this day. One possibility is that bypass transition is associated with so-called algebraic (non-modal) growth of disturbances in shear flows. In the present work, an analysis of the optimal disturbances/streamwise vortices associated with the transient growth mechanism is performed for boundary layers in the presence of a streamwise <span class="hlt">pressure</span> <span class="hlt">gradient</span>. The theory will provide the optimal spacing of the control elements in the spanwise direction and their placement in the streamwise direction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AIPC.1685f0005Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AIPC.1685f0005Z"><span><span class="hlt">Acoustic</span> agglomeration of fine particles based on a high intensity <span class="hlt">acoustical</span> resonator</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Yun; Zeng, Xinwu; Tian, Zhangfu</p> <p>2015-10-01</p> <p><span class="hlt">Acoustic</span> agglomeration (AA) is considered to be a promising method for reducing the air pollution caused by fine aerosol particles. Removal efficiency and energy consuming are primary parameters and generally have a conflict with each other for the industry applications. It was proved that removal efficiency is increased with sound intensity and optimal frequency is presented for certain polydisperse aerosol. As a result, a high efficiency and low energy cost removal system was constructed using <span class="hlt">acoustical</span> resonance. High intensity standing wave is generated by a tube system with abrupt section driven by four loudspeakers. Numerical model of the tube system was built base on the finite element method, and the resonance condition and SPL increase were confirmd. Extensive tests were carried out to investigate the <span class="hlt">acoustic</span> field in the agglomeration chamber. Removal efficiency of fine particles was tested by the comparison of filter paper mass and particle size distribution at different operating conditions including sound <span class="hlt">pressure</span> level (SPL), and frequency. The experimental study has demonstrated that agglomeration increases with sound <span class="hlt">pressure</span> level. Sound <span class="hlt">pressure</span> level in the agglomeration chamber is between 145 dB and 165 dB from 500 Hz to 2 kHz. The resonance frequency can be predicted with the quarter tube theory. Sound <span class="hlt">pressure</span> level gain of more than 10 dB is gained at resonance frequency. With the help of high intensity sound waves, fine particles are reduced greatly, and the AA effect is enhanced at high SPL condition. The optimal frequency is 1.1kHz for aerosol generated by coal ash. In the resonace tube, higher resonance frequencies are not the integral multiplies of the first one. As a result, Strong nonlinearity is avoided by the dissonant characteristic and shock wave is not found in the testing results. The mechanism and testing system can be used effectively in industrial processes in the future.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790025267','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790025267"><span>Survey and bibliography on attainment of laminar flow control in air using <span class="hlt">pressure</span> <span class="hlt">gradient</span> and suction, volume 1</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bushnell, D. M.; Tuttle, M. H.</p> <p>1979-01-01</p> <p>A survey was conducted and a bibliography compiled on attainment of laminar flow in air through the use of favorable <span class="hlt">pressure</span> <span class="hlt">gradient</span> and suction. This report contains the survey, summaries of data for both ground and flight experiments, and abstracts of referenced reports. Much early information is also included which may be of some immediate use as background material for LFC applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19830027510','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19830027510"><span><span class="hlt">Acoustic</span> bubble removal method</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Trinh, E. H.; Elleman, D. D.; Wang, T. G. (Inventor)</p> <p>1983-01-01</p> <p>A method is described for removing bubbles from a liquid bath such as a bath of molten glass to be used for optical elements. Larger bubbles are first removed by applying <span class="hlt">acoustic</span> energy resonant to a bath dimension to drive the larger bubbles toward a <span class="hlt">pressure</span> well where the bubbles can coalesce and then be more easily removed. Thereafter, submillimeter bubbles are removed by applying <span class="hlt">acoustic</span> energy of frequencies resonant to the small bubbles to oscillate them and thereby stir liquid immediately about the bubbles to facilitate their breakup and absorption into the liquid.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhFl...30c7103B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhFl...30c7103B"><span>Numerical study of droplet evaporation in an <span class="hlt">acoustic</span> levitator</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bänsch, Eberhard; Götz, Michael</p> <p>2018-03-01</p> <p>We present a finite element method for the simulation of all relevant processes of the evaporation of a liquid droplet suspended in an <span class="hlt">acoustic</span> levitation device. The mathematical model and the numerical implementation take into account heat and mass transfer across the interface between the liquid and gaseous phase and the influence of <span class="hlt">acoustic</span> streaming on this process, as well as the displacement and deformation of the droplet due to <span class="hlt">acoustic</span> radiation <span class="hlt">pressure</span>. We apply this numerical method to several theoretical and experimental examples and compare our results with the well-known d2-law for the evaporation of spherical droplets and with theoretical predictions for the <span class="hlt">acoustic</span> streaming velocity. We study the influence of <span class="hlt">acoustic</span> streaming on the distribution of water vapor and temperature in the levitation device, with special attention to the vapor distribution in the emerging toroidal vortices. We also compare the evaporation rate of a droplet with and without <span class="hlt">acoustic</span> streaming, as well as the evaporation rates in dependence of different temperatures and sound <span class="hlt">pressure</span> levels. Finally, a simple model of protein inactivation due to heat damage is considered and studied for different evaporation settings and their respective influence on protein damage.</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/servlets/purl/871545','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/871545"><span>Method and apparatus for sizing and separating warp yarns using <span class="hlt">acoustical</span> energy</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Sheen, Shuh-Haw; Chien, Hual-Te; Raptis, Apostolos C.; Kupperman, David S.</p> <p>1998-01-01</p> <p>A slashing process for preparing warp yarns for weaving operations including the steps of sizing and/or desizing the yarns in an <span class="hlt">acoustic</span> resonance box and separating the yarns with a leasing apparatus comprised of a set of <span class="hlt">acoustically</span> agitated lease rods. The sizing step includes immersing the yarns in a size solution contained in an <span class="hlt">acoustic</span> resonance box. <span class="hlt">Acoustic</span> transducers are positioned against the exterior of the box for generating an <span class="hlt">acoustic</span> <span class="hlt">pressure</span> field within the size solution. Ultrasonic waves that result from the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> field continuously agitate the size solution to effect greater mixing and more uniform application and penetration of the size onto the yarns. The sized yarns are then separated by passing the warp yarns over and under lease rods. Electroacoustic transducers generate <span class="hlt">acoustic</span> waves along the longitudinal axis of the lease rods, creating a shearing motion on the surface of the rods for splitting the yarns.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/644409','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/644409"><span>Method and apparatus for sizing and separating warp yarns using <span class="hlt">acoustical</span> energy</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Sheen, S.H.; Chien, H.T.; Raptis, A.C.; Kupperman, D.S.</p> <p>1998-05-19</p> <p>A slashing process is disclosed for preparing warp yarns for weaving operations including the steps of sizing and/or desizing the yarns in an <span class="hlt">acoustic</span> resonance box and separating the yarns with a leasing apparatus comprised of a set of <span class="hlt">acoustically</span> agitated lease rods. The sizing step includes immersing the yarns in a size solution contained in an <span class="hlt">acoustic</span> resonance box. <span class="hlt">Acoustic</span> transducers are positioned against the exterior of the box for generating an <span class="hlt">acoustic</span> <span class="hlt">pressure</span> field within the size solution. Ultrasonic waves that result from the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> field continuously agitate the size solution to effect greater mixing and more uniform application and penetration of the size onto the yarns. The sized yarns are then separated by passing the warp yarns over and under lease rods. Electroacoustic transducers generate <span class="hlt">acoustic</span> waves along the longitudinal axis of the lease rods, creating a shearing motion on the surface of the rods for splitting the yarns. 2 figs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApPhL.112e3902J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApPhL.112e3902J"><span>Dynamic Leidenfrost temperature on micro-textured surfaces: <span class="hlt">Acoustic</span> wave absorption into thin vapor layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jerng, Dong Wook; Kim, Dong Eok</p> <p>2018-01-01</p> <p>The dynamic Leidenfrost phenomenon is governed by three types of <span class="hlt">pressure</span> potentials induced via vapor hydrodynamics, liquid dynamic <span class="hlt">pressure</span>, and the water hammer effect resulting from the generation of <span class="hlt">acoustic</span> waves at the liquid-vapor interface. The prediction of the Leidenfrost temperature for a dynamic droplet needs quantitative evaluation and definition for each of the <span class="hlt">pressure</span> fields. In particular, the textures on a heated surface can significantly affect the vapor hydrodynamics and the water hammer <span class="hlt">pressure</span>. We present a quantitative model for evaluating the water hammer <span class="hlt">pressure</span> on micro-textured surfaces taking into account the absorption of <span class="hlt">acoustic</span> waves into the thin vapor layer. The model demonstrates that the strength of the <span class="hlt">acoustic</span> flow into the liquid droplet, which directly contributes to the water hammer <span class="hlt">pressure</span>, depends on the magnitude of the <span class="hlt">acoustic</span> resistance (impedance) in the droplet and the vapor region. In consequence, the micro-textures of the surface and the increased spacing between them reduce the water hammer coefficient ( kh ) defined as the ratio of the <span class="hlt">acoustic</span> flow into the droplet to total generated flow. Aided by numerical calculations that solve the laminar Navier-Stokes equation for the vapor flow, we also predict the dynamic Leidenfrost temperature on a micro-textured surface with reliable accuracy consistent with the experimental data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003APS..DFD.JL012W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003APS..DFD.JL012W"><span>A Method for Large Eddy Simulation of <span class="hlt">Acoustic</span> Combustion Instabilities</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wall, Clifton; Moin, Parviz</p> <p>2003-11-01</p> <p>A method for performing Large Eddy Simulation of <span class="hlt">acoustic</span> combustion instabilities is presented. By extending the low Mach number <span class="hlt">pressure</span> correction method to the case of compressible flow, a numerical method is developed in which the Poisson equation for <span class="hlt">pressure</span> is replaced by a Helmholtz equation. The method avoids the <span class="hlt">acoustic</span> CFL condition by using implicit time advancement, leading to large efficiency gains at low Mach number. The method also avoids artificial damping of <span class="hlt">acoustic</span> waves. The numerical method is attractive for the simulation of <span class="hlt">acoustics</span> combustion instabilities, since these flows are typically at low Mach number, and the <span class="hlt">acoustic</span> frequencies of interest are usually low. Additionally, new boundary conditions based on the work of Poinsot and Lele have been developed to model the <span class="hlt">acoustic</span> effect of a long channel upstream of the computational inlet, thus avoiding the need to include such a channel in the computational domain. The turbulent combustion model used is the Level Set model of Duchamp de Lageneste and Pitsch for premixed combustion. Comparison of LES results to the reacting experiments of Besson et al. will be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080015546','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080015546"><span>Post Test Evaluation of HSCT Nozzle <span class="hlt">Acoustic</span> Liner Subcomponents Subjected to a Hot <span class="hlt">Acoustic</span> Durability Test</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Verrilli, Michael J.; Lee, Kuan</p> <p>2008-01-01</p> <p>The <span class="hlt">acoustic</span> liner system designed for use in the High Speed Civil Transport (HSCT) was tested in a thermal-<span class="hlt">acoustic</span> environment. Five ceramic matrix composite (CMC) <span class="hlt">acoustic</span> tile configurations, five bulk <span class="hlt">acoustic</span> absorbers, and one thermal protection system design were tested. The CMC <span class="hlt">acoustic</span> tiles were subjected to two 2 3/4 hr ambient temperature <span class="hlt">acoustic</span> exposures to measure their dynamic response. One exposure was conducted on the tiles alone and the second exposure included the tiles and the T-foam bulk absorber. The measured tile RMS strains were small. With or without the T-foam absorber, the dynamic strains were below strain levels that would cause damage during fatigue loading. After the ambient exposure, a 75-hr durability test of the entire <span class="hlt">acoustic</span> liner system was conducted using a thermal-<span class="hlt">acoustic</span> cycle that approximated the anticipated service cycle. <span class="hlt">Acoustic</span> loads up to 139 dB/Hz and temperatures up to 1670 F (910 C) were employed during this 60 cycle test. During the durability test, the CMC tiles were exposed to temperatures up to 1780 F and a transient through thickness <span class="hlt">gradient</span> up to 490 F. The TPS peak temperatures on the hot side of the panels ranged from 750 to 1000 F during the 60 cycles. The through thickness delta T ranged from 450 to 650 F, varying with TPS location and cycle number. No damage, such as cracks or chipping, was observed in the CMC tiles after completion of the testing. However, on tile warped during the durability test and was replaced after 43 or 60 cycles. No externally observed damage was found in this tile. No failure of the CMC fasteners occurred, but damage was observed. Cracks and missing material occurred, only in the fastener head region. No indication of damage was observed in the T-foam <span class="hlt">acoustic</span> absorbers. The SiC foam <span class="hlt">acoustic</span> absorber experienced damage after about 43 cycles. Cracking in the TPS occurred around the attachment holes and under a vent. In spite of the development of damage, the TPS maintained</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29439881','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29439881"><span>Prospective assessment of the frequency of low <span class="hlt">gradient</span> severe aortic stenosis with preserved left ventricular ejection fraction: Critical impact of aortic flow misalignment and <span class="hlt">pressure</span> recovery phenomenon.