Sample records for portable pressure wave-maker

  1. Portable Dynamic Pressure Calibrator

    NASA Technical Reports Server (NTRS)

    Wright, Morgan S.; Maynard, Everett (Technical Monitor)

    1996-01-01

    A portable, dynamic pressure calibrator was fabricated for use on wind tunnel models at NASA-Ames Research Center. The calibrator generates sine wave pressures at levels up to 1 PSIG P-P(168dB) at frequencies from 10Hz to 6KHz and .5 PSIG P.P (162dB) at frequencies from 6KHz to 20KHz. The calibrator consists of two units connected by a single cable. The handheld unit contains a pressure transducer, speaker, and deadman switch. This unit allows application of dynamic pressure to transducers/ports on installed wind tunnel models. The base unit contains all of power supplies, controls and displays. This unit allows amplitude and frequency to be set and verified at a safe location off of the model.

  2. Study on ambient noise generated from breaking waves simulated by a wave maker in a tank

    NASA Astrophysics Data System (ADS)

    Wei, Ruey-Chang; Chan, Hsiang-Chih

    2002-11-01

    This paper studies ambient noise in the surf zone that was simulated by a piston-type wave maker in a tank. The experiment analyzed the bubbles of a breaking wave by using a hydrophone to receive the acoustic signal, and the images of bubbles were recorded by a digital video camera to observe the distribution of the bubbles. The slope of the simulated seabed is 1:5, and the dimensions of the water tank are 35 m x1 m x1.2 m. The studied parameters of ambient noise generated by breaking wave bubbles were wave height, period, and water depth. Short-time Fourier transform was applied to obtain the acoustic spectrum of bubbles, MATLAB programs were used to calculate mean sound pressure level, and determine the number of bubbles. Bubbles with resonant frequency from 0.5 to 10 kHz were studied, counted from peaks in the spectrum. The number of bubbles generated by breaking waves could be estimated by the bubbles energy distributions. The sound pressure level of ambient noise was highly related to the wave height and period, with correlation coefficient 0.7.

  3. 29 CFR 1915.172 - Portable air receivers and other unfired pressure vessels.

    Code of Federal Regulations, 2012 CFR

    2012-07-01

    ... 29 Labor 7 2012-07-01 2012-07-01 false Portable air receivers and other unfired pressure vessels... SHIPYARD EMPLOYMENT Portable, Unfired Pressure Vessels, Drums and Containers, Other Than Ship's Equipment § 1915.172 Portable air receivers and other unfired pressure vessels. (a) Portable, unfired pressure...

  4. 29 CFR 1915.172 - Portable air receivers and other unfired pressure vessels.

    Code of Federal Regulations, 2013 CFR

    2013-07-01

    ... 29 Labor 7 2013-07-01 2013-07-01 false Portable air receivers and other unfired pressure vessels... SHIPYARD EMPLOYMENT Portable, Unfired Pressure Vessels, Drums and Containers, Other Than Ship's Equipment § 1915.172 Portable air receivers and other unfired pressure vessels. (a) Portable, unfired pressure...

  5. 29 CFR 1915.172 - Portable air receivers and other unfired pressure vessels.

    Code of Federal Regulations, 2014 CFR

    2014-07-01

    ... 29 Labor 7 2014-07-01 2014-07-01 false Portable air receivers and other unfired pressure vessels... SHIPYARD EMPLOYMENT Portable, Unfired Pressure Vessels, Drums and Containers, Other Than Ship's Equipment § 1915.172 Portable air receivers and other unfired pressure vessels. (a) Portable, unfired pressure...

  6. Portable fixture facilitates pressure testing of instrumentation fittings

    NASA Technical Reports Server (NTRS)

    Olson, G. A.

    1967-01-01

    Portable fixture facilitates pressure testing to detect possible leaks in instrumentation fittings mounted on tank bulkheads. It uses a vacuum cup which seals a pressure regulator adapter around one side of the fitting to be pressure tested. Leakage is detected with a gas sniffer.

  7. High-pressure portable pneumatic drive unit.

    PubMed

    Hete, B F; Savage, M; Batur, C; Smith, W A; Golding, L A; Nosé, Y

    1989-12-01

    The left ventricular assist device (LVAD) of the Cleveland Clinic Foundation (CCF) is a single-chamber assist pump, driven by a high-pressure pneumatic cylinder. A low-cost, portable driver that will allow cardiac care patients, with a high-pressure pneumatic ventricle assist, more freedom of movement has been developed. The compact and light-weight configuration can provide periods of 2 h of freedom from a fixed position driver and does not use exotic technology.

  8. 29 CFR 1915.172 - Portable air receivers and other unfired pressure vessels.

    Code of Federal Regulations, 2011 CFR

    2011-07-01

    ... 29 Labor 7 2011-07-01 2011-07-01 false Portable air receivers and other unfired pressure vessels. 1915.172 Section 1915.172 Labor Regulations Relating to Labor (Continued) OCCUPATIONAL SAFETY AND HEALTH ADMINISTRATION, DEPARTMENT OF LABOR (CONTINUED) OCCUPATIONAL SAFETY AND HEALTH STANDARDS FOR SHIPYARD EMPLOYMENT Portable, Unfired Pressure...

  9. Portable Ultrasonic Guided Wave Inspection with MACRO Fiber Composite Actuators

    NASA Astrophysics Data System (ADS)

    Haig, A.; Mudge, P.; Catton, P.; Balachandran, W.

    2010-02-01

    The development of portable ultrasonic guided wave transducer arrays that utilize Macro Fiber Composite actuators (MFCs) is described. Portable inspection equipment can make use of ultrasonic guided waves to rapidly screen large areas of many types of engineering structures for defects. The defect finding performance combined with the difficulty of application determines how much the engineering industry makes use of this non-destructive, non-disruptive technology. The developments with MFCs have the potential to make considerable improvements in both these aspects. MFCs are highly efficient because they use interdigital electrodes to facilitate the extensional, d33 displacement mode. Their fiber composite design allows them to be thin, lightweight, flexible and durable. The flexibility affords them conformance with curved surfaces, which can facilitate good mechanical coupling. The suitability of a given transducer for Long Range Ultrasonic Testing is governed by the nature and amplitude of the displacement that it excites/senses in the contact area of the target structure. This nature is explored for MFCs through directional sensitivity analysis and empirical testing. Housing methods that facilitate non-permanent coupling techniques are discussed. Finally, arrangements of arrays of MFCs for the guided wave inspection of plates and pipes are considered and some broad design criteria are given.

  10. New Global Art Connection: Paying Tribute to the Wave-Makers (1910-2010)

    ERIC Educational Resources Information Center

    Kan, Koon Hwee

    2013-01-01

    This paper highlights "Wave-Makers (1910--2010)", a collaborative timeline redesign project, which involves interactive and advanced web-based technology to connect and complement arts curricula at two higher education institutions, one located in China and another in the United States. Through in-depth research, video-conferencing,…

  11. Solid Sampling with a Diode Laser for Portable Ambient Mass Spectrometry.

    PubMed

    Yung, Yeni P; Wickramasinghe, Raveendra; Vaikkinen, Anu; Kauppila, Tiina J; Veryovkin, Igor V; Hanley, Luke

    2017-07-18

    A hand-held diode laser is implemented for solid sampling in portable ambient mass spectrometry (MS). Specifically, a pseudocontinuous wave battery-powered surgical laser diode is employed for portable laser diode thermal desorption (LDTD) at 940 nm and compared with nanosecond pulsed laser ablation at 2940 nm. Postionization is achieved in both cases using atmospheric pressure photoionization (APPI). The laser ablation atmospheric pressure photoionization (LAAPPI) and LDTD-APPI mass spectra of sage leaves (Salvia officinalis) using a field-deployable quadrupole ion trap MS display many similar ion peaks, as do the mass spectra of membrane grown biofilms of Pseudomonas aeruginosa. These results indicate that LDTD-APPI method should be useful for in-field sampling of plant and microbial communities, for example, by portable ambient MS. The feasibility of many portable MS applications is facilitated by the availability of relatively low cost, portable, battery-powered diode lasers. LDTD could also be coupled with plasma- or electrospray-based ionization for the analysis of a variety of solid samples.

  12. 29 CFR 1915.172 - Portable air receivers and other unfired pressure vessels.

    Code of Federal Regulations, 2010 CFR

    2010-07-01

    ..., 1963. They shall be subjected to a hydrostatic pressure test of one and one-half times the working... quarterly by a competent person. They shall be subjected yearly to a hydrostatic pressure test of one and... 29 Labor 7 2010-07-01 2010-07-01 false Portable air receivers and other unfired pressure vessels...

  13. A portable pressure pump for microfluidic lab-on-a-chip systems using a porous polydimethylsiloxane (PDMS) sponge.

    PubMed

    Cha, Kyoung Je; Kim, Dong Sung

    2011-10-01

    In this paper, we propose a novel portable and disposable pressure pump using a porous polydimethylsiloxane (PDMS) sponge and demonstrate its application to a microfluidic lab-on-a-chip. The porous PDMS sponge was simply fabricated by a sugar leaching technique based on capillary suction of pre-cured PDMS into lumps of sugar, thereby enabling us to achieve the porous PDMS sponge composed of interconnected micropores. To indicate the characteristics of the porous PDMS sponge and pump, we measured the average porosities of them whose values were 0.64 and 0.34, respectively. A stress-strain relationship of the fabricated portable pressure pump represented a linear behavior in the compressive strain range of 0 to 20%. Within this range, a pumping volume of the pressure pump could be linearly controlled by the compressed strain. Finally, the fabricated porous PDMS pump was successfully demonstrated as a portable pressure pump for a disposable microfluidic lab-on-a-chip for efficient detection of agglutination. The proposed portable pressure pump can be potentially applicable to various disposable microfluidic lab-on-a-chip systems.

  14. Portable digital pressure indicator for calibrating magnetic tape recorders

    NASA Technical Reports Server (NTRS)

    Mccormick, Royce F.; Leighty, Bradley D.

    1989-01-01

    The design of a portable Digital Pressure Indicator (DPI) to be used for calibrating the pressure systems on Langley's magnetic tape recorders is described. High-speed magnetic tape recorders require pressure (0 to 20 psig) for providing an air cushion across the tape guides and a slight vacuum (30 inch H2O) for maintaining the proper number of tape loops in the advance and feed chamber. The DPI is a hand-held device that can be quickly coupled to a magnetic tape recorder and includes a two-position switch for selecting either measured pressure or vacuum, to be displayed digitally in engineering units (psig or inches H2O). The DPI is currently in use in Langley's Analysis and Computation Division.

  15. Solid Sampling with a Diode Laser for Portable Ambient Mass Spectrometry

    PubMed Central

    2017-01-01

    A hand-held diode laser is implemented for solid sampling in portable ambient mass spectrometry (MS). Specifically, a pseudocontinuous wave battery-powered surgical laser diode is employed for portable laser diode thermal desorption (LDTD) at 940 nm and compared with nanosecond pulsed laser ablation at 2940 nm. Postionization is achieved in both cases using atmospheric pressure photoionization (APPI). The laser ablation atmospheric pressure photoionization (LAAPPI) and LDTD-APPI mass spectra of sage leaves (Salvia officinalis) using a field-deployable quadrupole ion trap MS display many similar ion peaks, as do the mass spectra of membrane grown biofilms of Pseudomonas aeruginosa. These results indicate that LDTD-APPI method should be useful for in-field sampling of plant and microbial communities, for example, by portable ambient MS. The feasibility of many portable MS applications is facilitated by the availability of relatively low cost, portable, battery-powered diode lasers. LDTD could also be coupled with plasma- or electrospray-based ionization for the analysis of a variety of solid samples. PMID:28632988

  16. Portable power supply options for positive airway pressure devices.

    PubMed

    Riaz, Muhammad; Certal, Victor; Camacho, Macario

    2015-01-01

    Patients with obstructive sleep apnea (OSA) often face the challenge of how to power their positive airway pressure (PAP) devices when alternating current power supplies are not available in remote areas with lack of electricity or frequent power outages. This article elucidates portable power supply options for PAP devices with the aim to increase alternative power source awareness among medical providers. A search of scientific databases (Medline, Scopus, Web of Science, Google Scholar, and the Cochrane Library) was carried out on the topic of alternative portable power supply options for treatment of OSA. Scientific databases listed above yielded only limited results. Most articles were found via Google search. These articles were reviewed for alternative power supply options for OSA patients when alternating current is not available. The power supply options in this article include lead-acid batteries (starter, marine and deep-cycle batteries), lithium ion batteries, solar kits, battery packs, backup power systems, portable generators, and travel-size PAP devices. There are several options to power PAP devices with direct current when alternating current is not available. Knowledgeable primary care physicians especially in rural and remote areas can help OSA patients improve PAP compliance in order to mitigate morbidity and long-term complications of OSA.