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ringle, Anne; Castel, Anne-Laure; Le Goffic, Caroline; Delelis, François; Binda, Camille; Bohbot, Yohan; Ennezat, Pierre Vladimir; Guerbaai, Raphaëlle A; Levy, Franck; Vincentelli, André; Graux, Pierre; Tribouilloy, Christophe; Maréchaux, Sylvestre</p> <p>2018-02-10</p> <p>The frequency of paradoxical low-<span class="hlt">gradient</span> severe aortic stenosis (AS) varies widely across studies. The impact of misalignment of aortic flow and <span class="hlt">pressure</span> recovery phenomenon on the frequency of low-<span class="hlt">gradient</span> severe AS with preserved left ventricular ejection fraction (LVEF) has not been evaluated in prospective studies. To investigate prospectively the impact of aortic flow misalignment by Doppler and lack of <span class="hlt">pressure</span> recovery phenomenon correction on the frequency of low-<span class="hlt">gradient</span> (LG) severe aortic stenosis (AS) with preserved LVEF. Aortic jet velocities and mean <span class="hlt">pressure</span> <span class="hlt">gradient</span> (MPG) were obtained by interrogating all windows in 68 consecutive patients with normal LVEF and severe AS (aortic valve area [AVA] ≤1cm 2 ) on the basis of the apical imaging window alone (two-dimensional [2D] apical approach). Patients were classified as having LG or high-<span class="hlt">gradient</span> (HG) AS according to MPG <40mmHg or ≥40mmHg, and normal flow (NF) or low flow (LF) according to stroke volume index >35mL/m 2 or ≤35mL/m 2 , on the basis of the 2D apical approach, the multiview approach (multiple windows evaluation) and AVA corrected for <span class="hlt">pressure</span> recovery. The proportion of LG severe AS was 57% using the 2D apical approach alone. After the multiview approach and correction for <span class="hlt">pressure</span> recovery, the proportion of LG severe AS decreased from 57% to 13% (LF-LG severe AS decreased from 23% to 3%; NF-LG severe AS decreased from 34% to 10%). As a result, 25% of patients were reclassified as having HG severe AS (AVA ≤1cm 2 and MPG ≥40mmHg) and 19% as having moderate AS. Hence, 77% of patients initially diagnosed with LG severe AS did not have "true" LG severe AS when the multiview approach and the <span class="hlt">pressure</span> recovery phenomenon correction were used. Aortic flow misevaluation, resulting from lack of use of multiple windows evaluation and <span class="hlt">pressure</span> recovery phenomenon correction, accounts for a large proportion of incorrectly graded AS and considerable overestimation of the frequency of LG</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2680658','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2680658"><span>Customization of the <span class="hlt">acoustic</span> field produced by a piezoelectric array through interelement delays</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Chitnis, Parag V.; Barbone, Paul E.; Cleveland, Robin O.</p> <p>2008-01-01</p> <p>A method for producing a prescribed <span class="hlt">acoustic</span> <span class="hlt">pressure</span> field from a piezoelectric array was investigated. The array consisted of 170 elements placed on the inner surface of a 15 cm radius spherical cap. Each element was independently driven by using individual pulsers each capable of generating 1.2 kV. <span class="hlt">Acoustic</span> field customization was achieved by independently controlling the time when each element was excited. The set of time delays necessary to produce a particular <span class="hlt">acoustic</span> field was determined by using an optimization scheme. The <span class="hlt">acoustic</span> field at the focal plane was simulated by using the angular spectrum method, and the optimization searched for the time delays that minimized the least squared difference between the magnitudes of the simulated and desired <span class="hlt">pressure</span> fields. The <span class="hlt">acoustic</span> field was shaped in two different ways: the −6 dB focal width was increased to different desired widths and the ring-shaped <span class="hlt">pressure</span> distributions of various prescribed diameters were produced. For both cases, the set of delays resulting from the respective optimization schemes were confirmed to yield the desired <span class="hlt">pressure</span> distributions by using simulations and measurements. The simulations, however, predicted peak positive <span class="hlt">pressures</span> roughly half those obtained from the measurements, which was attributed to the exclusion of nonlinearity in the simulations. PMID:18537369</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28929163','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28929163"><span><span class="hlt">Acoustic</span> tweezing of particles using decaying opposing travelling surface <span class="hlt">acoustic</span> waves (DOTSAW).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ng, Jia Wei; Devendran, Citsabehsan; Neild, Adrian</p> <p>2017-10-11</p> <p>Surface <span class="hlt">acoustic</span> waves offer a versatile and biocompatible method of manipulating the location of suspended particles or cells within microfluidic systems. The most common approach uses the interference of identical frequency, counter propagating travelling waves to generate a standing surface <span class="hlt">acoustic</span> wave, in which particles migrate a distance less than half the <span class="hlt">acoustic</span> wavelength to their nearest <span class="hlt">pressure</span> node. The result is the formation of a periodic pattern of particles. Subsequent displacement of this pattern, the prerequisite for tweezing, can be achieved by translation of the standing wave, and with it the <span class="hlt">pressure</span> nodes; this requires changing either the frequency of the pair of waves, or their relative phase. Here, in contrast, we examine the use of two counterpropagating traveling waves of different frequency. The non-linearity of the <span class="hlt">acoustic</span> forces used to manipulate particles, means that a small frequency difference between the two waves creates a substantially different force field, which offers significant advantages. Firstly, this approach creates a much longer range force field, in which migration takes place across multiple wavelengths, and causes particles to be gathered together in a single trapping site. Secondly, the location of this single trapping site can be controlled by the relative amplitude of the two waves, requiring simply an attenuation of one of the electrical drive signals. Using this approach, we show that by controlling the powers of the opposing incoherent waves, 5 μm particles can be migrated laterally across a fluid flow to defined locations with an accuracy of ±10 μm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860013901','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860013901"><span>Free-jet feasibility study of a thermal <span class="hlt">acoustic</span> shield concept for AST/VCE application-dual stream nozzles. Comprehensive data report. Volume 2: Laser velocimeter and suppressor. Base <span class="hlt">pressure</span> data</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Janardan, B. A.; Brausch, J. F.; Price, A. O.</p> <p>1984-01-01</p> <p><span class="hlt">Acoustic</span> and diagnostic data that were obtained to determine the influence of selected geometric and aerodynamic flow variables of coannular nozzles with thermal <span class="hlt">acoustic</span> shields are summarized in this comprehensive data report. A total of 136 static and simulated flight <span class="hlt">acoustic</span> test points were conducted with 9 scale-model nozzles. Aerodynamic laser velocimeter measurements were made for four selected plumes. In addition, static <span class="hlt">pressure</span> data in the chute base region of the suppressor configurations were obtained to assess the influence of the shield stream on the suppressor base drag.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820021986','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820021986"><span><span class="hlt">Acoustic</span> tooth cleaner</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Heyman, J. S. (Inventor)</p> <p>1982-01-01</p> <p>An <span class="hlt">acoustic</span> oral hygiene unit is described that uses <span class="hlt">acoustic</span> energy to oscillate mild abrasive particles in a water suspension which is then directed in a low <span class="hlt">pressure</span> stream onto the teeth. The oscillating abrasives scrub the teeth clean removing food particles, plaque, calculous, and other foreign material from tooth surfaces, interproximal areas, and tooth-gingiva interface more effectively than any previous technique. The relatively low power output and the basic design makes the invention safe and convenient for everyday use in the home without special training. This invention replaces all former means of home dental prophylaxis, and requires no augmentation to fulfill all requirements for daily oral hygienic care.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26070191','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26070191"><span>Radiation dominated acoustophoresis driven by surface <span class="hlt">acoustic</span> waves.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Guo, Jinhong; Kang, Yuejun; Ai, Ye</p> <p>2015-10-01</p> <p>Acoustophoresis-based particle manipulation in microfluidics has gained increasing attention in recent years. Despite the fact that experimental studies have been extensively performed to demonstrate this technique for various microfluidic applications, numerical simulation of acoustophoresis driven by surface <span class="hlt">acoustic</span> waves (SAWs) has still been largely unexplored. In this work, a numerical model taking into account the <span class="hlt">acoustic</span>-piezoelectric interaction was developed to simulate the generation of a standing surface <span class="hlt">acoustic</span> wave (SSAW) field and predict the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> field in the liquid. <span class="hlt">Acoustic</span> radiation dominated particle tracing was performed to simulate acoustophoresis of particles with different sizes undergoing a SSAW field. A microfluidic device composed of two interdigital transducers (IDTs) for SAW generation and a microfluidic channel was fabricated for experimental validation. Numerical simulations could well capture the focusing phenomenon of particles to the <span class="hlt">pressure</span> nodes in the experimental observation. Further comparison of particle trajectories demonstrated considerably quantitative agreement between numerical simulations and experimental results with fitting in the applied voltage. Particle switching was also demonstrated using the fabricated device that could be further developed as an active particle sorting device. Copyright © 2015 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29152026','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29152026"><span>Particle separation by phase modulated surface <span class="hlt">acoustic</span> waves.