  17. EVOLUTION of the Pressure Wave Supercharger Concept

    NASA Astrophysics Data System (ADS)

    Costiuc, Iuliana; Chiru, Anghel

    2017-10-01

    Born more than a century ago, the concept of exploiting the pressure wave phenomenon has evolved with rather small steps, experiencing an accelerated progress over the past decades. This paper aims an overview on the researchers’ results over time regarding the pressure wave technology and its applications, pointing out on the internal combustion engine’s supercharging application. This review complements the past reports on the subject, presenting the evolution of the concept and technology, as well as the researcher’s efforts on solving the specific shortcomings of this pressure wave technology. Undoubtedly, the pressure wave rotors have been a research goal over the years. At first, most of the researches were experimental and the theoretical calculations required to improve the technology were too arduous. Recently, new computer software dedicated to accurate simulation of the processes governing the wave rotor operation, altogether with modern experimental measurement instruments and well-developed diagnostic techniques have opened wide possibilities to innovate the pressure wave supercharging technology. This paper also highlights the challenges that specialists still have to overcome and aspects to become future preoccupations and research directions.

  18. Miniaturised electrically actuated high pressure injection valve for portable capillary liquid chromatography.

    PubMed

    Li, Yan; Pace, Kirsten; Nesterenko, Pavel N; Paull, Brett; Stanley, Roger; Macka, Mirek

    2018-04-01

    A miniaturised high pressure 6-port injection valve has been designed and evaluated for its performance in order to facilitate the development of portable capillary high performance liquid chromatography (HPLC). The electrically actuated valve features a very small size (65 × 19 × 19mm) and light weight (33g), and therefore can be easily integrated in a miniaturised modular capillary LC system suited for portable field analysis. The internal volume of the injection valve was determined as 98 nL. The novel conical shape of the stator and rotor and the spring-loaded rotor performed well up to 32MPa (4641psi), the maximum operating pressure investigated. Suitability for application was demonstrated using a miniaturised capillary LC system applied to the chromatographic separation of a mixture of biogenic amines and common cations. The RSD (relative standard deviation) values of retention times and peak areas of 6 successive runs were 0.5-0.7% and 1.8-2.8% for the separation of biogenic amines, respectively, and 0.1-0.2% and 2.1-3.0% for the separation of cations, respectively. This performance was comparable with bench-top HPLC systems thus demonstrating the applicability of the valve for use in portable and miniaturised capillary HPLC systems. Copyright © 2017 Elsevier B.V. All rights reserved.

  19. The Portable War Room Research Project

    NASA Technical Reports Server (NTRS)

    Govers, Francis X., III; Fry, Mark

    1997-01-01

    The Portable War Room is an internal TASC project to research and develop a visualization and simulation environment to provide for decision makers the power to review the past, understand the present, and peer into the future.

  20. Modeling of wave-coherent pressures in the turbulent boundary layer above water waves

    NASA Technical Reports Server (NTRS)

    Papadimitrakis, Yiannis ALEX.

    1988-01-01

    The behavior of air pressure fluctuations induced by progressive water waves generated mechanically in a laboratory tank was simulated by solving a modified Orr-Sommerfeld equation in a transformed Eulerian wave-following frame of reference. Solution is obtained by modeling the mean and wave-coherent turbulent Reynolds stresses, the behavior of which in the turbulent boundary layer above the waves was simulated using a turbulent kinetic energy-dissipation model, properly modified to account for free-surface proximity and favorable pressure gradient effects. The distribution of both the wave-coherent turbulent Reynolds stress and pressure amplitudes and their corresponding phase lags was found to agree reasonably well with available laboratory data.

  1. Plateau Waves of Intracranial Pressure and Partial Pressure of Cerebral Oxygen.

    PubMed

    Lang, Erhard W; Kasprowicz, Magdalena; Smielewski, Peter; Pickard, John; Czosnyka, Marek

    2016-01-01

    This study investigates 55 intracranial pressure (ICP) plateau waves recorded in 20 patients after severe traumatic brain injury (TBI) with a focus on a moving correlation coefficient between mean arterial pressure (ABP) and ICP, called PRx, which serves as a marker of cerebrovascular reactivity, and a moving correlation coefficient between ABP and cerebral partial pressure of oxygen (pbtO2), called ORx, which serves as a marker for cerebral oxygen reactivity. ICP and ICPamplitude increased significantly during the plateau waves, whereas CPP and pbtO2 decreased significantly. ABP, ABP amplitude, and heart rate remained unchanged. In 73 % of plateau waves PRx increased during the wave. ORx showed an increase during and a decrease after the plateau waves, which was not statistically significant. Our data show profound cerebral vasoparalysis on top of the wave and, to a lesser extent, impairment of cerebral oxygen reactivity. The different behavior of the indices may be due to the different latencies of the cerebral blood flow and oxygen level control mechanisms. While cerebrovascular reactivity is a rapidly reacting mechanism, cerebral oxygen reactivity is slower.

  2. Pressures, flow, and brain oxygenation during plateau waves of intracranial pressure.

    PubMed

    Dias, Celeste; Maia, Isabel; Cerejo, António; Varsos, Georgios; Smielewski, Peter; Paiva, José-Artur; Czosnyka, Marek

    2014-08-01

    Plateau waves are common in traumatic brain injury. They constitute abrupt increases of intracranial pressure (ICP) above 40 mmHg associated with a decrease in cerebral perfusion pressure (CPP). The aim of this study was to describe plateau waves characteristics with multimodal brain monitoring in head injured patients admitted in neurocritical care. Prospective observational study in 18 multiple trauma patients with head injury admitted to Neurocritical Care Unit of Hospital Sao Joao in Porto. Multimodal systemic and brain monitoring of primary variables [heart rate, arterial blood pressure, ICP, CPP, pulse amplitude, end tidal CO₂, brain temperature, brain tissue oxygenation pressure, cerebral oximetry (CO) with transcutaneous near-infrared spectroscopy and cerebral blood flow (CBF)] and secondary variables related to cerebral compensatory reserve and cerebrovascular reactivity were supported by dedicated software ICM+ ( www.neurosurg.cam.ac.uk/icmplus) . The compiled data were analyzed in patients who developed plateau waves. In this study we identified 59 plateau waves that occurred in 44% of the patients (8/18). During plateau waves CBF, cerebrovascular resistance, CO, and brain tissue oxygenation decreased. The duration and magnitude of plateau waves were greater in patients with working cerebrovascular reactivity. After the end of plateau wave, a hyperemic response was recorded in 64% of cases with increase in CBF and brain oxygenation. The magnitude of hyperemia was associated with better autoregulation status and low oxygenation levels at baseline. Multimodal brain monitoring facilitates identification and understanding of intrinsic vascular brain phenomenon, such as plateau waves, and may help the adequate management of acute head injury at bed side.

  3. Comparison of three portable instruments to measure compression pressure.

    PubMed

    Partsch, H; Mosti, G

    2010-10-01

    Measurement of interface pressure between the skin and a compression device has gained practical importance not only for characterizing the efficacy of different compression products in physiological and clinical studies but also for the training of medical staff. A newly developed portable pneumatic pressure transducer (Picopress®) was compared with two established systems (Kikuhime® and SIGaT tester®) measuring linearity, variability and accuracy on a cylindrical model using a stepwise inflated sphygmomanometer as the reference. In addition the variation coefficients were measured by applying the transducers repeatedly under a blood pressure cuff on the distal lower leg of a healthy human subject with stepwise inflation. In the pressure range between 10 and 80 mmHg all three devices showed a linear association compared with the sphygmomanometer values (Pearson r>0.99). The best reproducibility (variation coefficients between 1.05-7.4%) and the highest degree of accuracy demonstrated by Bland-Altman plots was achieved with the Picopress® transducer. Repeated measurements of pressure in a human leg revealed average variation coefficients for the three devices of 4.17% (Kikuhime®), 8.52% (SIGaT®) and 2.79% (Picopress®). The results suggest that the Picopress® transducer, which also allows dynamic pressure tracing in connection with a software program and which may be left under a bandage for several days, is a reliable instrument for measuring the pressure under a compression device.

  4. Orthogonal P-wave morphology is affected by intra-atrial pressures.

    PubMed

    Petersson, Richard; Smith, J Gustav; Larsson, David A; Reitan, Öyvind; Carlson, Jonas; Platonov, Pyotr; Holmqvist, Fredrik

    2017-12-06

    It has previously been shown that the morphology of the P-wave neither depends on atrial size in healthy subjects with physiologically enlarged atria nor on the physiological anatomical variation in transverse orientation of the left atrium. The present study aimed to investigate if different pressures in the left and right atrium are associated with different P-wave morphologies. 38 patients with isolated, increased left atrial pressure, 51 patients with isolated, increased right atrial pressure and 76 patients with biatrially increased pressure were studied. All had undergone right heart catheterization and had 12-lead electrocardiographic recordings, which were transformed into vectorcardiograms for detailed P-wave morphology analysis. Normal P-wave morphology (type 1) was more common in patients with isolated increased pressure in the right atrium while abnormal P-wave morphology (type 2) was more common in the groups with increased left atrial pressure (P = 0.032). Moreover, patients with increased left atrial pressure, either isolated or in conjunction with increased right atrial pressure, had significantly more often a P-wave morphology with a positive deflection in the sagittal plane (P = 0.004). Isolated elevated right atrial pressure was associated with normal P-wave morphology while left-sided atrial pressure elevation, either isolated or in combination with right atrial pressure elevation, was associated with abnormal P-wave morphology.

  5. Design and implementation of a smartphone-based portable ultrasound pulsed-wave Doppler device for blood flow measurement.

    PubMed

    Huang, Chih-Chung; Lee, Po-Yang; Chen, Pay-Yu; Liu, Ting-Yu

    2012-01-01

    Blood flow measurement using Doppler ultrasound has become a useful tool for diagnosing cardiovascular diseases and as a physiological monitor. Recently, pocket-sized ultrasound scanners have been introduced for portable diagnosis. The present paper reports the implementation of a portable ultrasound pulsed-wave (PW) Doppler flowmeter using a smartphone. A 10-MHz ultrasonic surface transducer was designed for the dynamic monitoring of blood flow velocity. The directional baseband Doppler shift signals were obtained using a portable analog circuit system. After hardware processing, the Doppler signals were fed directly to a smartphone for Doppler spectrogram analysis and display in real time. To the best of our knowledge, this is the first report of the use of this system for medical ultrasound Doppler signal processing. A Couette flow phantom, consisting of two parallel disks with a 2-mm gap, was used to evaluate and calibrate the device. Doppler spectrograms of porcine blood flow were measured using this stand-alone portable device under the pulsatile condition. Subsequently, in vivo portable system verification was performed by measuring the arterial blood flow of a rat and comparing the results with the measurement from a commercial ultrasound duplex scanner. All of the results demonstrated the potential for using a smartphone as a novel embedded system for portable medical ultrasound applications. © 2012 IEEE

  6. Pressure waves in a supersaturated bubbly magma

    USGS Publications Warehouse

    Kurzon, I.; Lyakhovsky, V.; Navon, O.; Chouet, B.

    2011-01-01

    We study the interaction of acoustic pressure waves with an expanding bubbly magma. The expansion of magma is the result of bubble growth during or following magma decompression and leads to two competing processes that affect pressure waves. On the one hand, growth in vesicularity leads to increased damping and decreased wave amplitudes, and on the other hand, a decrease in the effective bulk modulus of the bubbly mixture reduces wave velocity, which in turn, reduces damping and may lead to wave amplification. The additional acoustic energy originates from the chemical energy released during bubble growth. We examine this phenomenon analytically to identify conditions under which amplification of pressure waves is possible. These conditions are further examined numerically to shed light on the frequency and phase dependencies in relation to the interaction of waves and growing bubbles. Amplification is possible at low frequencies and when the growth rate of bubbles reaches an optimum value for which the wave velocity decreases sufficiently to overcome the increased damping of the vesicular material. We examine two amplification phase-dependent effects: (1) a tensile-phase effect in which the inserted wave adds to the process of bubble growth, utilizing the energy associated with the gas overpressure in the bubble and therefore converting a large proportion of this energy into additional acoustic energy, and (2) a compressive-phase effect in which the pressure wave works against the growing bubbles and a large amount of its acoustic energy is dissipated during the first cycle, but later enough energy is gained to amplify the second cycle. These two effects provide additional new possible mechanisms for the amplification phase seen in Long-Period (LP) and Very-Long-Period (VLP) seismic signals originating in magma-filled cracks.

  7. Plateau Waves of Intracranial Pressure and Multimodal Brain Monitoring.

    PubMed

    Dias, Celeste; Maia, Isabel; Cerejo, Antonio; Smielewski, Peter; Paiva, José-Artur; Czosnyka, Marek

    2016-01-01

    The aim of this study was to describe multimodal brain monitoring characteristics during plateau waves of intracranial pressure (ICP) in patients with head injury, using ICM+ software for continuous recording. Plateau waves consist of an abrupt elevation of ICP above 40 mmHg for 5-20 min. This is a prospective observational study of patients with head injury who were admitted to a neurocritical care unit and who developed plateau waves. We analyzed 59 plateau waves that occurred in 8 of 18 patients (44 %). At the top of plateau waves arterial blood pressure remained almost constant, but cerebral perfusion pressure, cerebral blood flow, brain tissue oxygenation, and cerebral oximetry decreased. After plateau waves, patients with a previously better autoregulation status developed hyperemia, demonstrated by an increase in cerebral blood flow and brain oxygenation. Pressure and oxygen cerebrovascular reactivity indexes (pressure reactivity index and ORxshort) increased significantly during the plateau wave as a sign of disruption of autoregulation. Bedside multimodal brain monitoring is important to characterize increases in ICP and give differential diagnoses of plateau waves, as management of this phenomenon differs from that of regular ICP.