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Simon, Gergely; Andrade, Marco A B; Reboud, Julien; Marques-Hueso, Jose; Desmulliez, Marc P Y; Cooper, Jonathan M; Riehle, Mathis O; Bernassau, Anne L</p> <p>2017-09-01</p> <p>High efficiency isolation of cells or particles from a heterogeneous mixture is a critical processing step in lab-on-a-chip devices. <span class="hlt">Acoustic</span> techniques offer contactless and label-free manipulation, preserve viability of biological cells, and provide versatility as the applied electrical signal can be adapted to various scenarios. Conventional <span class="hlt">acoustic</span> separation methods use time-of-flight and achieve separation up to distances of quarter wavelength with limited separation power due to slow <span class="hlt">gradients</span> in the force. The method proposed here allows separation by half of the wavelength and can be extended by repeating the modulation pattern and can ensure maximum force acting on the particles. In this work, we propose an optimised phase modulation scheme for particle separation in a surface <span class="hlt">acoustic</span> wave microfluidic device. An expression for the <span class="hlt">acoustic</span> radiation force arising from the interaction between <span class="hlt">acoustic</span> waves in the fluid was derived. We demonstrated, for the first time, that the expression of the <span class="hlt">acoustic</span> radiation force differs in surface <span class="hlt">acoustic</span> wave and bulk devices, due to the presence of a geometric scaling factor. Two phase modulation schemes are investigated theoretically and experimentally. Theoretical findings were experimentally validated for different mixtures of polystyrene particles confirming that the method offers high selectivity. A Monte-Carlo simulation enabled us to assess performance in real situations, including the effects of particle size variation and non-uniform <span class="hlt">acoustic</span> field on sorting efficiency and purity, validating the ability to separate particles with high purity and high resolution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JSV...394..237T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JSV...394..237T"><span>Coherent entropy induced and <span class="hlt">acoustic</span> noise separation in compact nozzles</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tao, Wenjie; Schuller, Thierry; Huet, Maxime; Richecoeur, Franck</p> <p>2017-04-01</p> <p>A method to separate entropy induced noise from an <span class="hlt">acoustic</span> <span class="hlt">pressure</span> wave in an harmonically perturbed flow through a nozzle is presented. It is tested on an original experimental setup generating simultaneously <span class="hlt">acoustic</span> and temperature fluctuations in an air flow that is accelerated by a convergent nozzle. The setup mimics the direct and indirect noise contributions to the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> field in a confined combustion chamber by producing synchronized <span class="hlt">acoustic</span> and temperature fluctuations, without dealing with the complexity of the combustion process. It allows generating temperature fluctuations with amplitude up to 10 K in the frequency range from 10 to 100 Hz. The noise separation technique uses experiments with and without temperature fluctuations to determine the relative level of <span class="hlt">acoustic</span> and entropy fluctuations in the system and to identify the nozzle response to these forcing waves. It requires multi-point measurements of <span class="hlt">acoustic</span> <span class="hlt">pressure</span> and temperature. The separation method is first validated with direct numerical simulations of the nonlinear Euler equations. These simulations are used to investigate the conditions for which the separation technique is valid and yield similar trends as the experiments for the investigated flow operating conditions. The separation method then gives successfully the <span class="hlt">acoustic</span> reflection coefficient but does not recover the same entropy reflection coefficient as predicted by the compact nozzle theory due to the sensitivity of the method to signal noises in the explored experimental conditions. This methodology provides a framework for experimental investigation of direct and indirect combustion noises originating from synchronized perturbations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110024051','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110024051"><span><span class="hlt">Acoustic</span> and Vibration Environment for Crew Launch Vehicle Mobile Launcher</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vu, Bruce T.</p> <p>2007-01-01</p> <p>A launch-induced <span class="hlt">acoustic</span> environment represents a dynamic load on the exposed facilities and ground support equipment (GSE) in the form of random <span class="hlt">pressures</span> fluctuating around the ambient atmospheric <span class="hlt">pressure</span>. In response to these fluctuating <span class="hlt">pressures</span>, structural vibrations are generated and transmitted throughout the structure and to the equipment items supported by the structure. Certain equipment items are also excited by the direct <span class="hlt">acoustic</span> input as well as by the vibration transmitted through the supporting structure. This paper presents the predicted <span class="hlt">acoustic</span> and vibration environments induced by the launch of the Crew Launch Vehicle (CLV) from Launch Complex (LC) 39. The predicted <span class="hlt">acoustic</span> environment depicted in this paper was calculated by scaling the statistically processed measured data available from Saturn V launches to the anticipated environment of the CLV launch. The scaling was accomplished by using the 5-segment Solid Rocket Booster (SRB) engine parameters. Derivation of vibration environment for various Mobile Launcher (ML) structures throughout the base and tower was accomplished by scaling the Saturn V vibration environment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810026299&hterms=Acoustic+levitation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DAcoustic%2Blevitation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810026299&hterms=Acoustic+levitation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DAcoustic%2Blevitation"><span>Some limitations on processing materials in <span class="hlt">acoustic</span> levitation devices</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Oran, W. A.; Witherow, W. K.; Ross, B. B.; Rush, J. E.</p> <p>1979-01-01</p> <p>The spot heating of samples, suspended in an <span class="hlt">acoustic</span> field, was investigated to determine if the technique could be used to process materials. A single axis resonance device operating in air at 25 C with an rms <span class="hlt">pressure</span> maximum of 160 to 170 db was used in the experiments. The heat flow from a hot object suspended in a levitation node is dominated by the effects of the field, with the heat loss approximately 20 times larger than that due to natural convection. The <span class="hlt">acoustic</span> forces which suspend the body at a node also serve to eject the heated air. The coupling between the locally heated region around the body and the <span class="hlt">acoustic</span> field results in instabilities in both the <span class="hlt">pressure</span> wave and force field. The investigations indicated the extreme difficulties in developing a materials processing device based on <span class="hlt">acoustic</span>/spot heating for use in a terrestrial environment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3778006','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3778006"><span>Selective <span class="hlt">Pressure</span> along a Latitudinal <span class="hlt">Gradient</span> Affects Subindividual Variation in Plants</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Sobral, Mar; Guitián, José; Guitián, Pablo; Larrinaga, Asier R.</p> <p>2013-01-01</p> <p>Individual plants produce repeated structures such as leaves, flowers or fruits, which, although belonging to the same genotype, are not phenotypically identical. Such subindividual variation reflects the potential of individual genotypes to vary with micro-environmental conditions. Furthermore, variation in organ traits imposes costs to foraging animals such as time, energy and increased predation risk. Therefore, animals that interact with plants may respond to this variation and affect plant fitness. Thus, phenotypic variation within an individual plant could be, in part, an adaptive trait. Here we investigated this idea and we found that subindividual variation of fruit size of Crataegus monogyna, in different populations throughout the latitudinal <span class="hlt">gradient</span> in Europe, was explained at some extent by the selective <span class="hlt">pressures</span> exerted by seed-dispersing birds. These findings support the hypothesis that within-individual variation in plants is an adaptive trait selected by interacting animals which may have important implications for plant evolution. PMID:24069297</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19800025708','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19800025708"><span>A feasibility study of a 3-D finite element solution scheme for aeroengine duct <span class="hlt">acoustics</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Abrahamson, A. L.</p> <p>1980-01-01</p> <p>The advantage from development of a 3-D model of aeroengine duct <span class="hlt">acoustics</span> is the ability to analyze axial and circumferential liner segmentation simultaneously. The feasibility of a 3-D duct <span class="hlt">acoustics</span> model was investigated using Galerkin or least squares element formulations combined with Gaussian elimination, successive over-relaxation, or conjugate <span class="hlt">gradient</span> solution algorithms on conventional scalar computers and on a vector machine. A least squares element formulation combined with a conjugate <span class="hlt">gradient</span> solver on a CDC Star vector computer initially appeared to have great promise, but severe difficulties were encountered with matrix ill-conditioning. These difficulties in conditioning rendered this technique impractical for realistic problems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19323864','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19323864"><span>Social class-related <span class="hlt">gradient</span> in the association of skeletal growth with blood <span class="hlt">pressure</span> among adolescent boys in India.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rao, Shobha; Apte, Priti</p> <p>2009-12-01</p> <p>In view of the fact that height differences between socio-economic groups are apparent early in childhood, it is of interest to examine whether skeletal growth is reflective of the social class <span class="hlt">gradient</span> in CVD risk. The present study examined blood <span class="hlt">pressure</span> levels, adiposity and growth of adolescent boys from high and low social classes. In a cross-sectional study, skeletal growth (height and sitting height), adiposity (weight, BMI and body fat) and blood <span class="hlt">pressure</span> levels of the adolescents were measured. Pune, India. Adolescent schoolboys (9-16 years) from high socio-economic (HSE; n 1146) and low socio-economic (LSE; n 932) class. LSE boys were thin, short and undernourished (mean BMI: 15.5 kg/m2 v. 19.3 kg/m2 in HSE boys, P = 0.00). Social <span class="hlt">gradient</span> was revealed in differing health risks. The prevalence of high systolic blood <span class="hlt">pressure</span> (HSBP) was high in HSE class (10.5 % v. 2.7 % in LSE class, P = 0.00) and was associated with adiposity, while the prevalence of high diastolic blood <span class="hlt">pressure</span> (HDBP) was high in LSE class (9.8 % v. 7.0 % in HSE class, P = 0.00) and had only a weak association with adiposity. Despite this, lower ratio of leg length to height was associated with significantly higher respective health risks, i.e. for HDBP in LSE class (OR = 1.99, 95 % CI 1.14, 3.47) and for HSBP in HSE class (OR = 1.69, 95 % CI 1.02, 2.77). As stunting in childhood is a major problem in India and Asia, the leg length to height indicator needs to be validated in different populations to understand CVD risks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MS%26E..232a2012C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MS%26E..232a2012C"><span><span class="hlt">Acoustical</span> contribution calculation and analysis of compressor shell based on <span class="hlt">acoustic</span> transfer vector method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Xiaol; Guo, Bei; Tuo, Jinliang; Zhou, Ruixin; Lu, Yang</p> <p>2017-08-01</p> <p>Nowadays, people are paying more and more attention to the noise reduction of household refrigerator compressor. This paper established a sound field bounded by compressor shell and ISO3744 standard field points. The <span class="hlt">Acoustic</span> Transfer Vector (ATV) in the sound field radiated by a refrigerator compressor shell were calculated which fits the test result preferably. Then the compressor shell surface is divided into several parts. Based on <span class="hlt">Acoustic</span> Transfer Vector approach, the sound <span class="hlt">pressure</span> contribution to the field points and the sound power contribution to the sound field of each part were calculated. To obtain the noise radiation in the sound field, the sound <span class="hlt">pressure</span> cloud charts were analyzed, and the contribution curves in different frequency of each part were acquired. Meanwhile, the sound power contribution of each part in different frequency was analyzed, to ensure those parts where contributes larger sound power. Through the analysis of <span class="hlt">acoustic</span> contribution, those parts where radiate larger noise on the compressor shell were determined. This paper provides a credible and effective approach on the structure optimal design of refrigerator compressor shell, which is meaningful in the noise and vibration reduction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25606963','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25606963"><span>Imaging of <span class="hlt">acoustic</span> fields using optical feedback interferometry.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bertling, Karl; Perchoux, Julien; Taimre, Thomas; Malkin, Robert; Robert, Daniel; Rakić, Aleksandar D; Bosch, Thierry</p> <p>2014-12-01</p> <p>This study introduces optical feedback interferometry as a simple and effective technique for the two-dimensional visualisation of <span class="hlt">acoustic</span> fields. We present imaging results for several <span class="hlt">pressure</span> distributions including those for progressive waves, standing waves, as well as the diffraction and interference patterns of the <span class="hlt">acoustic</span> waves. The proposed solution has the distinct advantage of extreme optical simplicity and robustness thus opening the way to a low cost <span class="hlt">acoustic</span> field imaging system based on mass produced laser diodes.</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/29342858','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29342858"><span>Novel Fiber-Optic Ring <span class="hlt">Acoustic</span> Emission Sensor.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wei, Peng; Han, Xiaole; Xia, Dong; Liu, Taolin; Lang, Hao</p> <p>2018-01-13</p> <p><span class="hlt">Acoustic</span> emission technology has been applied to many fields for many years. However, the conventional piezoelectric <span class="hlt">acoustic</span> emission sensors cannot be used in extreme environments, such as those with heavy electromagnetic interference, high <span class="hlt">pressure</span>, or strong corrosion. In this paper, a novel fiber-optic ring <span class="hlt">acoustic</span> emission sensor is proposed. The sensor exhibits high sensitivity, anti-electromagnetic interference, and corrosion resistance. First, the principle of a novel fiber-optic ring sensor is introduced. Different from piezoelectric and other fiber <span class="hlt">acoustic</span> emission sensors, this novel sensor includes both a sensing skeleton and a sensing fiber. Second, a heterodyne interferometric demodulating method is presented. In addition, a fiber-optic ring sensor <span class="hlt">acoustic</span> emission system is built based on this method. Finally, fiber-optic ring <span class="hlt">acoustic</span> emission experiments are performed. The novel fiber-optic ring sensor is glued onto the surface of an aluminum plate. The 150 kHz standard continuous sinusoidal signals and broken lead signals are successfully detected by the novel fiber-optic ring <span class="hlt">acoustic</span> emission sensor. In addition, comparison to the piezoelectric <span class="hlt">acoustic</span> emission sensor is performed, which shows the availability and reliability of the novel fiber-optic ring <span class="hlt">acoustic</span> emission sensor. In the future, this novel fiber-optic ring <span class="hlt">acoustic</span> emission sensor will provide a new route to <span class="hlt">acoustic</span> emission detection in harsh environments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920019479','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920019479"><span>Mobility power flow analysis of coupled plate structure subjected to mechanical and <span class="hlt">acoustic</span> excitation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cuschieri, J. M.</p> <p>1992-01-01</p> <p>The mobility power flow approach that was previously applied in the derivation of expressions for the vibrational power flow between coupled plate substructures forming an L configuration and subjected to mechanical loading is generalized. Using the generalized expressions, both point and distributed mechanical loads on one or both of the plates can be considered. The generalized approach is extended to deal with <span class="hlt">acoustic</span> excitation of one of the plate substructures. In this case, the forces (<span class="hlt">acoustic</span> <span class="hlt">pressures</span>) acting on the structure are dependent on the response of the structure because of the scattered <span class="hlt">pressure</span> component. The interaction between the plate structure and the <span class="hlt">acoustic</span> fluid leads to the derivation of a corrected mode shape for the plates' normal surface velocity and also for the structure mobility functions. The determination of the scattered <span class="hlt">pressure</span> components in the expressions for the power flow represents an additional component in the power flow balance for the source plate and the receiver plate. This component represents the radiated <span class="hlt">acoustical</span> power from the plate structure. For a number of coupled plate substrates, the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> generated by one substructure will interact with the motion of another substructure. That is, in the case of the L-shaped plate, <span class="hlt">acoustic</span> interaction exists between the two plate substructures due to the generation of the <span class="hlt">acoustic</span> waves by each of the substructures. An approach to deal with this phenomena is described.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MS%26E..281a2002X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MS%26E..281a2002X"><span>MEMS-based Optic Fiber Fabry-Perot Sensor for Underwater <span class="hlt">Acoustic</span> Measurement with A Wavelength-switched System</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xia, J.; Y Wang, F.; Luo, H.; Hu, Y. M.; Xiong, S. D.</p> <p>2017-12-01</p> <p>In this paper, a MEMS-based extrinsic Farby-Perot Interferometric (EFPI) <span class="hlt">acoustic</span> <span class="hlt">pressure</span> <span class="hlt">acoustic</span> sensor is presented. The diaphragm structure is used as the second reflected surface, and the sensitive surface to <span class="hlt">acoustic</span> <span class="hlt">pressure</span>. A wavelength-switched phase demodulation system for EFPI sensors is used for <span class="hlt">acoustic</span> signal recovery. The modified phase demodulation system has been demonstrated to recover the signal to a stable intensity fluctuation level of ±0.5 dB at the test frequency of 2000 Hz. In the test depth of 50cm, the sensor has a resonant frequency of 3.7 kHz, a flat frequency range of 10-800Hz, and a corresponding <span class="hlt">acoustic</span> <span class="hlt">pressure</span> sensitivity of -159 dB re. 1/μPa.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.2564T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.2564T"><span>Microseismicity Induced by Fluid <span class="hlt">Pressure</span> Drop (Laboratory Study)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Turuntaev, Sergey; Zenchenko, Evgeny; Melchaeva, Olga</p> <p>2013-04-01</p> <p>Pore <span class="hlt">pressure</span> change in saturated porous rocks may result in its fracturing (Maury et Fourmaintraux, 1993) and corresponding microseismic event occurrences. Microseismicity due to fluid injection is considered in numerous papers (Maxwell, 2010, Shapiro et al., 2005). Another type of the porous medium fracturing is related with rapid pore <span class="hlt">pressure</span> drop at some boundary. The mechanism of such fracturing was considered by (Khristianovich, 1985) as a model of sudden coal blowing and by (Alidibirov, Panov, 1998) as a model of volcano eruptions. If the porous saturated medium has a boundary where it directly contacted with fluid under the high <span class="hlt">pressure</span> (in a hydraulic fracture or in a borehole), and the <span class="hlt">pressure</span> at that boundary is dropped, the conditions for tensile cracks can be achieved at some distance from the boundary. In the paper, the results of experimental study of saturated porous sample fracturing due to pore <span class="hlt">pressure</span> rapid drop are discussed. The samples (82 mm high, ∅60 mm) were made of quartz sand, which was cemented by "liquid glass" glue with mass fraction 1%. The sample (porosity 35%, uniaxial unconfined compression strength 2.5 MPa) was placed in a mould and saturated by oil. The upper end of the sample contacted with the mould upper lid, the lower end contacted with fluid. The fluid <span class="hlt">pressure</span> was increased to 10 MPa and then discharged through the bottom nipple. The <span class="hlt">pressure</span> increases/drops were repeated 30-50 times. Pore <span class="hlt">pressure</span> and <span class="hlt">acoustic</span> emission (AE) were registered by transducers mounted into upper and bottom lids of the mould. It was found, that AE sources (corresponded to microfracturing) were spreading from the open end to the closed end of the sample, and that maximal number of AE events was registered at some distance from the opened end. The number of AE pulses increased with every next <span class="hlt">pressure</span> drop, meanwhile the number of pulses with high amplitudes diminished. It was found that AE maximal rate corresponded to the fluid <span class="hlt">pressure</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26964964','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26964964"><span>Scavenging dissolved oxygen via <span class="hlt">acoustic</span> droplet vaporization.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Radhakrishnan, Kirthi; Holland, Christy K; Haworth, Kevin J</p> <p>2016-07-01</p> <p><span class="hlt">Acoustic</span> droplet vaporization (ADV) of perfluorocarbon emulsions has been explored for diagnostic and therapeutic applications. Previous studies have demonstrated that vaporization of a liquid droplet results in a gas microbubble with a diameter 5-6 times larger than the initial droplet diameter. The expansion factor can increase to a factor of 10 in gassy fluids as a result of air diffusing from the surrounding fluid into the microbubble. This study investigates the potential of this process to serve as an ultrasound-mediated gas scavenging technology. Perfluoropentane droplets diluted in phosphate-buffered saline (PBS) were insonified by a 2 MHz transducer at peak rarefactional <span class="hlt">pressures</span> lower than and greater than the ADV <span class="hlt">pressure</span> amplitude threshold in an in vitro flow phantom. The change in dissolved oxygen (DO) of the PBS before and after ADV was measured. A numerical model of gas scavenging, based on conservation of mass and equal partial <span class="hlt">pressures</span> of gases at equilibrium, was developed. At insonation <span class="hlt">pressures</span> exceeding the ADV threshold, the DO of air-saturated PBS decreased with increasing insonation <span class="hlt">pressures</span>, dropping as low as 25% of air saturation within 20s. The decrease in DO of the PBS during ADV was dependent on the volumetric size distribution of the droplets and the fraction of droplets transitioned during ultrasound exposure. Numerically predicted changes in DO from the model agreed with the experimentally measured DO, indicating that concentration <span class="hlt">gradients</span> can explain this phenomenon. Using computationally modified droplet size distributions that would be suitable for in vivo applications, the DO of the PBS was found to decrease with increasing concentrations. This study demonstrates that ADV can significantly decrease the DO in an aqueous fluid, which may have direct therapeutic applications and should be considered for ADV-based diagnostic or therapeutic applications. Copyright © 2016 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4788814','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4788814"><span>Scavenging dissolved oxygen via <span class="hlt">acoustic</span> droplet vaporization</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Radhakrishnan, Kirthi; Holland, Christy K.; Haworth, Kevin J.</p> <p>2016-01-01</p> <p><span class="hlt">Acoustic</span> droplet vaporization (ADV) of perfluorocarbon emulsions has been explored for diagnostic and therapeutic applications. Previous studies have demonstrated that vaporization of a liquid droplet results in a gas microbubble with a diameter 5 to 6 times larger than the initial droplet diameter. The expansion factor can increase to a factor of 10 in gassy fluids as a result of air diffusing from the surrounding fluid into the microbubble. This study investigates the potential of this process to serve as an ultrasound-mediated gas scavenging technology. Perfluoropentane droplets diluted in phosphate-buffered saline (PBS) were insonified by a 2 MHz transducer at peak rarefactional <span class="hlt">pressures</span> lower than and greater than the ADV <span class="hlt">pressure</span> amplitude threshold in an in vitro flow phantom. The change in dissolved oxygen (DO) of the PBS before and after ADV was measured. A numerical model of gas scavenging, based on conservation of mass and equal partial <span class="hlt">pressures</span> of gases at equilibrium, was developed. At insonation <span class="hlt">pressures</span> exceeding the ADV threshold, the DO of air-saturated PBS decreased with increasing insonation <span class="hlt">pressures</span>, dropping as low as 25% of air saturation within 20 s. The decrease in DO of the PBS during ADV was dependent on the volumetric size distribution of the droplets and the fraction of droplets transitioned during ultrasound exposure. Numerically predicted changes in DO from the model agreed with the experimentally measured DO, indicating that concentration <span class="hlt">gradients</span> can explain this phenomenon. Using computationally modified droplet size distributions that would be suitable for in vivo applications, the DO of the PBS was found to decrease with increasing concentrations. This study demonstrates that ADV can significantly decrease the DO in an aqueous fluid, which may have direct therapeutic applications and should be considered for ADV-based diagnostic or therapeutic applications. PMID:26964964</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930091005','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930091005"><span>The Compressible Laminar Boundary Layer with Heat Transfer and Arbitrary <span class="hlt">Pressure</span> <span class="hlt">Gradient</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cohen, Clarence B; Reshotko, Eli</p> <p>1956-01-01</p> <p>An approximate method for the calculation of the compressible laminar boundary layer with heat transfer and arbitrary <span class="hlt">pressure</span> <span class="hlt">gradient</span>, based on Thwaites' correlation concept, is presented. With the definition of dimensionless shear and heat-transfer parameters and an assumed correlation of these parameters in terms of a momentum parameter, a complete system of relations for calculating skin friction and heat transfer results. Knowledge of velocity or temperature profiles is not necessary in using this calculation method. When the method is applied to a convergent-divergent, axially symmetric rocket nozzle, it shows that high rates of heat transfer are obtained at the initial stagnation point and at the throat of the nozzle. Also indicated are negative displacement thicknesses in the convergent portion of the nozzle; these occur because of the high density within the lower portions of the cooled boundary layer. (author)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19740014526','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19740014526"><span>Development of <span class="hlt">acoustically</span> lined ejector technology for multitube jet noise suppressor nozzles by model and engine tests over a wide range of jet <span class="hlt">pressure</span> ratios and temperatures</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Atvars, J.; Paynter, G. C.; Walker, D. Q.; Wintermeyer, C. F.