  8. Pressure reducing capacity of felt: a feasibility study using a new portable system with thin sensors.

    PubMed

    Deschamps, Kevin; Messier, Benjamin

    2015-03-01

    Pressure redistribution and off-loading is a vital component in the management of the foot in diabetes. In the present study, a new portable system encompassing thin piezoresistors was tested for clinical utility and efficacy with respect to a commonly used pressure relieving dressing for the foot in diabetes. Copyright © 2015 Elsevier Ireland Ltd. All rights reserved.

  9. 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.

  10. Corotating pressure waves without streams in the solar wind

    NASA Technical Reports Server (NTRS)

    Burlaga, L. F.

    1983-01-01

    Voyager 1 and 2 magnetic field and plasma data are presented which demonstrate the existence of large scale, corotating, non-linear pressure waves between 2 AU and 4 AU that are not accompanied by fast streams. The pressure waves are presumed to be generated by corotating streams near the Sun. For two of the three pressure waves that are discussed, the absence of a stream is probably a real, physical effect, viz., a consequence of deceleration of the stream by the associated compression wave. For the third pressure wave, the apparent absence of a stream may be a geometrical effect; it is likely that the stream was at latitudes just above those of the spacecraft, while the associated shocks and compression wave extended over a broader range of latitudes so that they could be observed by the spacecraft. It is suggested that the development of large-scale non-linear pressure waves at the expense of the kinetic energy of streams produces a qualitative change in the solar wind in the outer heliosphere. Within a few AU the quasi-stationary solar wind structure is determined by corotating streams whose structure is determined by the boundary conditions near the Sun.

  11. Pneumatic pressure wave generator provides economical, simple testing of pressure transducers

    NASA Technical Reports Server (NTRS)

    Gaal, A. E.; Weldon, T. P.

    1967-01-01

    Testing device utilizes the change in pressure about a bias or reference pressure level produced by displacement of a center-driven piston in a closed cylinder. Closely controlled pneumatic pressure waves allow testing under dynamic conditions.

  12. Wave Shape and Impact Pressure Measurements at a Rock Coast Cliff

    NASA Astrophysics Data System (ADS)

    Varley, S. J.; Rosser, N. J.; Brain, M.; Vann Jones, E. C.

    2016-02-01

    Rock coast research focuses largely on wave behaviour across beaches and shore platforms but rarely considers direct wave interaction with cliffs. Hydraulic action is one of the most important drivers of erosion along rock coasts. The magnitude of wave impact pressure has been shown by numerical and laboratory studies to be related to the wave shape. In deep water, a structure is only subjected to the hydrostatic pressure due to the oscillating clapotis. Dynamic pressures, related to the wave celerity, are exerted in shallower water when the wave is breaking at the point of impact; very high magnitude, short duration shock pressures are theorised to occur when the approaching wavefront is vertical. As such, wave shape may directly influence the potential of the impact to weaken rock and cause erosion. Measurements of impact pressure at coastal cliffs are limited, and the occurrence and influence of this phenomenon is currently poorly constrained. To address this, we have undertaken a field monitoring study on the magnitude and vertical distribution of wave impact pressures at the rocky, macro-tidal coastline of Staithes, North Yorkshire, UK. A series of piezo-resistive pressure transducers and a camera were installed at the base of the cliff during low tide. Transducers were deployed vertically up the cliff face and aligned shore-normal to capture the variation in static and dynamic pressure with height during a full spring tidal cycle. Five minute bursts of 5 kHz pressure readings and 4 Hz wave imaging were sampled every 30 minutes for six hours during high tide. Pressure measurements were then compensated for temperature and combined with wave imaging to produce a pressure time series and qualitative wave shape category for each wave impact. Results indicate the presence of a non-linear relationship between pressure impact magnitude, the occurrence of shock pressures, wave shape and tidal stage, and suggest that breaker type on impact (and controls thereof) may

  13. Second harmonic generation: Effects of the multiple reflections of the fundamental and the second harmonic waves on the Maker fringes

    NASA Astrophysics Data System (ADS)

    Tellier, Gildas; Boisrobert, Christian

    2007-11-01

    The Maker fringes technique is commonly used for the determination of nonlinear optical coefficients. In this article, we present a new formulation of Maker fringes in parallel-surface samples, using boundary conditions taking into account the anisotropy of the crystal, the refractive-index dispersion, and the reflections of the fundamental and the second harmonic waves inside the material. Complete expressions for the generated second harmonic intensity are given for birefringent crystals for the case of no pump depletion. A comparison between theory and experimental results is made, showing the accuracy of our theoretical expressions.

  14. Novel wave power analysis linking pressure-flow waves, wave potential, and the forward and backward components of hydraulic power.

    PubMed

    Mynard, Jonathan P; Smolich, Joseph J

    2016-04-15

    Wave intensity analysis provides detailed insights into factors influencing hemodynamics. However, wave intensity is not a conserved quantity, so it is sensitive to diameter variations and is not distributed among branches of a junction. Moreover, the fundamental relation between waves and hydraulic power is unclear. We, therefore, propose an alternative to wave intensity called "wave power," calculated via incremental changes in pressure and flow (dPdQ) and a novel time-domain separation of hydraulic pressure power and kinetic power into forward and backward wave-related components (ΠP±and ΠQ±). Wave power has several useful properties:1) it is obtained directly from flow measurements, without requiring further calculation of velocity;2) it is a quasi-conserved quantity that may be used to study the relative distribution of waves at junctions; and3) it has the units of power (Watts). We also uncover a simple relationship between wave power and changes in ΠP±and show that wave reflection reduces transmitted power. Absolute values of ΠP±represent wave potential, a recently introduced concept that unifies steady and pulsatile aspects of hemodynamics. We show that wave potential represents the hydraulic energy potential stored in a compliant pressurized vessel, with spatial gradients producing waves that transfer this energy. These techniques and principles are verified numerically and also experimentally with pressure/flow measurements in all branches of a central bifurcation in sheep, under a wide range of hemodynamic conditions. The proposed "wave power analysis," encompassing wave power, wave potential, and wave separation of hydraulic power provides a potent time-domain approach for analyzing hemodynamics. Copyright © 2016 the American Physiological Society.

  15. Fiber optic diffraction grating maker

    DOEpatents

    Deason, Vance A.; Ward, Michael B.

    1991-01-01

    A compact and portable diffraction grating maker comprised of a laser beam, optical and fiber optics devices coupling the beam to one or more evanescent beam splitters, and collimating lenses or mirrors directing the split beam at an appropriate photosensitive material. The collimating optics, the output ends of the fiber optic coupler and the photosensitive plate holder are all mounted on an articulated framework so that the angle of intersection of the beams can be altered at will without disturbing the spatial filter, collimation or beam quality, and assuring that the beams will always intersect at the position of the plate.

  16. Predicting S-wave velocities for unconsolidated sediments at low effective pressure

    USGS Publications Warehouse

    Lee, Myung W.

    2010-01-01

    Accurate S-wave velocities for shallow sediments are important in performing a reliable elastic inversion for gas hydrate-bearing sediments and in evaluating velocity models for predicting S-wave velocities, but few S-wave velocities are measured at low effective pressure. Predicting S-wave velocities by using conventional methods based on the Biot-Gassmann theory appears to be inaccurate for laboratory-measured velocities at effective pressures less than about 4-5 megapascals (MPa). Measured laboratory and well log velocities show two distinct trends for S-wave velocities with respect to P-wave velocity: one for the S-wave velocity less than about 0.6 kilometer per second (km/s) which approximately corresponds to effective pressure of about 4-5 MPa, and the other for S-wave velocities greater than 0.6 km/s. To accurately predict S-wave velocities at low effective pressure less than about 4-5 MPa, a pressure-dependent parameter that relates the consolidation parameter to shear modulus of the sediments at low effective pressure is proposed. The proposed method in predicting S-wave velocity at low effective pressure worked well for velocities of water-saturated sands measured in the laboratory. However, this method underestimates the well-log S-wave velocities measured in the Gulf of Mexico, whereas the conventional method performs well for the well log velocities. The P-wave velocity dispersion due to fluid in the pore spaces, which is more pronounced at high frequency with low effective pressures less than about 4 MPa, is probably a cause for this discrepancy.

  17. Impact of plunging breaking waves on a partially submerged cube

    NASA Astrophysics Data System (ADS)

    Wang, A.; Ikeda, C.; Duncan, J. H.

    2013-11-01

    The impact of a deep-water plunging breaking wave on a partially submerged cube is studied experimentally in a tank that is 14.8 m long and 1.2 m wide with a water depth of 0.91 m. The breakers are created from dispersively focused wave packets generated by a programmable wave maker. The water surface profile in the vertical center plane of the cube is measured using a cinematic laser-induced fluorescence technique with movie frame rates ranging from 300 to 4,500 Hz. The pressure distribution on the front face of the cube is measured with 24 fast-response sensors simultaneously with the wave profile measurements. The cube is positioned vertically at three heights relative to the mean water level and horizontally at a distance from the wave maker where a strong vertical water jet is formed. The portion of the water surface between the contact point on the front face of the cube and the wave crest is fitted with a circular arc and the radius and vertical position of the fitted circle is tracked during the impact. The vertical acceleration of the contact point reaches more than 50 times the acceleration of gravity and the pressure distribution just below the free surface shows a localized high-pressure region with a very high vertical pressure gradient. This work is supported by the Office of Naval Research under grant N000141110095.

  18. A Non-Intrusive Pressure Sensor by Detecting Multiple Longitudinal Waves

    PubMed Central

    Zhou, Hongliang; Lin, Weibin; Ge, Xiaocheng; Zhou, Jian

    2016-01-01

    Pressure vessels are widely used in industrial fields, and some of them are safety-critical components in the system—for example, those which contain flammable or explosive material. Therefore, the pressure of these vessels becomes one of the critical measurements for operational management. In the paper, we introduce a new approach to the design of non-intrusive pressure sensors, based on ultrasonic waves. The model of this sensor is built based upon the travel-time change of the critically refracted longitudinal wave (LCR wave) and the reflected longitudinal waves with the pressure. To evaluate the model, experiments are carried out to compare the proposed model with other existing models. The results show that the proposed model can improve the accuracy compared to models based on a single wave. PMID:27527183

  19. Fiber optic diffraction grating maker

    DOEpatents

    Deason, V.A.; Ward, M.B.

    1991-05-21

    A compact and portable diffraction grating maker is comprised of a laser beam, optical and fiber optics devices coupling the beam to one or more evanescent beam splitters, and collimating lenses or mirrors directing the split beam at an appropriate photosensitive material. The collimating optics, the output ends of the fiber optic coupler and the photosensitive plate holder are all mounted on an articulated framework so that the angle of intersection of the beams can be altered at will without disturbing the spatial filter, collimation or beam quality, and assuring that the beams will always intersect at the position of the plate. 4 figures.

  20. Changes in Cerebral Partial Oxygen Pressure and Cerebrovascular Reactivity During Intracranial Pressure Plateau Waves.

    PubMed

    Lang, Erhard W; Kasprowicz, Magdalena; Smielewski, Peter; Pickard, John; Czosnyka, Marek

    2015-08-01

    Plateau waves in intracranial pressure (ICP) are frequently recorded in neuro intensive care and are not yet fully understood. To further investigate this phenomenon, we analyzed partial pressure of cerebral oxygen (pbtO2) and a moving correlation coefficient between ICP and mean arterial blood pressure (ABP), called PRx, along with the cerebral oxygen reactivity index (ORx), which is a moving correlation coefficient between cerebral perfusion pressure (CPP) and pbtO2 in an observational study. We analyzed 55 plateau waves in 20 patients after severe traumatic brain injury. We calculated ABP, ABP pulse amplitude (ampABP), ICP, CPP, pbtO2, heart rate (HR), ICP pulse amplitude (ampICP), PRx, and ORx, before, during, and after each plateau wave. The analysis of variance with Bonferroni post hoc test was used to compare the differences in the variables before, during, and after the plateau wave. We considered all plateau waves, even in the same patient, independent because they are separated by long intervals. We found increases for ICP and ampICP according to our operational definitions for plateau waves. PRx increased significantly (p = 0.00026), CPP (p < 0.00001) and pbtO2 (p = 0.00007) decreased significantly during the plateau waves. ABP, ampABP, and HR remained unchanged. PRx during the plateau was higher than before the onset of wave in 40 cases (73 %) with no differences in baseline parameters for those with negative and positive ΔPRx (difference during and after). ORx showed an increase during and a decrease after the plateau waves, however, not statistically significant. PbtO2 overshoot after the wave occurred in 35 times (64 %), the mean difference was 4.9 ± 4.6 Hg (mean ± SD), and we found no difference in baseline parameters between those who overshoot and those who did not overshoot. Arterial blood pressure remains stable in ICP plateau waves, while cerebral autoregulatory indices show distinct changes, which indicate cerebrovascular

  1. Fluid pressure waves trigger earthquakes

    NASA Astrophysics Data System (ADS)

    Mulargia, Francesco; Bizzarri, Andrea

    2015-03-01

    Fluids-essentially meteoric water-are present everywhere in the Earth's crust, occasionally also with pressures higher than hydrostatic due to the tectonic strain imposed on impermeable undrained layers, to the impoundment of artificial lakes or to the forced injections required by oil and gas exploration and production. Experimental evidence suggests that such fluids flow along preferred paths of high diffusivity, provided by rock joints and faults. Studying the coupled poroelastic problem, we find that such flow is ruled by a nonlinear partial differential equation amenable to a Barenblatt-type solution, implying that it takes place in form of solitary pressure waves propagating at a velocity which decreases with time as v ∝ t [1/(n - 1) - 1] with n ≳ 7. According to Tresca-Von Mises criterion, these waves appear to play a major role in earthquake triggering, being also capable to account for aftershock delay without any further assumption. The measure of stress and fluid pressure inside active faults may therefore provide direct information about fault potential instability.

  2. On the pressure field of nonlinear standing water waves

    NASA Technical Reports Server (NTRS)

    Schwartz, L. W.

    1980-01-01

    The pressure field produced by two dimensional nonlinear time and space periodic standing waves was calculated as a series expansion in the wave height. The high order series was summed by the use of Pade approximants. Calculations included the pressure variation at great depth, which was considered to be a likely cause of microseismic activity, and the pressure distribution on a vertical barrier or breakwater.

  3. Diaphragm Pressure Wave Generator Developments at Industrial Research Ltd

    NASA Astrophysics Data System (ADS)

    Caughley, A. J.; Emery, N.; Glasson, N. D.

    2010-04-01

    Industrial Research Ltd (IRL) have been developing a unique diaphragm based pressure wave generator technology for pulse tube and Stirling cryocoolers. Our system uses a metal diaphragm to separate the clean cryocooler gas circuit from a conventionally lubricated mechanical driver, thus producing a clean pressure wave with a long life drive that does not require the precision manufacture and associated costs of large linear motors. The first successful diaphragm pressure wave generator produced 3.2 kW of acoustic power at an electro-acoustic efficiency of 72% with a swept volume of 200 ml and a prototype has now accumulated over 2500 hours running. This paper describes recent developments in the technology. To explore scaling, a small diaphragm pressure wave generator with a swept volume of 20 ml has been constructed and has delivered 454 W of acoustic power at an electro-acoustic efficiency of 60%. Improvements have been made to the hydraulic force amplifier mechanism for driving the diaphragms resulting in a cheaper and lighter mechanism than the mechanical linkage originally used. To meet a customer's specific requirements, the 200 ml pressure wave generator's stroke was extended to achieve 240 ml of swept volume thereby increasing its acoustic power delivery to 4.1 kW without compromising efficiency.

  4. Particle image velocimetry investigation of a finite amplitude pressure wave

    NASA Astrophysics Data System (ADS)

    Thornhill, D.; Currie, T.; Fleck, R.; Chatfield, G.

    2006-03-01

    Particle image velocimetry is used to study the motion of gas within a duct subject to the passage of a finite amplitude pressure wave. The wave is representative of the pressure waves found in the exhaust systems of internal combustion engines. Gas particles are accelerated from stationary to 150 m/s and then back to stationary in 8 ms. It is demonstrated that gas particles at the head of the wave travel at the same velocity across the duct cross section at a given point in time. Towards the tail of the wave viscous effects are plainly evident causing the flow profile to tend towards parabolic. However, the instantaneous mean particle velocity across the section is shown to match well with the velocity calculated from a corresponding measured pressure history using 1D gas dynamic theory. The measured pressure history at a point in the duct was acquired using a high speed pressure transducer of the type typically used for engine research in intake and exhaust systems. It is demonstrated that these are unable to follow the rapid changes in pressure accurately and that they are prone to resonate under certain circumstances.

  5. Mode Identification of High-Amplitude Pressure Waves in Liquid Rocket Engines

    NASA Astrophysics Data System (ADS)

    EBRAHIMI, R.; MAZAHERI, K.; GHAFOURIAN, A.

    2000-01-01

    Identification of existing instability modes from experimental pressure measurements of rocket engines is difficult, specially when steep waves are present. Actual pressure waves are often non-linear and include steep shocks followed by gradual expansions. It is generally believed that interaction of these non-linear waves is difficult to analyze. A method of mode identification is introduced. After presumption of constituent modes, they are superposed by using a standard finite difference scheme for solution of the classical wave equation. Waves are numerically produced at each end of the combustion tube with different wavelengths, amplitudes, and phases with respect to each other. Pressure amplitude histories and phase diagrams along the tube are computed. To determine the validity of the presented method for steep non-linear waves, the Euler equations are numerically solved for non-linear waves, and negligible interactions between these waves are observed. To show the applicability of this method, other's experimental results in which modes were identified are used. Results indicate that this simple method can be used in analyzing complicated pressure signal measurements.

  6. Generation of realistic tsunami waves using a bottom-tilting wave maker

    NASA Astrophysics Data System (ADS)

    Park, Yong Sung; Hwang, Jin Hwan

    2016-11-01

    Tsunamis have caused more than 260,000 human losses and 250 billion in damage worldwide in the last ten years. Observations made during 2011 Japan Tohoku Tsunami revealed that the commonly used waves (solitary waves) to model tsunamis are at least an order-of-magnitude shorter than the real tsunamis, which calls for re-evaluation of the current understanding of tsunamis. To prompt the required paradigm shift, a new wave generator, namely the bottom-tilting wave generator, has been developed at the University of Dundee. The wave tank is fitted with an adjustable slope and a bottom flap hinged at the beginning of the slope. By moving the bottom flap up and down, we can generate very long waves. Here we will report characteristics of waves generated by simple bottom motions, either moving it upward or downward from an initial displacement ending it being horizontal. Two parameters, namely the initial displacement of the bottom and the speed of the motion, determine characteristics of the generated waves. Wave amplitudes scale well with the volume flux of the displaced water. On the other hand, due to combined effects of nonlinearity and dispersion, wavelengths show more complicated relationship with the two bottom motion parameters. We will also demonstrate that by combining simple up and down motions, it is possible to generate waves resembling the one measured during 2011 tsunami. YSP acknowledges financial support from the Royal Society of Edinburgh through the Royal Society of Edinburgh and Scottish Government Personal Research Fellowship Co-Funded by the Marie-Curie Actions.

  7. Pressure threshold for shock wave induced renal hemorrhage.

    PubMed

    Mayer, R; Schenk, E; Child, S; Norton, S; Cox, C; Hartman, C; Cox, C; Carstensen, E

    1990-12-01

    Studies were performed with an interest in determining a pressure threshold for extracorporeal shock wave induced renal damage. Histological evidence of intraparenchymal hemorrhage was used as an indicator of tissue trauma. Depilated C3H mice were anesthetized and placed on a special frame to enhance visualization and treatment of the kidneys in situ. A Wolf electrohydraulic generator and 9 French probe designed for endoscopic use were utilized to expose the kidneys to 10 double spherically divergent shock waves. Measurements of the shock waves revealed two positive pressure peaks of similar magnitude for each spark discharge. The kidneys were exposed to different peak pressures by choice of distance from the spark source and were removed immediately after treatment for histologic processing. A dose response was noted with severe corticomedullary damage apparent following 15 to 20 MPa shocks. Hemorrhage was more apparent in the medulla where evidence of damage could be seen following pressures as low as three to five MPa. When a latex membrane was interposed to prevent possible collapse of the initial bubble from the spark source against the skin surface, histological evaluation revealed substantial reduction of severe tissue damage associated with the highest pressures tested, 20 MPa. However, the threshold level for evidence of hemorrhage remained about three to five MPa. Hydrophonic measurements indicated that the membrane allowed transmission of the acoustic shock waves and suggested that collapse of the bubble generated by electrohydraulic probes may have local effects due to a cavitation-like mechanism.

  8. Air pressure waves from Mount St. Helens eruptions

    NASA Astrophysics Data System (ADS)

    Reed, Jack W.

    1987-10-01

    Infrasonic recordings of the pressure wave from the Mount St. Helens (MSH) eruption on May 18, 1980, together with the weather station barograph records were used to estimate an equivalent explosion airblast yield for this eruption. Pressure wave amplitudes versus distance patterns were found to be comparable with patterns found for a small-scale nuclear explosion, the Krakatoa eruption, and the Tunguska comet impact, indicating that the MSH wave came from an explosion equivalent of about 5 megatons of TNT. The peculiar audibility pattern reported, with the blast being heard only at ranges beyond about 100 km, is explained by consideration of finite-amplitude shock propagation developments.

  9. Onsite Portable Alarm System - Its Merit and Application

    NASA Astrophysics Data System (ADS)

    Saita, J.; Sato, T.; Nakamura, Y.

    2007-12-01

    Recently an existence of the earthquake early warning system (EEWS) becomes popular. In general, the EEWS will be installed in a fixed observation site and it may consist of several separated components such as a sensing portion, A/D converter, an information processing potion and so on. The processed information for warning may be transmitted to network via fixed communication line, and therefore this kind of alarm system is called as Network Alarm System. On the other hand, after the severe earthquake damage, it is very important to save the disaster victims immediately. These rescue staffs are also under the risk of aftershocks and need a local alarm not depending on the network, so this kind of alarm can be called as Onsite Alarm. But the common early warning system is too complex to set onsite temporary, and even if possible to install, the alarm is too late to receive at the epicentral area. However, the new generation earthquake early warning system FREQL can issue the P wave alarm by minimum 0.2 seconds after P wave detection. And FREQL is characterized as the unique all-in-one seismometer with power unit. At the time of the 2004 Niigata-Ken-Chuetsu earthquake, a land slide attacked a car just passing. A hyper rescue team of Tokyo Fire Department pulled the survivor, one baby, from the land slide area. During their activity the rescue team was exposed to the risk of secondary hazards caused by the aftershocks. It was clear that it is necessary to use a portable warning system to issue the onsite P wave alarm. Because FREQL was originally developed as portable equipment, Tokyo Fire Department asked us to modify it to the portable equipment with the loud sound and the light signal. In this moment, this portable FREQL has equipped in nation wide. When the hyper rescue team of Tokyo Fire Department was sent to Pakistan as a task force for rescue work of the 2005 Pakistan earthquake, the portable FREQL was used as important onsite portable warning system and P

  10. Spatial patterns of fasting and fed antropyloric pressure waves in humans.

    PubMed Central

    Sun, W M; Hebbard, G S; Malbert, C H; Jones, K L; Doran, S; Horowitz, M; Dent, J

    1997-01-01

    1. Gastric mechanics were investigated by categorizing the temporal and spatial patterning of pressure waves associated with individual gastric contractions. 2. In twelve healthy volunteers, intraluminal pressures were monitored from nine side hole recording points spaced at 1.5 cm intervals along the antrum, pylorus and duodenum. 3. Pressure wave sequences that occurred during phase II fasting contractions (n = 221) and after food (n = 778) were evaluated. 4. The most common pattern of pressure wave onset along the antrum was a variable combination of antegrade, synchronous and retrograde propagation between side hole pairs. This variable pattern accounted for 42% of sequences after food, and 34% during fasting (P < 0.05). Other common pressure wave sequence patterns were: purely antegrade-29% after food and 42% during fasting (P < 0.05); purely synchronous-23% fed and 17% fasting; and purely retrograde-6% fed and 8% fasting. The length of sequences was shorter after food (P < 0.05). Some sequences 'skipped' individual recording points. 5. The spatial patterning of gastric pressure wave sequences is diverse, and may explain the differing mechanical outcomes among individual gastric contractions. 6. Better understanding of gastric mechanics may be gained from temporally precise correlations of luminal flows and pressures and gastric wall motion during individual gastric contraction sequences. PMID:9306286

  11. 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.

  12. 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.

  13. Portable concealed weapon detection using millimeter-wave FMCW radar imaging

    NASA Astrophysics Data System (ADS)

    Johnson, Michael A.; Chang, Yu-Wen

    2001-02-01

    Unobtrusive detection of concealed weapons on persons or in abandoned bags would provide law enforcement a powerful tool to focus resources and increase traffic throughput in high- risk situations. We have developed a fast image scanning 94 GHz radar system that is suitable for portable operation and remote viewing of radar data. This system includes a novel fast image-scanning antenna that allows for the acquisition of medium resolution 3D millimeter wave images of stationary targets with frame times on order of one second. The 3D radar data allows for potential isolation of concealed weapons from body and environmental clutter such as nearby furniture or other people. The radar is an active system so image quality is not affected indoors, emitted power is however very low so there are no health concerns for operator or targets. The low power operation is still sufficient to penetrate heavy clothing or material. Small system size allows for easy transport and rapid deployment of the system as well as an easy migration path to future hand held systems.