</p> <p>1974-01-01</p> <p>An experimental program comprising model nozzle and full-scale engine tests was undertaken to acquire parametric data for <span class="hlt">acoustically</span> lined ejectors applied to primary jet noise suppression. Ejector lining design technology and <span class="hlt">acoustical</span> scaling of lined ejector configurations were the major objectives. Ground static tests were run with a J-75 turbojet engine fitted with a 37-tube, area ratio 3.3 suppressor nozzle and two lengths of ejector shroud (L/D = 1 and 2). Seven ejector lining configurations were tested over the engine <span class="hlt">pressure</span> ratio range of 1.40 to 2.40 with corresponding jet velocities between 305 and 610 M/sec. One-fourth scale model nozzles were tested over a <span class="hlt">pressure</span> ratio range of 1.40 to 4.0 with jet total temperatures between ambient and 1088 K. Scaling of multielement nozzle ejector configurations was also studied using a single element of the nozzle array with identical ejector lengths and lining materials. <span class="hlt">Acoustic</span> far field and near field data together with nozzle thrust performance and jet aerodynamic flow profiles are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20130000776&hterms=ares&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dares','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20130000776&hterms=ares&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dares"><span>Verification of Ares I Liftoff <span class="hlt">Acoustic</span> Environments via the Ares I Scale Model <span class="hlt">Acoustic</span> Test</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Counter, Douglas D.; Houston, Janice D.</p> <p>2012-01-01</p> <p>Launch environments, such as Liftoff <span class="hlt">Acoustic</span> (LOA) and Ignition Overpressure (IOP), are important design factors for any vehicle and are dependent upon the design of both the vehicle and the ground systems. The NASA Constellation Program had several risks to the development of the Ares I vehicle linked to LOA which are used in the development of the vibro-<span class="hlt">acoustic</span> environments. The risks included cost, schedule and technical impacts for component qualification due to high predicted vibro-<span class="hlt">acoustic</span> environments. One solution is to mitigate the environment at the component level. However, where the environment is too severe to mitigate at the component level, reduction of the launch environments is required. The Ares I Scale Model <span class="hlt">Acoustic</span> Test (ASMAT) program was implemented to verify the predicted Ares I launch environments and to determine the <span class="hlt">acoustic</span> reduction for the LOA environment with an above deck water sound suppression system. The test article included a 5% scale Ares I vehicle model, tower and Mobile Launcher. <span class="hlt">Acoustic</span> and <span class="hlt">pressure</span> data were measured by approximately 200 instruments. The ASMAT results are compared to the Ares I LOA predictions and water suppression effectiveness results are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27113387','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27113387"><span>Use of ecoacoustics to determine biodiversity patterns across ecological <span class="hlt">gradients</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Grant, Paul B C; Samways, Michael J</p> <p>2016-12-01</p> <p>The variety of local animal sounds characterizes a landscape. We used ecoacoustics to noninvasively assess the species richness of various biotopes typical of an ecofriendly forest plantation with diverse ecological <span class="hlt">gradients</span> and both nonnative and indigenous vegetation. The reference area was an adjacent large World Heritage Site protected area (PA). All sites were in a global biodiversity hotspot. Our results showed how taxa segregated into various biotopes. We identified 65 singing species, including birds, frogs, crickets, and katydids. Large, natural, protected grassland sites in the PA had the highest mean <span class="hlt">acoustic</span> diversity (14.1 species/site). Areas covered in nonnative timber or grass species were devoid of <span class="hlt">acoustic</span> species. Sites grazed by native and domestic megaherbivores were fairly rich (5.1) in <span class="hlt">acoustic</span> species but none were unique to this habitat type, where <span class="hlt">acoustic</span> diversity was greater than in intensively managed grassland sites (0.04). Natural vegetation patches inside the plantation mosaic supported high mean <span class="hlt">acoustic</span> diversity (indigenous forests 7.6, grasslands 8.0, wetlands 9.1), which increased as plant heterogeneity and patch size increased. Indigenous forest patches within the plantation mosaic contained a highly characteristic <span class="hlt">acoustic</span> species assemblage, emphasizing their complementary contribution to local biodiversity. Overall, <span class="hlt">acoustic</span> signals determined spatial biodiversity patterns and can be a useful tool for guiding conservation. © 2016 Society for Conservation Biology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27807249','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27807249"><span>Singing whales generate high levels of particle motion: implications for <span class="hlt">acoustic</span> communication and hearing?</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mooney, T Aran; Kaplan, Maxwell B; Lammers, Marc O</p> <p>2016-11-01</p> <p><span class="hlt">Acoustic</span> signals are fundamental to animal communication, and cetaceans are often considered bioacoustic specialists. Nearly all studies of their <span class="hlt">acoustic</span> communication focus on sound <span class="hlt">pressure</span> measurements, overlooking the particle motion components of their communication signals. Here we characterized the levels of <span class="hlt">acoustic</span> particle velocity (and <span class="hlt">pressure</span>) of song produced by humpback whales. We demonstrate that whales generate <span class="hlt">acoustic</span> fields that include significant particle velocity components that are detectable over relatively long distances sufficient to play a role in <span class="hlt">acoustic</span> communication. We show that these signals attenuate predictably in a manner similar to <span class="hlt">pressure</span> and that direct particle velocity measurements can provide bearings to singing whales. Whales could potentially use such information to determine the distance of signalling animals. Additionally, the vibratory nature of particle velocity may stimulate bone conduction, a hearing modality found in other low-frequency specialized mammals, offering a parsimonious mechanism of <span class="hlt">acoustic</span> energy transduction into the massive ossicles of whale ears. With substantial concerns regarding the effects of increasing anthropogenic ocean noise and major uncertainties surrounding mysticete hearing, these results highlight both an unexplored pathway that may be available for whale <span class="hlt">acoustic</span> communication and the need to better understand the biological role of <span class="hlt">acoustic</span> particle motion. © 2016 The Author(s).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5134030','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5134030"><span>Singing whales generate high levels of particle motion: implications for <span class="hlt">acoustic</span> communication and hearing?</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kaplan, Maxwell B.; Lammers, Marc O.</p> <p>2016-01-01</p> <p><span class="hlt">Acoustic</span> signals are fundamental to animal communication, and cetaceans are often considered bioacoustic specialists. Nearly all studies of their <span class="hlt">acoustic</span> communication focus on sound <span class="hlt">pressure</span> measurements, overlooking the particle motion components of their communication signals. Here we characterized the levels of <span class="hlt">acoustic</span> particle velocity (and <span class="hlt">pressure</span>) of song produced by humpback whales. We demonstrate that whales generate <span class="hlt">acoustic</span> fields that include significant particle velocity components that are detectable over relatively long distances sufficient to play a role in <span class="hlt">acoustic</span> communication. We show that these signals attenuate predictably in a manner similar to <span class="hlt">pressure</span> and that direct particle velocity measurements can provide bearings to singing whales. Whales could potentially use such information to determine the distance of signalling animals. Additionally, the vibratory nature of particle velocity may stimulate bone conduction, a hearing modality found in other low-frequency specialized mammals, offering a parsimonious mechanism of <span class="hlt">acoustic</span> energy transduction into the massive ossicles of whale ears. With substantial concerns regarding the effects of increasing anthropogenic ocean noise and major uncertainties surrounding mysticete hearing, these results highlight both an unexplored pathway that may be available for whale <span class="hlt">acoustic</span> communication and the need to better understand the biological role of <span class="hlt">acoustic</span> particle motion. PMID:27807249</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9708E..2BD','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9708E..2BD"><span>Taking advantage of <span class="hlt">acoustic</span> inhomogeneities in photoacoustic measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Da Silva, Anabela; Handschin, Charles; Riedinger, Christophe; Piasecki, Julien; Mensah, Serge; Litman, Amélie; Akhouayri, Hassan</p> <p>2016-03-01</p> <p>Photoacoustic offers promising perspectives in probing and imaging subsurface optically absorbing structures in biological tissues. The optical uence absorbed is partly dissipated into heat accompanied with microdilatations that generate <span class="hlt">acoustic</span> <span class="hlt">pressure</span> waves, the intensity which is related to the amount of fluuence absorbed. Hence the photoacoustic signal measured offers access, at least potentially, to a local monitoring of the absorption coefficient, in 3D if tomographic measurements are considered. However, due to both the diffusing and absorbing nature of the surrounding tissues, the major part of the uence is deposited locally at the periphery of the tissue, generating an intense <span class="hlt">acoustic</span> <span class="hlt">pressure</span> wave that may hide relevant photoacoustic signals. Experimental strategies have been developed in order to measure exclusively the photoacoustic waves generated by the structure of interest (orthogonal illumination and detection). Temporal or more sophisticated filters (wavelets) can also be applied. However, the measurement of this primary <span class="hlt">acoustic</span> wave carries a lot of information about the <span class="hlt">acoustically</span> inhomogeneous nature of the medium. We propose a protocol that includes the processing of this primary intense <span class="hlt">acoustic</span> wave, leading to the quantification of the surrounding medium sound speed, and, if appropriate to an <span class="hlt">acoustical</span> parametric image of the heterogeneities. This information is then included as prior knowledge in the photoacoustic reconstruction scheme to improve the localization and quantification.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1816b0002C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1816b0002C"><span>Full <span class="hlt">acoustic</span> and thermal characterization of HIFU field in the presence of a ribcage model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cao, Rui; Le, Nhan; Nabi, Ghulam; Huang, Zhihong</p> <p>2017-03-01</p> <p>In the treatment of abdominal organs using high intensity focused ultrasound (HIFU), the patient's ribs are in the pathway of the HIFU beams which could result in <span class="hlt">acoustic</span> distortion, occasional skin burns and insufficient energy delivered to the target organs. To provide full characterization of HIFU field with the influence of ribcage, the ribcage phantom reconstructed from a patient's CT images was created by tissue mimicking materials and its effect on <span class="hlt">acoustic</span> field was characterized. The effect of the ribcage on <span class="hlt">acoustic</span> field has been provided in <span class="hlt">acoustic</span> <span class="hlt">pressure</span> distribution, <span class="hlt">acoustic</span> power and focal temperature. Measurement result shows focus splitting with one main focus and two secondary intensity maxima. With the presence of ribcage phantom, the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> was reduced by 48.3% and another two peak values were observed near the main focus, reduced by 65.0% and 71.7% respectively. The <span class="hlt">acoustic</span> power was decreased by 47.5% to 52.5%. With these characterization results, the form of the focus, the <span class="hlt">acoustic</span> power, <span class="hlt">acoustic</span> <span class="hlt">pressure</span> and temperature rise are provided before the transcostal HIFU treatment, which are significant to determine the energy delivery dose. In conclusion, this ribcage model and characterization technique will be useful for the further study in the abdominal HIFU treatment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27810603','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27810603"><span>Overdrainage after ventriculoperitoneal shunting in a patient with a wide depressed skull bone defect: The effect of atmospheric <span class="hlt">pressure</span> <span class="hlt">gradient</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhou, Lixiang; Yu, Jinlu; Sun, Lichao; Han, Yanwu; Wang, Guangming</p> <p>2016-01-01</p> <p>In patients with traumatic brain injury, an effective approach for managing refractory intracranial hypertension is wide decompressive craniectomy. Postoperative hydrocephalus is a frequent complication requiring cerebrospinal fluid (CSF) diversion. A 50-year-old male who underwent decompressive craniectomy after traumatic brain injury. He developed hydrocephalus postoperatively, and accordingly we placed a ventriculoperitoneal shunt. However, an imbalance between the intra- and extra-cranial atmospheric <span class="hlt">pressures</span> led to overdrainage, and he suffered cognitive disorders and extremity weakness. He remained supine for 5days to avoid the effect of gravity on CSF diversion. After 20days, we performed a cranioplasty using a titanium plate. The postoperative course was uneventful, and the patient achieved satisfactory recovery. The gravitational effect and the atmospheric <span class="hlt">pressure</span> <span class="hlt">gradient</span> effect are two factors associated in the ventriculoperitoneal (VP) shunt treatment of hydrocephalus for the patient who had decompressive craniectomy. These effects can be eliminated by supine bed rest and cranioplasty. We herein emphasize the efficacy of VP shunt, supine bed rest and cranioplasty in treating hydrocephalus patients who have undergone craniectomy. A flexible application of these procedures to change the gravitational effect and the atmospheric <span class="hlt">pressure</span> <span class="hlt">gradient</span> effect should promote a favorable outcome. Copyright © 2016 The Authors. Published by Elsevier Ltd.. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110014600','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110014600"><span>The Development of the <span class="hlt">Acoustic</span> Design of NASA Glenn Research Center's New Reverberant <span class="hlt">Acoustic</span> Test Facility</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hughes, William O.; McNelis, Mark E.; Hozman, Aron D.; McNelis, Anne M.</p> <p>2011-01-01</p> <p>The National Aeronautics and Space Administration (NASA) Glenn Research Center (GRC) is leading the design and build of the new world-class vibroacoustic test capabilities at the NASA GRC s Plum Brook Station in Sandusky, Ohio. Benham Companies, LLC is currently constructing modal, base-shake sine and reverberant <span class="hlt">acoustic</span> test facilities to support the future testing needs of NASA s space exploration program. The large Reverberant <span class="hlt">Acoustic</span> Test Facility (RATF) will be approximately 101,000 ft3 in volume and capable of achieving an empty chamber <span class="hlt">acoustic</span> overall sound <span class="hlt">pressure</span> level (OASPL) of 163 dB. This combination of size and <span class="hlt">acoustic</span> power is unprecedented amongst the world s known active reverberant <span class="hlt">acoustic</span> test facilities. The key to achieving the expected <span class="hlt">acoustic</span> test spectra for a range of many NASA space flight environments in the RATF is the knowledge gained from a series of ground <span class="hlt">acoustic</span> tests. Data was obtained from several NASA-sponsored test programs, including testing performed at the National Research Council of Canada s <span class="hlt">acoustic</span> test facility in Ottawa, Ontario, Canada, and at the Redstone Technical Test Center <span class="hlt">acoustic</span> test facility in Huntsville, Alabama. The majority of these tests were performed to characterize the <span class="hlt">acoustic</span> performance of the modulators (noise generators) and representative horns that would be required to meet the desired spectra, as well as to evaluate possible supplemental gas jet noise sources. The knowledge obtained in each of these test programs enabled the design of the RATF sound generation system to confidently advance to its final <span class="hlt">acoustic</span> design and subsequent on-going construction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110014480','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110014480"><span>The Development of the <span class="hlt">Acoustic</span> Design of NASA Glenn Research Center's New Reverberant <span class="hlt">Acoustic</span> Test Facility</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hughes, William O.; McNelis, Mark E.; Hozman, Aron D.; McNelis, Anne M.</p> <p>2011-01-01</p> <p>The National Aeronautics and Space Administration (NASA) Glenn Research Center (GRC) is leading the design and build of the new world-class vibroacoustic test capabilities at the NASA GRC's Plum Brook Station in Sandusky, Ohio, USA. Benham Companies, LLC is currently constructing modal, base-shake sine and reverberant <span class="hlt">acoustic</span> test facilities to support the future testing needs of NASA s space exploration program. The large Reverberant <span class="hlt">Acoustic</span> Test Facility (RATF) will be approximately 101,000 ft3 in volume and capable of achieving an empty chamber <span class="hlt">acoustic</span> overall sound <span class="hlt">pressure</span> level (OASPL) of 163 dB. This combination of size and <span class="hlt">acoustic</span> power is unprecedented amongst the world s known active reverberant <span class="hlt">acoustic</span> test facilities. The key to achieving the expected <span class="hlt">acoustic</span> test spectra for a range of many NASA space flight environments in the RATF is the knowledge gained from a series of ground <span class="hlt">acoustic</span> tests. Data was obtained from several NASA-sponsored test programs, including testing performed at the National Research Council of Canada s <span class="hlt">acoustic</span> test facility in Ottawa, Ontario, Canada, and at the Redstone Technical Test Center <span class="hlt">acoustic</span> test facility in Huntsville, Alabama, USA. The majority of these tests were performed to characterize the <span class="hlt">acoustic</span> performance of the modulators (noise generators) and representative horns that would be required to meet the desired spectra, as well as to evaluate possible supplemental gas jet noise sources. The knowledge obtained in each of these test programs enabled the design of the RATF sound generation system to confidently advance to its final <span class="hlt">acoustic</span> design and subsequent on-going construction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060041530&hterms=torque&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dtorque','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060041530&hterms=torque&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dtorque"><span>A General <span class="hlt">Pressure</span> <span class="hlt">Gradient</span> Formulation for Ocean Models, Part 1: Scheme Design and Diagnostic Analysis, Part II: Energy, Momentum, and Bottom Torque Consistency</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Song, Y. T.</p> <p>1998-01-01</p> <p>A Jacobian formulation of the <span class="hlt">pressure</span> <span class="hlt">gradient</span> force for use in models with topography following coordinates is proposed. It can be used in conjunction with any vertical coordinate system and is easily implemented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800009039&hterms=topic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dtopic','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800009039&hterms=topic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dtopic"><span>Selected topics from the structural <span class="hlt">acoustics</span> program for the B-1 aircraft</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Belcher, P. M.</p> <p>1979-01-01</p> <p>The major elements of the structural <span class="hlt">acoustics</span> program for the B-1 aircraft are considered. <span class="hlt">Acoustic</span> <span class="hlt">pressures</span> measured at 280 sites on the surface of the vehicle were used to develop <span class="hlt">pressure</span> models for a resizing of airframe components for aircraft No. 4 (A/C4). <span class="hlt">Acoustical</span> fatigue design data for two dynamically complex structural configurations were acquired in laboratory programs, the conceptions for and executions of which detailed significant departures from the conventional. Design requirements for mechanical fasteners for configurations other than these two made use of analytical extensions of regrettably limited available information.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3355403','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3355403"><span><span class="hlt">Acoustic</span> Transmitters for Underwater Neutrino Telescopes</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ardid, Miguel; Martínez-Mora, Juan A.; Bou-Cabo, Manuel; Larosa, Giuseppina; Adrián-Martínez, Silvia; Llorens, Carlos D.</p> <p>2012-01-01</p> <p>In this paper <span class="hlt">acoustic</span> transmitters that were developed for use in underwater neutrino telescopes are presented. Firstly, an <span class="hlt">acoustic</span> transceiver has been developed as part of the <span class="hlt">acoustic</span> positioning system of neutrino telescopes. These infrastructures are not completely rigid and require a positioning system in order to monitor the position of the optical sensors which move due to sea currents. To guarantee a reliable and versatile system, the transceiver has the requirements of reduced cost, low power consumption, high <span class="hlt">pressure</span> withstanding (up to 500 bars), high intensity for emission, low intrinsic noise, arbitrary signals for emission and the capacity of acquiring and processing received signals. Secondly, a compact <span class="hlt">acoustic</span> transmitter array has been developed for the calibration of <span class="hlt">acoustic</span> neutrino detection systems. The array is able to mimic the signature of ultra-high-energy neutrino interaction in emission directivity and signal shape. The technique of parametric <span class="hlt">acoustic</span> sources has been used to achieve the proposed aim. The developed compact array has practical features such as easy manageability and operation. The prototype designs and the results of different tests are described. The techniques applied for these two <span class="hlt">acoustic</span> systems are so powerful and versatile that may be of interest in other marine applications using <span class="hlt">acoustic</span> transmitters. PMID:22666022</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_24 --> <div id="page_25" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="481"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18272454','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18272454"><span><span class="hlt">Acoustic</span> and vibrational damping in porous solids.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Göransson, Peter</p> <p>2006-01-15</p> <p>A porous solid may be characterized as an elastic-viscoelastic and <span class="hlt">acoustic</span>-viscoacoustic medium. For a flexible, open cell porous foam, the transport of energy is carried both through the sound <span class="hlt">pressure</span> waves propagating through the fluid in the pores, and through the elastic stress waves carried through the solid frame of the material. For a given situation, the balance between energy dissipated through vibration of the solid frame, changes in the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> and the coupling between the waves varies with the topological arrangement, choice of material properties, interfacial conditions, etc. Engineering of foams, i.e. designs built on systematic and continuous relationships between polymer chemistry, processing, micro-structure, is still a vision for the future. However, using state-of-the-art simulation techniques, multiple layer arrangements of foams may be tuned to provide <span class="hlt">acoustic</span> and vibrational damping at a low-weight penalty. In this paper, Biot's modelling of porous foams is briefly reviewed from an <span class="hlt">acoustics</span> and vibrations perspective with a focus on the energy dissipation mechanisms. Engineered foams will be discussed in terms of results from simulations performed using finite element solutions. A layered vehicle-type structure is used as an example.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3210749','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3210749"><span>Evaluation of Transmitral <span class="hlt">Pressure</span> <span class="hlt">Gradients</span> in the Intraoperative Echocardiographic Diagnosis of Mitral Stenosis after Mitral Valve Repair</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Segal, Scott; Fox, John A.; Eltzschig, Holger K.; Shernan, Stanton K.</p> <p>2011-01-01</p> <p>Objective Acute mitral stenosis (MS) following mitral valve (MV) repair is a rare but severe complication. We hypothesize that intraoperative echocardiography can be utilized to diagnose iatrogenic MS immediately after MV repair. Methods The medical records of 552 consecutive patients undergoing MV repair at a single institution were reviewed. Post-cardiopulmonary bypass peak and mean transmitral <span class="hlt">pressure</span> <span class="hlt">gradients</span> (TMPG), and <span class="hlt">pressure</span> half time (PHT) were obtained from intraoperative transesophageal echocardiographic (TEE) examinations in each patient. Results Nine patients (9/552 = 1.6%) received a reoperation for primary MS, prior to hospital discharge. Interestingly, all of these patients already showed intraoperative post-CPB mean and peak TMPGs that were significantly higher compared to values for those who did not: 10.7±4.8 mmHg vs 2.9±1.6 mmHg; p<0.0001 and 22.9±7.9 mmHg vs 7.6±3.7 mmHg; p<0.0001, respectively. However, PHT varied considerably (87±37 ms; range: 20–439 ms) within the entire population, and only weakly predicted the requirement for reoperation (113±56 vs. 87±37 ms, p = 0.034). Receiver operating characteristic curves showed strong discriminating ability for mean <span class="hlt">gradients</span> (AUC = 0.993) and peak <span class="hlt">gradients</span> (area under the curve, AUC = 0.996), but poor performance for PHT (AUC = 0.640). A value of ≥7 mmHg for mean, and ≥17 mmHg for peak TMPG, best separated patients who required reoperation for MS from those who did not. Conclusions Intraoperative TEE diagnosis of a peak TMPG ≥17 mmHg or mean TMPG ≥7 mmHg immediately following CPB are suggestive of clinically relevant MS after MV repair. PMID:22087230</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15749561','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15749561"><span><span class="hlt">Pressure</span>-dependent attenuation with microbubbles at low mechanical index.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tang, Meng-Xing; Eckersley, Robert J; Noble, J Alison</p> <p>2005-03-01</p> <p>It has previously been shown that the attenuation of ultrasound (US) by microbubble contrast agents is dependent on <span class="hlt">acoustic</span> <span class="hlt">pressure</span> (Chen et al. 2002). Although previous studies have modelled the <span class="hlt">pressure</span>-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 <span class="hlt">pressure</span>-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 <span class="hlt">acoustic</span> <span class="hlt">pressures</span>, a linear relationship between the attenuation of Sonovue, measured in dB, and the insonating <span class="hlt">acoustic</span> <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24008165','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24008165"><span>Radial mean arterial <span class="hlt">pressure</span> reliably reflects femoral mean arterial <span class="hlt">pressure</span> in uncomplicated pediatric cardiac surgery.