  14. Genesis of the characteristic pulmonary venous pressure waveform as described by the reservoir-wave model

    PubMed Central

    Bouwmeester, J Christopher; Belenkie, Israel; Shrive, Nigel G; Tyberg, John V

    2014-01-01

    Conventional haemodynamic analysis of pulmonary venous and left atrial (LA) pressure waveforms yields substantial forward and backward waves throughout the cardiac cycle; the reservoir wave model provides an alternative analysis with minimal waves during diastole. Pressure and flow in a single pulmonary vein (PV) and the main pulmonary artery (PA) were measured in anaesthetized dogs and the effects of hypoxia and nitric oxide, volume loading, and positive-end expiratory pressure (PEEP) were observed. The reservoir wave model was used to determine the reservoir contribution to PV pressure and flow. Subtracting reservoir pressure and flow resulted in ‘excess’ quantities which were treated as wave-related. Wave intensity analysis of excess pressure and flow quantified the contributions of waves originating upstream (from the PA) and downstream (from the LA and/or left ventricle (LV)). Major features of the characteristic PV waveform are caused by sequential LA and LV contraction and relaxation creating backward compression (i.e. pressure-increasing) waves followed by decompression (i.e. pressure-decreasing) waves. Mitral valve opening is linked to a backwards decompression wave (i.e. diastolic suction). During late systole and early diastole, forward waves originating in the PA are significant. These waves were attenuated less with volume loading and delayed with PEEP. The reservoir wave model shows that the forward and backward waves are negligible during LV diastasis and that the changes in pressure and flow can be accounted for by the discharge of upstream reservoirs. In sharp contrast, conventional analysis posits forward and backward waves such that much of the energy of the forward wave is opposed by the backward wave. PMID:25015922

  15. 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.

  16. On propagation of axisymmetric waves in pressurized functionally graded elastomeric hollow cylinders

    NASA Astrophysics Data System (ADS)

    Wu, Bin; Su, Yipin; Liu, Dongying; Chen, Weiqiu; Zhang, Chuanzeng

    2018-05-01

    Soft materials can be designed with a functionally graded (FG) property for specific applications. Such material inhomogeneity can also be found in many soft biological tissues whose functionality is only partly understood to date. In this paper, we analyze the axisymmetric guided wave propagation in a pressurized FG elastomeric hollow cylinder. The cylinder is subjected to a combined action of axial pre-stretch and pressure difference applied to the inner and outer cylindrical surfaces. We consider both torsional waves and longitudinal waves propagating in the FG cylinder made of incompressible isotropic elastomer, which is characterized by the Mooney-Rivlin strain energy function but with the material parameters varying with the radial coordinate in an affine way. The pressure difference generates an inhomogeneous deformation field in the FG cylinder, which dramatically complicates the superimposed wave problem described by the small-on-large theory. A particularly efficient approach is hence employed which combines the state-space formalism for the incremental wave motion with the approximate laminate or multi-layer technique. Dispersion relations for the two types of axisymmetric guided waves are then derived analytically. The accuracy and convergence of the proposed approach is validated numerically. The effects of the pressure difference, material gradient, and axial pre-stretch on both the torsional and the longitudinal wave propagation characteristics are discussed in detail through numerical examples. It is found that the frequency of axisymmetric waves depends nonlinearly on the pressure difference and the material gradient, and an increase in the material gradient enhances the capability of the pressure difference to adjust the wave behavior in the FG cylinder. This work provides a theoretical guidance for characterizing FG soft materials by in-situ ultrasonic nondestructive evaluation and for designing tunable waveguides via material tailoring along

  17. Ultrasonic wave based pressure measurement in small diameter pipeline.

    PubMed

    Wang, Dan; Song, Zhengxiang; Wu, Yuan; Jiang, Yuan

    2015-12-01

    An effective non-intrusive method of ultrasound-based technique that allows monitoring liquid pressure in small diameter pipeline (less than 10mm) is presented in this paper. Ultrasonic wave could penetrate medium, through the acquisition of representative information from the echoes, properties of medium can be reflected. This pressure measurement is difficult due to that echoes' information is not easy to obtain in small diameter pipeline. The proposed method is a study on pipeline with Kneser liquid and is based on the principle that the transmission speed of ultrasonic wave in pipeline liquid correlates with liquid pressure and transmission speed of ultrasonic wave in pipeline liquid is reflected through ultrasonic propagation time providing that acoustic distance is fixed. Therefore, variation of ultrasonic propagation time can reflect variation of pressure in pipeline. Ultrasonic propagation time is obtained by electric processing approach and is accurately measured to nanosecond through high resolution time measurement module. We used ultrasonic propagation time difference to reflect actual pressure in this paper to reduce the environmental influences. The corresponding pressure values are finally obtained by acquiring the relationship between variation of ultrasonic propagation time difference and pressure with the use of neural network analysis method, the results show that this method is accurate and can be used in practice. Copyright © 2015 Elsevier B.V. All rights reserved.

  18. Development of High Precision Metal Micro-Electro-Mechanical-Systems Column for Portable Surface Acoustic Wave Gas Chromatograph

    NASA Astrophysics Data System (ADS)

    Iwaya, Takamitsu; Akao, Shingo; Sakamoto, Toshihiro; Tsuji, Toshihiro; Nakaso, Noritaka; Yamanaka, Kazushi

    2012-07-01

    In the field of environmental measurement and security, a portable gas chromatograph (GC) is required for the on-site analysis of multiple hazardous gases. Although the gas separation column has been downsized using micro-electro-mechanical-systems (MEMS) technology, an MEMS column made of silicon and glass still does not have sufficient robustness and a sufficiently low fabrication cost for a portable GC. In this study, we fabricated a robust and inexpensive high-precision metal MEMS column by combining diffusion-bonded etched stainless-steel plates with alignment evaluation using acoustic microscopy. The separation performance was evaluated using a desktop GC with a flame ionization detector and we achieved the high separation performance comparable to the best silicon MEMS column fabricated using a dynamic coating method. As an application, we fabricated a palm-size surface acoustic wave (SAW) GC combining this column with a ball SAW sensor and succeeded in separating and detecting a mixture of volatile organic compounds.

  19. Forced wave induced by an atmospheric pressure disturbance moving towards shore

    NASA Astrophysics Data System (ADS)

    Chen, Yixiang; Niu, Xiaojing

    2018-05-01

    Atmospheric pressure disturbances moving over a vast expanse of water can induce different wave patterns, which can be determined by the Froude number Fr. Generally, Fr = 1 is a critical value for the transformation of the wave pattern and the well-known Proudman resonance happens when Fr = 1. In this study, the forced wave induced by an atmospheric pressure disturbance moving over a constant slope from deep sea to shore is numerically investigated. The wave pattern evolves from a concentric-circle type into a triangular type with the increase of the Froude number, as the local water depth decreases, which is in accord with the analysis in the unbounded flat-bottom cases. However, a hysteresis effect has been observed, which implies the obvious amplification of the forced wave induced by a pressure disturbance can not be simply predicted by Fr = 1. The effects of the characteristic parameters of pressure disturbances and slope gradient have been discussed. The results show that it is not always possible to observe significant peak of the maximum water elevation before the landing of pressure disturbances, and a significant peak can be generated by a pressure disturbance with small spatial scale and fast moving velocity over a milder slope. Besides, an extremely high run-up occurs when the forced wave hits the shore, which is an essential threat to coastal security. The results also show that the maximum run-up is not monotonously varying with the increase of disturbance moving speed and spatial scale. There exists a most dangerous speed and scale which may cause disastrous nearshore surge.

  20. 49 CFR 178.274 - Specifications for UN portable tanks.

    Code of Federal Regulations, 2010 CFR

    2010-10-01

    ... and 178.277, as applicable. Design type means a portable tank or series of portable tanks made of... the top of the shell during the hydraulic pressure test equal to not less than 1.5 times the design... be designed and constructed to withstand a hydraulic test pressure of not less than 1.5 times the...

  1. 49 CFR 178.274 - Specifications for UN portable tanks.

    Code of Federal Regulations, 2013 CFR

    2013-10-01

    ... and 178.277, as applicable. Design type means a portable tank or series of portable tanks made of... the top of the shell during the hydraulic pressure test equal to not less than 1.5 times the design... be designed and constructed to withstand a hydraulic test pressure of not less than 1.5 times the...

  2. Portable device for detection of petit mal epilepsy

    NASA Technical Reports Server (NTRS)

    Smith, R. G.; Houge, J. C.; Webster, J. G.

    1979-01-01

    A portable device that analyzes the electroencephalogram to determine if petit mal epilepsy waveforms are present is developed and tested. Clinicians should find it useful in diagnosing seizure activity of their patients. The micropower, battery-operated, portable device indicates a seizure has occurred if three criteria are satisfied: (1) frequencies of 2.5-7 Hz, (2) large-amplitude waves, and (3) minimum number of waves per second. Levels and counts are adjustable, thus insuring high reliability against noise artifacts and permitting each subject to be individually fitted. The device has shown promise in giving the patient a possible mechanism of seizure control or suppression.

  3. Influence of flow and pressure on wave propagation in the canine aorta.

    NASA Technical Reports Server (NTRS)

    Histand, M. B.; Anliker, M.

    1973-01-01

    Data on wave speed acquired from 20 anesthetized dogs showed that the thoracic aorta was essentially nondispersive for small artificially generated pressure waves traveling in the downstream or the upstream direction and having frequencies between 40 and 120 Hz. The amplitude of these waves decayed exponentially with the distance traveled. Theoretical studies are cited which have shown that changes in wave speed due to variations in pressure and flow produce marked nonlinear effects in hemodynamics.

  4. Cardiac output in idiopathic normal pressure hydrocephalus: association with arterial blood pressure and intracranial pressure wave amplitudes and outcome of shunt surgery

    PubMed Central

    2011-01-01

    Background In patients with idiopathic normal pressure hydrocephalus (iNPH) responding to shunt surgery, we have consistently found elevated intracranial pressure (ICP) wave amplitudes during diagnostic ICP monitoring prior to surgery. It remains unknown why ICP wave amplitudes are increased in these patients. Since iNPH is accompanied by a high incidence of vascular co-morbidity, a possible explanation is that there is reduced vascular compliance accompanied by elevated arterial blood pressure (ABP) wave amplitudes and even altered cardiac output (CO). To investigate this possibility, the present study was undertaken to continuously monitor CO to determine if it is correlated to ABP and ICP wave amplitudes and the outcome of shunting in iNPH patients. It was specifically addressed whether the increased ICP wave amplitudes seen in iNPH shunt responders were accompanied by elevated CO and/or ABP wave amplitude levels. Methods Prospective iNPH patients (29) were clinically graded using an NPH grading scale. Continuous overnight minimally-invasive monitoring of CO and ABP was done simultaneously with ICP monitoring; the CO, ABP, and ICP parameters were parsed into 6-second time windows. Patients were assessed for shunt surgery on clinical grade, Evan's index, and ICP wave amplitude. Follow-up clinical grading was performed 12 months after surgery. Results ICP wave amplitudes but not CO or ABP wave amplitude, showed good correlation with the response to shunt treatment. The patients with high ICP wave amplitude did not have accompanying high levels of CO or ABP wave amplitude. Correlation analysis between CO and ICP wave amplitudes in individual patients showed different profiles [significantly positive in 10 (35%) and significantly negative in 16 (55%) of 29 recordings]. This depended on whether there was also a correlation between ABP and ICP wave amplitudes and on the average level of ICP wave amplitude. Conclusions These results gave no evidence that the increased

  5. Unique determination of stratified steady water waves from pressure

    NASA Astrophysics Data System (ADS)

    Chen, Robin Ming; Walsh, Samuel

    2018-01-01

    Consider a two-dimensional stratified solitary wave propagating through a body of water that is bounded below by an impermeable ocean bed. In this work, we study how such a wave can be recovered from data consisting of the wave speed, upstream and downstream density and velocity profile, and the trace of the pressure on the bed. In particular, we prove that this data uniquely determines the wave, both in the (real) analytic and Sobolev regimes.

  6. Comparison of two ways of altering carpal tunnel pressure with ultrasound surface wave elastography.

    PubMed

    Cheng, Yu-Shiuan; Zhou, Boran; Kubo, Kazutoshi; An, Kai-Nan; Moran, Steven L; Amadio, Peter C; Zhang, Xiaoming; Zhao, Chunfeng

    2018-06-06

    Higher carpal tunnel pressure is related to the development of carpal tunnel syndrome. Currently, the measurement of carpal tunnel pressure is invasive and therefore, a noninvasive technique is needed. We previously demonstrated that speed of wave propagation through a tendon in the carpal tunnel measured by ultrasound elastography could be used as an indicator of carpal tunnel pressure in a cadaveric model, in which a balloon had to be inserted into the carpal tunnel to adjust the carpal tunnel pressure. However, the method for adjusting the carpal tunnel pressure in the cadaveric model is not applicable for the in vivo model. The objective of this study was to utilize a different technique to adjust carpal tunnel pressure via pressing the palm and to validate it with ultrasound surface wave elastography in a human cadaveric model. The outcome was also compared with a previous balloon insertion technique. Results showed that wave speed of intra-carpal tunnel tendon and the ratio of wave speed of intra-and outer-carpal tunnel tendons increased linearly with carpal tunnel pressure. Moreover, wave speed of intra carpal tunnel tendon via both ways of altering carpal tunnel pressure showed similar results with high correlation. Therefore, it was concluded that the technique of pressing the palm can be used to adjust carpal tunnel pressure, and pressure changes can be detected via ultrasound surface wave elastography in an ex vivo model. Future studies will utilize this technique in vivo to validate the usefulness of ultrasound surface wave elastography for measuring carpal tunnel pressure. Copyright © 2018 Elsevier Ltd. All rights reserved.

  7. Portable Fluorescence Imaging System for Hypersonic Flow Facilities

    NASA Technical Reports Server (NTRS)

    Wilkes, J. A.; Alderfer, D. W.; Jones, S. B.; Danehy, P. M.

    2003-01-01

    A portable fluorescence imaging system has been developed for use in NASA Langley s hypersonic wind tunnels. The system has been applied to a small-scale free jet flow. Two-dimensional images were taken of the flow out of a nozzle into a low-pressure test section using the portable planar laser-induced fluorescence system. Images were taken from the center of the jet at various test section pressures, showing the formation of a barrel shock at low pressures, transitioning to a turbulent jet at high pressures. A spanwise scan through the jet at constant pressure reveals the three-dimensional structure of the flow. Future capabilities of the system for making measurements in large-scale hypersonic wind tunnel facilities are discussed.

  8. Portable evanescent wave fiber biosensor for highly sensitive detection of Shigella

    NASA Astrophysics Data System (ADS)

    Xiao, Rui; Rong, Zhen; Long, Feng; Liu, Qiqi

    2014-11-01

    A portable evanescent wave fiber biosensor was developed to achieve the rapid and highly sensitive detection of Shigella. In this study, a DNA probe was covalently immobilized onto fiber-optic biosensors that can hybridize with a fluorescently labeled complementary DNA. The sensitivity of detection for synthesized oligonucleotides can reach 10-10 M. The surface of the sensor can be regenerated with 0.5% sodium dodecyl sulfate solution (pH 1.9) for over 30 times without significant deterioration of performance. The total analysis time for a single sample, including the time for measurement and surface regeneration, was less than 6 min. We employed real-time polymerase chain reaction (PCR) and compared the results of both methods to investigate the actual Shigella DNA detection capability of the fiber-optic biosensor. The fiber-optic biosensor could detect as low as 102 colony-forming unit/mL Shigella. This finding was comparable with that by real-time PCR, which suggests that this method is a potential alternative to existing detection methods.

  9. S-Wave Velocity Models Under the Saudi Arabian Portable Broadband Deployment: Evidence for Lithospheric Erosion Beneath the Arabian Shield

    NASA Astrophysics Data System (ADS)

    Julià, J.; Ammon, C. J.; Herrmann, R. B.

    2002-12-01

    Models of crustal evolution strongly rely on our knowledge on the mineralogical composition of subsurface rocks, as well as pressure and temperature conditions. Direct sampling of subsurface rocks is often not possible, so that constraints have to be placed from indirect estimates of rock properties. Detailed seismic imaging of subsurface rocks has the potential for providing such constraints, and probe the extent at depth of surface geologic observations. In this study, we provide detailed S-wave velocity profiles for the crust and uppermost mantle beneath the Saudi Arabian Portable Broadband Deployment stations. Seismic velocities have been estimated from the joint inversion of receiver functions and fundamental mode group velocities. Receiver functions are sensitive to S-wave velocity contrasts and vertical travel times, and surface-wave dispersion is sensitive to vertical S-wave velocity averages, so that their combination bridge resolution gaps associated with each individual data set. Our resulting models correlate well with surface geology observations in the Arabian Shield and characterize its terranes at depth: the Asir terrane consists of a 10-km thick upper crust of 3.3~km/s overlying a lower crust with shear-wave velocities of 3.7-3.8 km/s; the Afif terrane is made of a 20-km thick upper crust with average velocity of 3.6 km/s and a lower crust with a shear-velocity of about 3.8~km/s; the Nabitah mobile belt has a gradational, 15-km thick upper crust up to 3.6 km/s overlying a gradational lower crust with velocities up to 4.0 km/s. The crust-mantle transition is sharper in terranes of continental affinity and more gradational beneath terranes of oceanic affinity. In the uppermost mantle, our models suggest a thin lid between up to 50-60 km depth overlying a low velocity zone beneath station TAIF, located close to a region of upwelling mantle material. Temperatures in the lid are estimated to be about 1000 C, which are in good agreement with independent

  10. Relationship between orientation to a blast and pressure wave propagation inside the rat brain.

    PubMed

    Chavko, Mikulas; Watanabe, Tomas; Adeeb, Saleena; Lankasky, Jason; Ahlers, Stephen T; McCarron, Richard M

    2011-01-30

    Exposure to a blast wave generated during an explosion may result in brain damage and related neurological impairments. Several mechanisms by which the primary blast wave can damage the brain have been proposed, including: (1) a direct effect of the shock wave on the brain causing tissue damage by skull flexure and propagation of stress and shear forces; and (2) an indirect transfer of kinetic energy from the blast, through large blood vessels and cerebrospinal fluid (CSF), to the central nervous system. To address a basic question related to the mechanisms of blast brain injury, pressure was measured inside the brains of rats exposed to a low level of blast (~35kPa), while positioned in three different orientations with respect to the primary blast wave; head facing blast, right side exposed to blast and head facing away from blast. Data show different patterns and durations of the pressure traces inside the brain, depending on the rat orientation to blast. Frontal exposures (head facing blast) resulted in pressure traces of higher amplitude and longer duration, suggesting direct transmission and reflection of the pressure inside the brain (dynamic pressure transfer). The pattern of the pressure wave inside the brain in the head facing away from blast exposures assumes contribution of the static pressure, similar to hydrodynamic pressure to the pressure wave inside the brain. Published by Elsevier B.V.

  11. Fluid-structure interaction dynamic simulation of spring-loaded pressure relief valves under seismic wave

    NASA Astrophysics Data System (ADS)

    Lv, Dongwei; Zhang, Jian; Yu, Xinhai

    2018-05-01

    In this paper, a fluid-structure interaction dynamic simulation method of spring-loaded pressure relief valve was established. The dynamic performances of the fluid regions and the stress and strain of the structure regions were calculated at the same time by accurately setting up the contact pairs between the solid parts and the coupling surfaces between the fluid regions and the structure regions. A two way fluid-structure interaction dynamic simulation of a simplified pressure relief valve model was carried out. The influence of vertical sinusoidal seismic waves on the performance of the pressure relief valve was preliminarily investigated by loading sine waves. Under vertical seismic waves, the pressure relief valve will flutter, and the reseating pressure was affected by the amplitude and frequency of the seismic waves. This simulation method of the pressure relief valve under vertical seismic waves can provide effective means for investigating the seismic performances of the valves, and make up for the shortcomings of the experiment.

  12. Modeling and simulation of pressure waves generated by nano-thermite reactions

    NASA Astrophysics Data System (ADS)

    Martirosyan, Karen S.; Zyskin, Maxim; Jenkins, Charles M.; (Yuki) Horie, Yasuyuki

    2012-11-01

    This paper reports the modeling of pressure waves from the explosive reaction of nano-thermites consisting of mixtures of nanosized aluminum and oxidizer granules. Such nanostructured thermites have higher energy density (up to 26 kJ/cm3) and can generate a transient pressure pulse four times larger than that from trinitrotoluene (TNT) based on volume equivalence. A plausible explanation for the high pressure generation is that the reaction times are much shorter than the time for a shock wave to propagate away from the reagents region so that all the reaction energy is dumped into the gaseous products almost instantaneously and thereby a strong shock wave is generated. The goal of the modeling is to characterize the gas dynamic behavior for thermite reactions in a cylindrical reaction chamber and to model the experimentally measured pressure histories. To simplify the details of the initial stage of the explosive reaction, it is assumed that the reaction generates a one dimensional shock wave into an air-filled cylinder and propagates down the tube in a self-similar mode. Experimental data for Al/Bi2O3 mixtures were used to validate the model with attention focused on the ratio of specific heats and the drag coefficient. Model predictions are in good agreement with the measured pressure histories.

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

    NASA Technical Reports Server (NTRS)

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

    1992-01-01

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

  14. Initial condition effect on pressure waves in an axisymmetric jet

    NASA Technical Reports Server (NTRS)

    Miles, Jeffrey H.; Raman, Ganesh

    1988-01-01

    A pair of microphones (separated axially by 5.08 cm and laterally by 1.3 cm) are placed on either side of the jet centerline to investigate coherent pressure fluctuations in an axisymmetric jet at Strouhal numbers less than unity. Auto-spectra, transfer-function, and coherence measurements are made for a tripped and untripped boundary layer initial condition. It was found that coherent acoustic pressure waves originating in the upstream plenum chamber propagate a greater distance downstream for the tripped initial condition than for the untripped initial condition. In addition, for the untripped initial condition the development of the coherent hydrodynamic pressure waves shifts downstream.

  15. Intracochlear pressure measurements during acoustic shock wave exposure.

    PubMed

    Greene, Nathaniel T; Alhussaini, Mohamed A; Easter, James R; Argo, Theodore F; Walilko, Tim; Tollin, Daniel J

    2018-05-19

    Injuries to the peripheral auditory system are among the most common results of high intensity impulsive acoustic 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 pressure in human cadaveric temporal bones, with fiber optic pressure sensors placed in scala vestibuli (SV) and tympani (ST), during exposure to shock waves with peak positive pressures between ∼7 and 83 kPa. Eight full-cephalic human cadaver heads were exposed, face-on, to acoustic 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 pressure levels were measured with fiber-optic pressure 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 pressures 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 pressure showed gain, calculated from the frequency spectra, consistent with the ear canal resonance, and gain in the intracochlear pressures (normalized to the EAC pressure) 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

  16. Pressure wave propagation in fluid-filled co-axial elastic tubes. Part 1: Basic theory.

    PubMed

    Berkouk, K; Carpenter, P W; Lucey, A D

    2003-12-01

    Our work is motivated by ideas about the pathogenesis of syringomyelia. This is a serious disease characterized by the appearance of longitudinal cavities within the spinal cord. Its causes are unknown, but pressure propagation is probably implicated. We have developed an inviscid theory for the propagation of pressure waves in co-axial, fluid-filled, elastic tubes. This is intended as a simple model of the intraspinal cerebrospinal-fluid system. Our approach is based on the classic theory for the propagation of longitudinal waves in single, fluid-filled, elastic tubes. We show that for small-amplitude waves the governing equations reduce to the classic wave equation. The wave speed is found to be a strong function of the ratio of the tubes' cross-sectional areas. It is found that the leading edge of a transmural pressure pulse tends to generate compressive waves with converging wave fronts. Consequently, the leading edge of the pressure pulse steepens to form a shock-like elastic jump. A weakly nonlinear theory is developed for such an elastic jump.

  17. Increased aortic wave reflection contributes to higher systolic blood pressure in adolescents born preterm.

    PubMed

    Kowalski, Remi R; Beare, Richard; Mynard, Jonathan P; Cheong, Jeanie L Y; Doyle, Lex W; Smolich, Joseph J; Cheung, Michael M H

    2018-03-29

    To evaluate the wave reflection characteristics in the aortic arch and common carotid artery of ex-preterm adolescents and assess their relationship to central blood pressure in a cohort followed prospectively since birth. Central blood pressures, pulse wave velocity, augmentation index, microvascular reactive hyperemia, arterial distensibility, compliance and stiffness index, and also aortic and carotid wave intensity were measured in 18-year-olds born extremely preterm at below 28 weeks' gestation (n = 76) and term-born controls (n = 42). Compared with controls, ex-preterm adolescents had higher central systolic (111 ± 11 vs. 105 ± 10 mmHg; P < 0.001) and diastolic blood pressures (73 ± 7 vs. 67 ± 7 mmHg; P < 0.001). Although conventional measures of arterial function and biomechanics such as pulse wave velocity and augmentation index were no different between groups, wave intensity analysis revealed elevated backward compression wave area (-0.39 ± 0.21 vs. -0.29 ± 0.17 W/m/s × 10; P = 0.03), backward compression wave pressure change (9.0 ± 3.5 vs. 6.6 ± 2.5 mmHg; P = 0.001) and reflection index (0.44 ± 0.15 vs. 0.32 ± 0.08; P < 0.001) in the aorta of ex-preterm adolescents compared with controls. These changes were less pronounced in the carotid artery. On multivariable analysis, forward and backward compression wave areas were the only biomechanical variables associated with central systolic pressure. Ex-preterm adolescents demonstrate elevated wave reflection indices in the aortic arch, which correlate with central systolic pressure. Wave intensity analysis may provide a sensitive novel marker of evolving vascular dysfunction in ex-preterm survivors.

  18. Models of brachial to finger pulse wave distortion and pressure decrement.

    PubMed

    Gizdulich, P; Prentza, A; Wesseling, K H

    1997-03-01

    To model the pulse wave distortion and pressure decrement occurring between brachial and finger arteries. Distortion reversion and decrement correction were also our aims. Brachial artery pressure was recorded intra-arterially and finger pressure was recorded non-invasively by the Finapres technique in 53 adult human subjects. Mean pressure was subtracted from each pressure waveform and Fourier analysis applied to the pulsations. A distortion model was estimated for each subject and averaged over the group. The average inverse model was applied to the full finger pressure waveform. The pressure decrement was modelled by multiple regression on finger systolic and diastolic levels. Waveform distortion could be described by a general, frequency dependent model having a resonance at 7.3 Hz. The general inverse model has an anti-resonance at this frequency. It converts finger to brachial pulsations thereby reducing average waveform distortion from 9.7 (s.d. 3.2) mmHg per sample for the finger pulse to 3.7 (1.7) mmHg for the converted pulse. Systolic and diastolic level differences between finger and brachial arterial pressures changed from -4 (15) and -8 (11) to +8 (14) and +8 (12) mmHg, respectively, after inverse modelling, with pulse pressures correct on average. The pressure decrement model reduced both the mean and the standard deviation of systolic and diastolic level differences to 0 (13) and 0 (8) mmHg. Diastolic differences were thus reduced most. Brachial to finger pulse wave distortion due to wave reflection in arteries is almost identical in all subjects and can be modelled by a single resonance. The pressure decrement due to flow in arteries is greatest for high pulse pressures superimposed on low means.