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cetin, Secil; Pirat, Arash; Kundakci, Aycan; Camkiran, Aynur; Zeyneloglu, Pinar; Ozkan, Murat; Arslan, Gulnaz</p> <p>2014-02-01</p> <p>To see if radial mean arterial <span class="hlt">pressure</span> reliably reflects femoral mean arterial <span class="hlt">pressure</span> in uncomplicated pediatric cardiac surgery. An ethics committee-approved prospective interventional study. Operating room of a tertiary care hospital. Forty-five children aged 3 months to 4 years who underwent pediatric cardiac surgery with hypothermic cardiopulmonary bypass. Simultaneous femoral and radial arterial <span class="hlt">pressures</span> were recorded at 10-minute intervals intraoperatively. A <span class="hlt">pressure</span> <span class="hlt">gradient</span>>5mmHg was considered to be clinically significant. The patients' mean age was 14±11 months and and mean weight was 8.0±3.0kg. A total of 1,816 simultaneous measurements of arterial <span class="hlt">pressure</span> from the radial and femoral arteries were recorded during the pre-cardiopulmonary bypass, cardiopulmonary bypass, and post-cardiopulmonary bypass periods, including 520 (29%) systolic arterial <span class="hlt">pressures</span>, 520 (29%) diastolic arterial <span class="hlt">pressures</span>, and 776 (43%) mean arterial <span class="hlt">pressures</span>. The paired mean arterial <span class="hlt">pressure</span> measurements across the 3 periods were significantly and strongly correlated, and this was true for systolic arterial <span class="hlt">pressures</span> and diastolic arterial <span class="hlt">pressures</span> as well (r>0.93 and p<0.001 for all). Bland-Altman plots demonstrated good agreement between femoral and radial mean arterial <span class="hlt">pressures</span> during the pre-cardiopulmonary bypass, cardiopulmonary bypass, and post-cardiopulmonary bypass periods. A significant radial-to-femoral <span class="hlt">pressure</span> <span class="hlt">gradient</span> was observed in 150 (8%) of the total 1,816 measurements. These <span class="hlt">gradients</span> occurred most frequently between pairs of systolic arterial <span class="hlt">pressure</span> measurements (n = 113, 22% of all systolic arterial <span class="hlt">pressures</span>), followed by mean arterial <span class="hlt">pressure</span> measurements (n = 28, 4% of all mean arterial <span class="hlt">pressures</span>) and diastolic arterial <span class="hlt">pressures</span> measurements (n = 9, 2% of all diastolic arterial <span class="hlt">pressures</span>). These significant <span class="hlt">gradients</span> were not sustained (ie, were not recorded at 2 or more successive time points). The results suggested that radial mean</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28971512','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28971512"><span>Reduced <span class="hlt">acoustic</span> noise in diffusion tensor imaging on a compact MRI system.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tan, Ek T; Hardy, Christopher J; Shu, Yunhong; In, Myung-Ho; Guidon, Arnaud; Huston, John; Bernstein, Matt A; K F Foo, Thomas</p> <p>2018-06-01</p> <p>To investigate the feasibility of substantially reducing <span class="hlt">acoustic</span> noise while performing diffusion tensor imaging (DTI) on a compact 3T (C3T) MRI scanner equipped with a 42-cm inner-diameter asymmetric <span class="hlt">gradient</span>. A-weighted <span class="hlt">acoustic</span> measurements were made using 10 mT/m-amplitude sinusoidal waveforms, corresponding to echo-planar imaging (EPI) echo spacing of 0.25 to 5.0 ms, on a conventional, whole-body 3T MRI and on the C3T. <span class="hlt">Acoustic</span> measurements of DTI with trapezoidal EPI waveforms were then made at peak <span class="hlt">gradient</span> performance on the C3T (80 mT/m amplitude, 700 T/m/s slew rate) and at derated performance (33 mT/m, 10 to 50 T/m/s) for <span class="hlt">acoustic</span> noise reduction. DTI was acquired in two different phantoms and in seven human subjects, with and without <span class="hlt">gradient</span>-derating corresponding to multi- and single-shot acquisitions, respectively. Sinusoidal waveforms on the C3T were quieter by 8.5 to 15.6 A-weighted decibels (dBA) on average as compared to the whole-body MRI. The derated multishot DTI acquisition noise level was only 8.7 dBA (at 13 T/m/s slew rate) above ambient, and was quieter than non-derated, single-shot DTI by 22.3 dBA; however, the scan time was almost quadrupled. Although derating resulted in negligible diffusivity differences in the phantoms, small biases in diffusivity measurements were observed in human subjects (apparent diffusion coefficient = +9.3 ± 8.8%, fractional anisotropy = +3.2 ± 11.2%, radial diffusivity = +9.4 ± 16.8%, parallel diffusivity = +10.3 ± 8.4%). The feasibility of achieving reduced <span class="hlt">acoustic</span> noise levels with whole-brain DTI on the C3T MRI was demonstrated. Magn Reson Med 79:2902-2911, 2018. © 2017 International Society for Magnetic Resonance in Medicine. © 2017 International Society for Magnetic Resonance in Medicine.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23447010','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23447010"><span>Multi reflection of Lamb wave emission in an <span class="hlt">acoustic</span> waveguide sensor.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Schmitt, Martin; Olfert, Sergei; Rautenberg, Jens; Lindner, Gerhard; Henning, Bernd; Reindl, Leonhard Michael</p> <p>2013-02-27</p> <p>Recently, an <span class="hlt">acoustic</span> waveguide sensor based on multiple mode conversion of surface <span class="hlt">acoustic</span> waves at the solid-liquid interfaces has been introduced for the concentration measurement of binary and ternary mixtures, liquid level sensing, investigation of spatial inhomogenities or bubble detection. In this contribution the sound wave propagation within this <span class="hlt">acoustic</span> waveguide sensor is visualized by Schlieren imaging for continuous and burst operation the first time. In the <span class="hlt">acoustic</span> waveguide the antisymmetrical zero order Lamb wave mode is excited by a single phase transducer of 1 MHz on thin glass plates of 1 mm thickness. By contact to the investigated liquid Lamb waves propagating on the first plate emit <span class="hlt">pressure</span> waves into the adjacent liquid, which excites Lamb waves on the second plate, what again causes <span class="hlt">pressure</span> waves traveling inside the liquid back to the first plate and so on. The Schlieren images prove this multi reflection within the <span class="hlt">acoustic</span> waveguide, which confirms former considerations and calculations based on the receiver signal. With this knowledge the sensor concepts with the <span class="hlt">acoustic</span> waveguide sensor can be interpreted in a better manner.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3658713','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3658713"><span>Multi Reflection of Lamb Wave Emission in an <span class="hlt">Acoustic</span> Waveguide Sensor</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Schmitt, Martin; Olfert, Sergei; Rautenberg, Jens; Lindner, Gerhard; Henning, Bernd; Reindl, Leonhard Michael</p> <p>2013-01-01</p> <p>Recently, an <span class="hlt">acoustic</span> waveguide sensor based on multiple mode conversion of surface <span class="hlt">acoustic</span> waves at the solid—liquid interfaces has been introduced for the concentration measurement of binary and ternary mixtures, liquid level sensing, investigation of spatial inhomogenities or bubble detection. In this contribution the sound wave propagation within this <span class="hlt">acoustic</span> waveguide sensor is visualized by Schlieren imaging for continuous and burst operation the first time. In the <span class="hlt">acoustic</span> waveguide the antisymmetrical zero order Lamb wave mode is excited by a single phase transducer of 1 MHz on thin glass plates of 1 mm thickness. By contact to the investigated liquid Lamb waves propagating on the first plate emit <span class="hlt">pressure</span> waves into the adjacent liquid, which excites Lamb waves on the second plate, what again causes <span class="hlt">pressure</span> waves traveling inside the liquid back to the first plate and so on. The Schlieren images prove this multi reflection within the <span class="hlt">acoustic</span> waveguide, which confirms former considerations and calculations based on the receiver signal. With this knowledge the sensor concepts with the <span class="hlt">acoustic</span> waveguide sensor can be interpreted in a better manner. PMID:23447010</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008JFM...596..191B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008JFM...596..191B"><span>Dynamics of an <span class="hlt">acoustically</span> levitated particle using the lattice Boltzmann method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barrios, G.; Rechtman, R.</p> <p></p> <p>When the <span class="hlt">acoustic</span> force inside a cavity balances the gravitational force on a particle the result is known as <span class="hlt">acoustic</span> levitation. Using the lattice Boltzmann equation method we find the <span class="hlt">acoustic</span> force acting on a rounded particle for two different single-axis <span class="hlt">acoustic</span> levitators in two dimensions, the first with plane waves, the second with a rounded reflector that enhances the <span class="hlt">acoustic</span> force. With no gravitational force, a particle oscillates around a <span class="hlt">pressure</span> node; in the presence of gravity the oscillation is shifted a small vertical distance below the <span class="hlt">pressure</span> node. This distance increases linearly as the density ratio between the solid particle and fluid grows. For both cavities, the particle oscillates with the frequency of the sound source and its harmonics and in some cases there is a much smaller second dominant frequency. When the momentum of the <span class="hlt">acoustic</span> source changes, the oscillation around the average vertical position can have both frequencies mentioned above. However, if this quantity is large enough, the oscillations of the particle are aperiodic in the cavity with a rounded reflector.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1982asa..meet...26M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1982asa..meet...26M"><span><span class="hlt">Pressure</span> transfer function of a JT15D nozzle due to <span class="hlt">acoustic</span> and convected entropy fluctuations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Miles, J. H.</p> <p></p> <p>An <span class="hlt">acoustic</span> transmission matrix analysis of sound propagation in a variable area duct with and without flow is extended to include convected entropy fluctuations. The boundary conditions used in the analysis are a transfer function relating entropy and <span class="hlt">pressure</span> at the nozzle inlet and the nozzle exit impedance. The nozzle <span class="hlt">pressure</span> transfer function calculated is compared with JT15D turbofan engine nozzle data. The one dimensional theory for sound propagation in a variable area nozzle with flow but without convected entropy is good at the low engine speeds where the nozzle exit Mach number is low (M=0.2) and the duct exit impedance model is good. The effect of convected entropy appears to be so negligible that it is obscured by the inaccuracy of the nozzle exit impedance model, the lack of information on the magnitude of the convected entropy and its phase relationship with the <span class="hlt">pressure</span>, and the scatter in the data. An improved duct exit impedance model is required at the higher engine speeds where the nozzle exit Mach number is high (M=0.56) and at low frequencies (below 120 Hz).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930009581','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930009581"><span>Coupling between plate vibration and <span class="hlt">acoustic</span> radiation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Frendi, Abdelkader; Maestrello, Lucio; Bayliss, Alvin</p> <p>1992-01-01</p> <p>A detailed numerical investigation of the coupling between the vibration of a flexible plate and the <span class="hlt">acoustic</span> radiation is performed. The nonlinear Euler equations are used to describe the <span class="hlt">acoustic</span> fluid while the nonlinear plate equation is used to describe the plate vibration. Linear, nonlinear, and quasi-periodic or chaotic vibrations and the resultant <span class="hlt">acoustic</span> radiation are analyzed. We find that for the linear plate response, <span class="hlt">acoustic</span> coupling is negligible. However, for the nonlinear and chaotic responses, <span class="hlt">acoustic</span> coupling has a significant effect on the vibration level as the loading increases. The radiated <span class="hlt">pressure</span> from a plate undergoing nonlinear or chaotic vibrations is found to propagate nonlinearly into the far-field. However, the nonlinearity due to wave propagation is much weaker than that due to the plate vibrations. As the <span class="hlt">acoustic</span> wave propagates into the far-field, the relative difference in level between the fundamental and its harmonics and subharmonics decreases with distance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1010513','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1010513"><span><span class="hlt">Acoustic</span> Seaglider: PhilSea10 Data Analysis</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2016-06-13</p> <p>and (simple) Kalman filtering techniques will be explored to utilize the unique time-space sound speed sampling of the Seagliders to generate snapshots... temperature and salinity were deployed (Figure 1). General objectives of the experiment are to understand the <span class="hlt">acoustic</span> propagation in the...an <span class="hlt">acoustic</span> recording system (ARS) to record the moored source transmissions, as well as temperature , salinity and <span class="hlt">pressure</span> sensors (from which</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NPGeo..25...89L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NPGeo..25...89L"><span>Tipping point analysis of ocean <span class="hlt">acoustic</span> noise</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Livina, Valerie N.; Brouwer, Albert; Harris, Peter; Wang, Lian; Sotirakopoulos, Kostas; Robinson, Stephen</p> <p>2018-02-01</p> <p>We apply tipping point analysis to a large record of ocean <span class="hlt">acoustic</span> data to identify the main components of the <span class="hlt">acoustic</span> dynamical system and study possible bifurcations and transitions of the system. The analysis is based on a statistical physics framework with stochastic modelling, where we represent the observed data as a composition of deterministic and stochastic components estimated from the data using time-series techniques. We analyse long-term and seasonal trends, system states and <span class="hlt">acoustic</span> fluctuations to reconstruct a one-dimensional stochastic equation to approximate the <span class="hlt">acoustic</span> dynamical system. We apply potential analysis to <span class="hlt">acoustic</span> fluctuations and detect several changes in the system states in the past 14 years. These are most likely caused by climatic phenomena. We analyse trends in sound <span class="hlt">pressure</span> level within different frequency bands and hypothesize a possible anthropogenic impact on the <span class="hlt">acoustic</span> environment. The tipping point analysis framework provides insight into the structure of the <span class="hlt">acoustic</span> data and helps identify its dynamic phenomena, correctly reproducing the probability distribution and scaling properties (power-law correlations) of the time series.