  19. Effect of pressurization on helical guided wave energy velocity in fluid-filled pipes.

    PubMed

    Dubuc, Brennan; Ebrahimkhanlou, Arvin; Salamone, Salvatore

    2017-03-01

    The effect of pressurization stresses on helical guided waves in a thin-walled fluid-filled pipe is studied by modeling leaky Lamb waves in a stressed plate bordered by fluid. Fluid pressurization produces hoop and longitudinal stresses in a thin-walled pipe, which corresponds to biaxial in-plane stress in a plate waveguide model. The effect of stress on guided wave propagation is accounted for through nonlinear elasticity and finite deformation theory. Emphasis is placed on the stress dependence of the energy velocity of the guided wave modes. For this purpose, an expression for the energy velocity of leaky Lamb waves in a stressed plate is derived. Theoretical results are presented for the mode, frequency, and directional dependent variations in energy velocity with respect to stress. An experimental setup is designed for measuring variations in helical wave energy velocity in a thin-walled water-filled steel pipe at different levels of pressure. Good agreement is achieved between the experimental variations in energy velocity for the helical guided waves and the theoretical leaky Lamb wave solutions. Copyright © 2016 Elsevier B.V. All rights reserved.

  20. A fast estimation of shock wave pressure based on trend identification

    NASA Astrophysics Data System (ADS)

    Yao, Zhenjian; Wang, Zhongyu; Wang, Chenchen; Lv, Jing

    2018-04-01

    In this paper, a fast method based on trend identification is proposed to accurately estimate the shock wave pressure in a dynamic measurement. Firstly, the collected output signal of the pressure sensor is reconstructed by discrete cosine transform (DCT) to reduce the computational complexity for the subsequent steps. Secondly, the empirical mode decomposition (EMD) is applied to decompose the reconstructed signal into several components with different frequency-bands, and the last few low-frequency components are chosen to recover the trend of the reconstructed signal. In the meantime, the optimal component number is determined based on the correlation coefficient and the normalized Euclidean distance between the trend and the reconstructed signal. Thirdly, with the areas under the gradient curve of the trend signal, the stable interval that produces the minimum can be easily identified. As a result, the stable value of the output signal is achieved in this interval. Finally, the shock wave pressure can be estimated according to the stable value of the output signal and the sensitivity of the sensor in the dynamic measurement. A series of shock wave pressure measurements are carried out with a shock tube system to validate the performance of this method. The experimental results show that the proposed method works well in shock wave pressure estimation. Furthermore, comparative experiments also demonstrate the superiority of the proposed method over the existing approaches in both estimation accuracy and computational efficiency.

  1. Implications of pressure diffusion for shock waves

    NASA Technical Reports Server (NTRS)

    Ram, Ram Bachan

    1989-01-01

    The report deals with the possible implications of pressure diffusion for shocks in one dimensional traveling waves in an ideal gas. From this new hypothesis all aspects of such shocks can be calculated except shock thickness. Unlike conventional shock theory, the concept of entropy is not needed or used. Our analysis shows that temperature rises near a shock, which is of course an experimental fact; however, it also predicts that very close to a shock, density increases faster than pressure. In other words, a shock itself is cold.

  2. Pressure wave charged repetitively pulsed gas laser

    DOEpatents

    Kulkarny, Vijay A.

    1982-01-01

    A repetitively pulsed gas laser in which a system of mechanical shutters bracketing the laser cavity manipulate pressure waves resulting from residual energy in the cavity gas following a lasing event so as to draw fresh gas into the cavity and effectively pump spent gas in a dynamic closed loop.

  3. Portable tester for determining gas content within a core sample

    DOEpatents

    Garcia, Jr., Fred; Schatzel, Steven J.

    1998-01-01

    A portable tester is provided for reading and displaying the pressure of a gas released from a rock core sample stored within a sealed container and for taking a sample of the released pressurized gas for chemical analysis thereof for subsequent use in a modified direct method test which determines the volume of gas and specific type of gas contained within the core sample. The portable tester includes a pair of low and high range electrical pressure transducers for detecting a gas pressure; a pair of low and high range display units for displaying the pressure of the detected gas- a selector valve connected to the low and high range pressure transducers, a selector knob for selecting gas flow to one of the flow paths; control valve having an inlet connection to the sealed container, and outlets connected to: a sample gas canister, a second outlet port connected to the selector valve means for reading the pressure of the gas from the sealed container to either the low range or high range pressure transducers, and a connection for venting gas contained within the sealed container to the atmosphere. A battery is electrically connected to and supplies the power for operating the unit. The pressure transducers, display units, selector and control valve means and the battery is mounted to and housed within a protective casing for portable transport and use.

  4. Prompt Disappearance and Emergence of Radiation Belt Magnetosonic Waves Induced by Solar Wind Dynamic Pressure Variations

    NASA Astrophysics Data System (ADS)

    Liu, Nigang; Su, Zhenpeng; Zheng, Huinan; Wang, Yuming; Wang, Shui

    2018-01-01

    Magnetosonic waves are highly oblique whistler mode emissions transferring energy from the ring current protons to the radiation belt electrons in the inner magnetosphere. Here we present the first report of prompt disappearance and emergence of magnetosonic waves induced by the solar wind dynamic pressure variations. The solar wind dynamic pressure reduction caused the magnetosphere expansion, adiabatically decelerated the ring current protons for the Bernstein mode instability, and produced the prompt disappearance of magnetosonic waves. On the contrary, because of the adiabatic acceleration of the ring current protons by the solar wind dynamic pressure enhancement, magnetosonic waves emerged suddenly. In the absence of impulsive injections of hot protons, magnetosonic waves were observable even only during the time period with the enhanced solar wind dynamic pressure. Our results demonstrate that the solar wind dynamic pressure is an essential parameter for modeling of magnetosonic waves and their effect on the radiation belt electrons.

  5. Cross-sectional relations of arterial stiffness, pressure pulsatility, wave reflection, and arterial calcification.

    PubMed

    Tsao, Connie W; Pencina, Karol M; Massaro, Joseph M; Benjamin, Emelia J; Levy, Daniel; Vasan, Ramachandran S; Hoffmann, Udo; O'Donnell, Christopher J; Mitchell, Gary F

    2014-11-01

    Arterial hemodynamics and vascular calcification are associated with increased risk for cardiovascular disease, but their inter-relations remain unclear. We sought to examine the associations of arterial stiffness, pressure pulsatility, and wave reflection with arterial calcification in individuals free of prevalent cardiovascular disease. Framingham Heart Study Third Generation and Offspring Cohort participants free of cardiovascular disease underwent applanation tonometry to measure arterial stiffness, pressure pulsatility, and wave reflection, including carotid-femoral pulse wave velocity, central pulse pressure, forward wave amplitude, and augmentation index. Participants in each cohort (n=1905, 45±6 years and n=1015, 65±9 years, respectively) underwent multidetector computed tomography to assess the presence and quantity of thoracic aortic calcification, abdominal aortic calcification, and coronary artery calcification. In multivariable-adjusted models, both higher carotid-femoral pulse wave velocity and central pulse pressure were associated with greater thoracic aortic calcification and abdominal aortic calcification, whereas higher augmentation index was associated with abdominal aortic calcification. Among the tonometry measures, carotid-femoral pulse wave velocity was the strongest correlate of all calcification measures in multivariable-adjusted models (odds ratio per SD for thoracic aortic calcification, 2.69 [95% confidence interval, 2.17-3.35]; abdominal aortic calcification, 1.47 [95% confidence interval, 1.26-1.73]; and coronary artery calcification, 1.48 [95% confidence interval, 1.28-1.72]; all P<0.001, respectively). We observed stronger relations of carotid-femoral pulse wave velocity, central pulse pressure, and forward wave amplitude with nearly all continuous calcification measures in the younger Third Generation Cohort as compared with the Offspring Cohort. In community-dwelling individuals without prevalent cardiovascular disease

  6. Study on Pressure Wave Propagation in a Liquid Containing Spherical Bubbles in a Rectangular Duct

    NASA Astrophysics Data System (ADS)

    Kawahara, Junya; Watanabe, Masao; Kobayashi, Kazumichi

    2015-12-01

    Pressure wave propagation in a liquid containing several bubbles is numerically investigated. We simulate liner plane wave propagation in a liquid containing 10 spherical bubbles in a rectangular duct with the equation of motion for N spherical bubbles. The sound pressures of the reflected waves from the rigid walls are calculated by using the method of images. The result shows that the phase velocity of the pressure wave propagating in the liquid containing 10 spherical bubbles in the duct agrees well with the low-frequency speed of sound in a homogeneous bubbly liquid.

  7. Use of a portable, single-use negative pressure wound therapy device in home care patients with low to moderately exuding wounds: a case series.

    PubMed

    Hurd, Theresa; Trueman, Paul; Rossington, Alan

    2014-03-01

    Negative pressure wound therapy (NPWT) is widely used in the management of acute and chronic wounds. The purpose of this 8-week study was to evaluate outcomes of using a new canisterless, portable, single-use NPWT system in patients with wounds treated in a Canadian community healthcare setting. The device is designed to provide negative pressure at 80±20 mm Hg, 24 hours a day of continuous usage, for a maximum wear time of 7 days. Data on wound outcomes, including exudate levels, wound appearance, and wound area, were collected weekly by a Registered Nurse as part of routine practice. When treatment was discontinued, patients and nurses were asked to rate their satisfaction with the device. Data from patients who had used a conventional NPWT device to manage their wounds were retrospectively abstracted from their medical records. In the prospective study, conducted between October 2011 and July 2012, 326 patients (median age=61 years; range 17-91 years) with wounds of mixed etiology (53 pressure ulcers, 21 venous leg ulcers, 16 diabetic foot ulcers, and 15 traumatic and 221 surgical wounds) were treated for a maximum of 8 weeks with the portable NPWT device. The majority of patients (228 out of 326; 68%) achieved complete wound closure within 8 weeks of treatment. The Kaplan-Meier estimate of median time to healing of all wounds was 9 weeks. The majority of patients (318 patients, 97%) reported they were pleased or satisfied with the dressing performance. Nurses indicated satisfaction with the dressing performance for all but two patients (99%). The majority (89%) of patients managed with conventional NPWT (n=539) had an open surgical wound with moderate or high levels of exudate. Healing rates in the portable and conventional NPWT group were similar (10% to 11% per week). Portable, single-use NPWT has the potential to deliver good wound outcomes in community care settings and simplify the use of negative pressure for nurses and patients. Additional research is

  8. Influence of general anaesthesia on slow waves of intracranial pressure.

    PubMed

    Lalou, Despina A; Czosnyka, Marek; Donnelly, Joseph; Lavinio, Andrea; Pickard, John D; Garnett, Matthew; Czosnyka, Zofia

    2016-07-01

    Slow vasogenic intracranial pressure (ICP) waves are spontaneous ICP oscillations with a low frequency bandwidth of 0.3-4 cycles/min (B-waves). B-waves reflect dynamic oscillations in cerebral blood volume associated with autoregulatory cerebral vasodilation and vasoconstriction. This study quantifies the effects of general anaesthesia (GA) on the magnitude of B-waves compared to natural sleep and conscious state. The magnitude of B-waves was assessed in 4 groups of 30 patients each with clinical indications for ICP monitoring. Normal pressure hydrocephalus patients undergoing Cerebrospinal Fluid (CSF) infusion studies in the conscious state (GROUP A) and under GA (GROUP B), and hydrocephalus patients undergoing overnight ICP monitoring during physiological sleep (GROUP C) were compared to deeply sedated traumatic brain injury (TBI) patients with well-controlled ICP during the first night of Intensive Care Unit (ICU) stay (GROUP D). A total of 120 patients were included. During CSF infusion studies, the magnitude of slow waves was higher in conscious patients ( 0.23+/-0.10 mm Hg) when compared to anaesthetised patients ( 0.15+/-0.10 mm Hg; p = 0.011). Overnight magnitude of slow waves was higher in patients during natural sleep (GROUP C: 0.20+/-0.13 mm Hg) when compared to TBI patients under deep sedation (GROUP D: 0.11+/- 0.09 mm Hg; p = 0.002). GA and deep sedation are associated with a reduced magnitude of B-waves. ICP monitoring carried out under GA is affected by iatrogenic suppression of slow vasogenic waves of ICP. Accounting for the effects of anaesthesia on vasogenic waves may prevent the misidentification of potential shunt-responders as non-responders.

  9. Portable Tandem Mass Spectrometer Analyzer

    DTIC Science & Technology

    1991-07-01

    The planned instrument was to be small enough to be portable in small vehicles and was to be able to use either an atmospheric pressure ion source or a...conventional electron impact/chemical ionization ion source. In order to accomplish these developments an atmospheric pressure ionization source was...developed for a compact, commercially available tandem quadrupole mass spectrometer. This ion source could be readily exchanged with the conventional

  10. Pressure measurements of a three wave journal air bearing

    NASA Technical Reports Server (NTRS)

    Dimofte, Florin; Addy, Harold E., Jr.