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910012056','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910012056"><span>A new, simple electrostatic-<span class="hlt">acoustic</span> hybrid levitator</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lierke, E. G.; Loeb, H.; Gross, D.</p> <p>1990-01-01</p> <p>Battelle has developed a hybrid levitator by combining the known single-axis <span class="hlt">acoustic</span> standing wave levitator with a coaxial DC electric field. The resulting Coulomb forces on the charged liquid or solid sample support its weight and, together with the <span class="hlt">acoustic</span> force, center the sample. Liquid samples with volumes approximately less than 100 micro-liters are deployed from a syringe reservoir into the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> node. The sample is charged using a miniature high voltage power supply (approximately less than 20 kV) connected to the syringe needle. As the electric field, generated by a second miniature power supply, is increased, the <span class="hlt">acoustic</span> intensity is reduced. The combination of both fields allows stable levitation of samples larger than either single technique could position on the ground. Decreasing the <span class="hlt">acoustic</span> intensity reduces <span class="hlt">acoustic</span> convection and sample deformation. Neither the electrostatic nor the <span class="hlt">acoustic</span> field requires sample position sensing or active control. The levitator, now used for static and dynamic fluid physics investigations on the ground, can be easily modified for space operations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/867078','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/867078"><span>Heat-driven <span class="hlt">acoustic</span> cooling engine having no moving parts</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Wheatley, John C.; Swift, Gregory W.; Migliori, Albert; Hofler, Thomas J.</p> <p>1989-01-01</p> <p>A heat-driven <span class="hlt">acoustic</span> cooling engine having no moving parts receives heat from a heat source. The <span class="hlt">acoustic</span> cooling engine comprises an elongated resonant <span class="hlt">pressure</span> vessel having first and second ends. A compressible fluid having a substantial thermal expansion coefficient and capable of supporting an <span class="hlt">acoustic</span> standing wave is contained in the resonant <span class="hlt">pressure</span> vessel. The heat source supplies heat to the first end of the vessel. A first heat exchanger in the vessel is spaced-apart from the first end and receives heat from the first end. A first thermodynamic element is adjacent to the first heat exchanger and converts some of the heat transmitted by the first heat exchanger into <span class="hlt">acoustic</span> power. A second thermodynamic element has a first end located spaced-apart from the first thermodynamic element and a second end farther away from the first thermodynamic element than is its first end. The first end of the second thermodynamic element heats while its second end cools as a consequence of the <span class="hlt">acoustic</span> power. A second heat exchanger is adjacent to and between the first and second thermodynamic elements. A heat sink outside of the vessel is thermally coupled to and receives heat from the second heat exchanger. The resonant <span class="hlt">pressure</span> vessel can include a housing less than one-fourth wavelength in length coupled to a reservoir. The housing can include a reduced diameter portion communicating with the reservoir.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5796287','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5796287"><span>Novel Fiber-Optic Ring <span class="hlt">Acoustic</span> Emission Sensor</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Han, Xiaole; Xia, Dong; Liu, Taolin; Lang, Hao</p> <p>2018-01-01</p> <p><span class="hlt">Acoustic</span> emission technology has been applied to many fields for many years. However, the conventional piezoelectric <span class="hlt">acoustic</span> emission sensors cannot be used in extreme environments, such as those with heavy electromagnetic interference, high <span class="hlt">pressure</span>, or strong corrosion. In this paper, a novel fiber-optic ring <span class="hlt">acoustic</span> emission sensor is proposed. The sensor exhibits high sensitivity, anti-electromagnetic interference, and corrosion resistance. First, the principle of a novel fiber-optic ring sensor is introduced. Different from piezoelectric and other fiber <span class="hlt">acoustic</span> emission sensors, this novel sensor includes both a sensing skeleton and a sensing fiber. Second, a heterodyne interferometric demodulating method is presented. In addition, a fiber-optic ring sensor <span class="hlt">acoustic</span> emission system is built based on this method. Finally, fiber-optic ring <span class="hlt">acoustic</span> emission experiments are performed. The novel fiber-optic ring sensor is glued onto the surface of an aluminum plate. The 150 kHz standard continuous sinusoidal signals and broken lead signals are successfully detected by the novel fiber-optic ring <span class="hlt">acoustic</span> emission sensor. In addition, comparison to the piezoelectric <span class="hlt">acoustic</span> emission sensor is performed, which shows the availability and reliability of the novel fiber-optic ring <span class="hlt">acoustic</span> emission sensor. In the future, this novel fiber-optic ring <span class="hlt">acoustic</span> emission sensor will provide a new route to <span class="hlt">acoustic</span> emission detection in harsh environments. PMID:29342858</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29878010','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29878010"><span>Retrieving <span class="hlt">acoustic</span> energy densities and local <span class="hlt">pressure</span> amplitudes in microfluidics by holographic time-lapse imaging.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cacace, Teresa; Bianco, Vittorio; Paturzo, Melania; Memmolo, Pasquale; Vassalli, Massimo; Fraldi, Massimiliano; Mensitieri, Giuseppe; Ferraro, Pietro</p> <p>2018-06-26</p> <p>The development of techniques able to characterize and map the <span class="hlt">pressure</span> field is crucial for the widespread use of acoustofluidic devices in biotechnology and lab-on-a-chip platforms. In fact, acoustofluidic devices are powerful tools for driving precise manipulation of microparticles and cells in microfluidics in non-contact modality. Here, we report a full and accurate characterization of the movement of particles subjected to acoustophoresis in a microfluidic environment by holographic imaging. The particle displacement along the direction of the ultrasound wave propagation, coinciding with the optical axis, is observed and investigated. Two resonance frequencies are explored, varying for each the amplitude of the applied signal. The trajectories of individual tracers, accomplished by holographic measurements, are fitted with the theoretical model thus allowing the retrieval of the <span class="hlt">acoustic</span> energy densities and <span class="hlt">pressure</span> amplitudes through full holographic analysis. The absence of prior calibration, being independent of the object shape and the possibility of implementing automatic analysis make the use of holography very appealing for applications in devices for biotechnologies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19860043184&hterms=Acoustic+levitation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DAcoustic%2Blevitation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19860043184&hterms=Acoustic+levitation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DAcoustic%2Blevitation"><span>Dual-temperature <span class="hlt">acoustic</span> levitation and sample transport apparatus</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Trinh, E.; Robey, J.; Jacobi, N.; Wang, T.</p> <p>1986-01-01</p> <p>The properties of a dual-temperature resonant chamber to be used for <span class="hlt">acoustical</span> levitation and positioning have been theoretically and experimentally studied. The predictions of a first-order dissipationless treatment of the generalized wave equation for an inhomogeneous medium are in close agreement with experimental results for the temperature dependence of the resonant mode spectrum and the <span class="hlt">acoustic</span> <span class="hlt">pressure</span> distribution, although the measured magnitude of the <span class="hlt">pressure</span> variations does not correlate well with the calculated one. Ground-based levitation of low-density samples has been demonstrated at 800 C, where steady-state forces up to 700 dyn were generated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880062181&hterms=excessive+force&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dexcessive%2Bforce','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880062181&hterms=excessive+force&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dexcessive%2Bforce"><span><span class="hlt">Acoustic</span> radiation force on a heated sphere including effects of heat transfer and <span class="hlt">acoustic</span> streaming</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lee, Chun P.; Wang, Taylor G.</p> <p>1988-01-01</p> <p>A previous theoretical result on the subject of the <span class="hlt">acoustic</span> radiation force on a heated sphere (Lee and Wang, 1984) is reexamined. For a more complete understanding, effects of heat transfer and <span class="hlt">acoustic</span> streaming are taken into consideration. Essentially, it was found that, at high sound-<span class="hlt">pressure</span> levels in a steady situation, the force is not affected significantly by the temperature profile, consistent with the result of an experimental work (Leung and Wang, 1985). This resolves the earlier apparent contradiction between the theory and the experiment. If excessive hot air is accumulated around the sphere, which can happen in transient situations, the force can be weakened or reversed in sign. A heat transfer model due to <span class="hlt">acoustic</span> streaming was also found.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018RScI...89e5002Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018RScI...89e5002Y"><span>Helix structure for low frequency <span class="hlt">acoustic</span> energy harvesting</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yuan, Ming; Cao, Ziping; Luo, Jun; Pang, Zongqiang</p> <p>2018-05-01</p> <p>In this study, a novel helix <span class="hlt">acoustic</span> resonator is proposed to realize <span class="hlt">acoustic</span> energy harvesting (AEH). Compared with the traditional <span class="hlt">acoustic</span> resonators, the proposed structure occupies a small volume and is suitable for the low frequency range. At a specific incident frequency, the mechanical component of the AEH device can be intensely excited and the bonded piezoelectric patch is utilized to convert the strain energy into electrical energy. Analytical studies are carried out to disclose the <span class="hlt">acoustic</span> resonant system properties. Meanwhile, the pure <span class="hlt">acoustic</span> and coupled vibro-<span class="hlt">acoustic</span> properties of the proposed device are analyzed via the finite element method. The major part of the AEH device is fabricated via 3D printing for experimental study, which is favored for rapid prototyping. At <span class="hlt">acoustic</span> resonance frequency 175 Hz, 100 dB sound <span class="hlt">pressure</span> level excitation working condition, the measured experimental data show that the harvested power can be up to 7.3 μW.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29864807','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29864807"><span>Helix structure for low frequency <span class="hlt">acoustic</span> energy harvesting.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yuan, Ming; Cao, Ziping; Luo, Jun; Pang, Zongqiang</p> <p>2018-05-01</p> <p>In this study, a novel helix <span class="hlt">acoustic</span> resonator is proposed to realize <span class="hlt">acoustic</span> energy harvesting (AEH). Compared with the traditional <span class="hlt">acoustic</span> resonators, the proposed structure occupies a small volume and is suitable for the low frequency range. At a specific incident frequency, the mechanical component of the AEH device can be intensely excited and the bonded piezoelectric patch is utilized to convert the strain energy into electrical energy. Analytical studies are carried out to disclose the <span class="hlt">acoustic</span> resonant system properties. Meanwhile, the pure <span class="hlt">acoustic</span> and coupled vibro-<span class="hlt">acoustic</span> properties of the proposed device are analyzed via the finite element method. The major part of the AEH device is fabricated via 3D printing for experimental study, which is favored for rapid prototyping. At <span class="hlt">acoustic</span> resonance frequency 175 Hz, 100 dB sound <span class="hlt">pressure</span> level excitation working condition, the measured experimental data show that the harvested power can be up to 7.3 μW.</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>