    1994-01-01

    In order to validate theoretical predictions of a wave journal bearing concept, a bench test rig was assembled at NASA Lewis Research Center to measure the steady-state performance of a journal air bearing. The tester can run up to 30,000 RPM and the spindle has a run out of less than 1 micron. A three wave journal bearing (50 mm diameter and 58 mm length) has been machined at NASA Lewis. The pressures at 16 ports along the bearing circumference at the middle of the bearing length were measured and compared to the theoretical prediction. The bearing ran at speeds up to 15,000 RPM and certain loads. Good agreement was found between the measured and calculated pressures.

  11. Characterization of a Setup to test the Impact of High-Amplitude Pressure Waves on Living Cells

    PubMed Central

    Schmidt, Mischa; Kahlert, Ulf; Wessolleck, Johanna; Maciaczyk, Donata; Merkt, Benjamin; Maciaczyk, Jaroslaw; Osterholz, Jens; Nikkhah, Guido; Steinhauser, Martin O.

    2014-01-01

    The impact of pressure waves on cells may provide several possible applications in biology and medicine including the direct killing of tumors, drug delivery or gene transfection. In this study we characterize the physical properties of mechanical pressure waves generated by a nanosecond laser pulse in a setup with well-defined cell culture conditions. To systematically characterize the system on the relevant length and time scales (micrometers and nanoseconds) we use photon Doppler velocimetry (PDV) and obtain velocity profiles of the cell culture vessel at the passage of the pressure wave. These profiles serve as input for numerical pressure wave simulations that help to further quantify the pressure conditions on the cellular length scale. On the biological level we demonstrate killing of glioblastoma cells and quantify experimentally the pressure threshold for cell destruction. PMID:24458018

  12. Intracranial pressure increases during exposure to a shock wave.

    PubMed

    Leonardi, Alessandra Dal Cengio; Bir, Cynthia A; Ritzel, Dave V; VandeVord, Pamela J

    2011-01-01

    Traumatic brain injuries (TBI) caused by improvised explosive devices (IEDs) affect a significant percentage of surviving soldiers wounded in Iraq and Afghanistan. The extent of a blast TBI, especially initially, is difficult to diagnose, as internal injuries are frequently unrecognized and therefore underestimated, yet problems develop over time. Therefore it is paramount to resolve the physical mechanisms by which critical stresses are inflicted on brain tissue from blast wave encounters with the head. This study recorded direct pressure within the brains of male Sprague-Dawley rats during exposure to blast. The goal was to understand pressure wave dynamics through the brain. In addition, we optimized in vivo methods to ensure accurate measurement of intracranial pressure (ICP). Our results demonstrate that proper sealing techniques lead to a significant increase in ICP values, compared to the outside overpressure generated by the blast. Further, the values seem to have a direct relation to a rat's size and age: heavier, older rats had the highest ICP readings. These findings suggest that a global flexure of the skull by the transient shockwave is an important mechanism of pressure transmission inside the brain.

  13. Are Slow Waves of Intracranial Pressure Suppressed by General Anaesthesia?

    PubMed

    Lalou, Despina Afroditi; Czosnyka, Marek; Donnelly, Joseph; Lavinio, Andrea; Pickard, John D; Garnett, Matthew; Czosnyka, Zofia

    2018-01-01

    Slow waves of intracranial pressure (ICP) are spontaneous oscillations with a frequency of 0.3-4 cycles/min. They are often associated with pathological conditions, following vasomotor activity in the cranial enclosure. This study quantifies the effects of general anaesthesia (GA) on the magnitude of B-waves compared with natural sleep and the conscious state. Four groups of 30 patients each were formed to assess the magnitude of slow waves. Group A and group B consisted of normal pressure hydrocephalus (NPH) patients, each undergoing cerebrospinal fluid (CSF) infusion studies, conscious and under GA respectively. Group C comprised conscious, naturally asleep hydrocephalic patients undergoing overnight ICP monitoring; group D, which included deeply sedated head injury patients monitored in the intensive care unit (ICU), was compared with group C. The average amplitude for group A patients was higher (0.23 ± 0.10 mmHg) than that of group B (0.15 ± 0.10 mmHg; p = 0.01). Overnight magnitude of slow waves was higher in group C (0.20 ± 0.13 mmHg) than in group D (0.11 ± 0.09 mmHg; p = 0.002). Slow waves of ICP are suppressed by GA and deep sedation. When using slow waves in clinical decision-making, it is important to consider the patients' level of consciousness to avoid incorrect therapeutic and management decisions.

  14. Explosion yield estimation from pressure wave template matching

    PubMed Central

    Arrowsmith, Stephen; Bowman, Daniel

    2017-01-01

    A method for estimating the yield of explosions from shock-wave and acoustic-wave measurements is presented. The method exploits full waveforms by comparing pressure measurements against an empirical stack of prior observations using scaling laws. The approach can be applied to measurements across a wide-range of source-to-receiver distances. The method is applied to data from two explosion experiments in different regions, leading to mean relative errors in yield estimates of 0.13 using prior data from the same region, and 0.2 when applied to a new region. PMID:28618805

  15. Portable tester for determining gas content within a core sample

    DOEpatents

    Garcia, F. Jr.; Schatzel, S.J.

    1998-04-21

    A portable tester is provided for reading and displaying the pressure of a gas released from a rock core sample stored within a sealed container and for taking a sample of the released pressurized gas for chemical analysis thereof for subsequent use in a modified direct method test which determines the volume of gas and specific type of gas contained within the core sample. The portable tester includes a pair of low and high range electrical pressure transducers for detecting a gas pressure; a pair of low and high range display units for displaying the pressure of the detected gas; a selector valve connected to the low and high range pressure transducers and a selector knob for selecting gas flow to one of the flow paths; control valve having an inlet connection to the sealed container; and outlets connected to: a sample gas canister, a second outlet port connected to the selector valve means for reading the pressure of the gas from the sealed container to either the low range or high range pressure transducers, and a connection for venting gas contained within the sealed container to the atmosphere. A battery is electrically connected to and supplies the power for operating the unit. The pressure transducers, display units, selector and control valve means and the battery is mounted to and housed within a protective casing for portable transport and use. 5 figs.

  16. A new approximation for pore pressure accumulation in marine sediment due to water waves

    NASA Astrophysics Data System (ADS)

    Jeng, D.-S.; Seymour, B. R.; Li, J.

    2007-01-01

    The residual mechanism of wave-induced pore water pressure accumulation in marine sediments is re-examined. An analytical approximation is derived using a linear relation for pore pressure generation in cyclic loading, and mistakes in previous solutions (Int. J. Numer. Anal. Methods Geomech. 2001; 25:885-907; J. Offshore Mech. Arctic Eng. (ASME) 1989; 111(1):1-11) are corrected. A numerical scheme is then employed to solve the case with a non-linear relation for pore pressure generation. Both analytical and numerical solutions are verified with experimental data (Laboratory and field investigation of wave-sediment interaction. Joseph H. Defrees Hydraulics Laboratory, School of Civil and Environmental Engineering, Cornell University, Ithaca, NY, 1983), and provide a better prediction of pore pressure accumulation than the previous solution (J. Offshore Mech. Arctic Eng. (ASME) 1989; 111(1):1-11). The parametric study concludes that the pore pressure accumulation and use of full non-linear relation of pore pressure become more important under the following conditions: (1) large wave amplitude, (2) longer wave period, (3) shallow water, (4) shallow soil and (5) softer soils with a low consolidation coefficient. Copyright

  17. Modelling and Experimental Verification of Pressure Wave Following Gaseous Helium Storage Tank Rupture

    NASA Astrophysics Data System (ADS)

    Chorowski, M.; Grabowski, M.; Jędrusyna, A.; Wach, J.

    Helium inventory in high energy accelerators, tokamaks and free electron lasers may exceed tens of tons. The gaseous helium is stored in steel tanks under a pressure of about 20 bar and at environment temperature. Accidental rupture of any of the tanks filled with the gaseous helium will create a rapid energy release in form of physical blast. An estimation of pressure wave distribution following the tank rupture and potential consequences to the adjacent research infrastructure and buildings is a very important task, critical in the safety aspect of the whole cryogenic system. According to the present regulations the TNT equivalent approach is to be applied to evaluate the pressure wave following a potential gas storage tank rupture. A special test stand was designed and built in order to verify experimentally the blast effects in controlled conditions. In order to obtain such a shock wave a pressurized plastic tank was used. The tank was ruptured and the resulting pressure wave was recorded using a spatially-distributed array of pressure sensors connected to a high-speed data acquisition device. The results of the experiments and the comparison with theoretical values obtained from thermodynamic model of the blast are presented. A good agreement between the simulated and measured data was obtained. Recommendations regarding the applicability of thermodynamic model of physical blast versus TNT approach, to estimate consequences of gas storage tank rupture are formulated. The laboratory scale experimental results have been scaled to ITER pressurized helium storage tanks.

  18. Relationships between 24-h blood pressure variability and 24-h central arterial pressure, pulse wave velocity and augmentation index in hypertensive patients.

    PubMed

    Omboni, Stefano; Posokhov, Igor N; Rogoza, Anatoly N

    2017-04-01

    Twenty-four-h blood pressure variability (BPV) predicts cardiovascular complications in hypertension, but its association with pulse wave indices (central arterial pressure, pulse wave velocity (PWV) and augmentation index (AIx)) is poorly understood. In the present study, we assessed the degree of the effect of 24-h BPV on 24-h pulse wave indices. Brachial blood pressure was measured non-invasively over the 24 h with an electronic, oscillometric, automated device (BPLab) in 661 uncomplicated treated or untreated hypertensive patients. Digitalized oscillometric waveforms were analyzed with a validated algorithm to obtain pulse wave indices. Twenty-four-h BPV was calculated as the unweighted (SDu) or weighted s.d. (SDw) of the mean blood pressure or as the average real variability (ARV). Twenty-four-h systolic BPV showed a direct and significant relationship with the central arterial systolic pressure (r=0.28 SDu, r=0.40 SDw, r=0.34 ARV), PWV (r=0.10 SDu, r=0.21 SDw, r=0.19 ARV) and AIx (r=0.17 SDu, r=0.27 SDw, r=0.23 ARV). After adjustment for age, sex, body mass index, antihypertensive treatment and 24-h systolic blood pressure, the relationship lost some power but was still significant for all measures, except for the AIx. Pulse wave indices were higher in patients with high BPV than in those with low BPV: after adjustment, these differences were abolished for the AIx. The diastolic BPV showed a weak association with the pulse wave indices. In conclusion, in hypertensive patients, 24-h systolic BPV is moderately and independently associated with 24-h central arterial pressure and stiffness.

  19. Estimation of excitation forces for wave energy converters control using pressure measurements

    NASA Astrophysics Data System (ADS)

    Abdelkhalik, O.; Zou, S.; Robinett, R.; Bacelli, G.; Wilson, D.

    2017-08-01

    Most control algorithms of wave energy converters require prediction of wave elevation or excitation force for a short future horizon, to compute the control in an optimal sense. This paper presents an approach that requires the estimation of the excitation force and its derivatives at present time with no need for prediction. An extended Kalman filter is implemented to estimate the excitation force. The measurements in this approach are selected to be the pressures at discrete points on the buoy surface, in addition to the buoy heave position. The pressures on the buoy surface are more directly related to the excitation force on the buoy as opposed to wave elevation in front of the buoy. These pressure measurements are also more accurate and easier to obtain. A singular arc control is implemented to compute the steady-state control using the estimated excitation force. The estimated excitation force is expressed in the Laplace domain and substituted in the control, before the latter is transformed to the time domain. Numerical simulations are presented for a Bretschneider wave case study.

  20. Portable Planetariums Teach Science

    NASA Technical Reports Server (NTRS)

    2015-01-01

    With the Internet proving to be the wave of the future, in the 1990s Johnson Space Center awarded grants to Rice University in Houston for developing the world's first Internet-accessible museum kiosk. Further grants were awarded to the school for creating educational software for use in homes and schools, leading to the creation of Museums Teaching Planet Earth Inc. The company has gone on to develop and sell portable planetariums and accompanying educational shows.

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

    NASA Astrophysics Data System (ADS)

    Shi, Q.

    2017-12-01

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

  2. Compact portable diffraction moire interferometer

    DOEpatents

    Deason, Vance A.; Ward, Michael B.

    1989-01-01

    A compact and portable moire interferometer used to determine surface deformations of an object. The improved interferometer is comprised of a laser beam, optical and fiber optics devices coupling the beam to one or more evanescent wave splitters, and collimating lenses directing the split beam at one or more specimen gratings. Observation means including film and video cameras may be used to view and record the resultant fringe patterns.

  3. Compact portable diffraction moire interferometer

    DOEpatents

    Deason, V.A.; Ward, M.B.

    1988-05-23

    A compact and portable moire interferometer used to determine surface deformations of an object. The improved interferometer is comprised of a laser beam, optical and fiber optics devices coupling the beam to one or more evanescent wave splitters, and collimating lenses directing the split beam at one or more specimen gratings. Observations means including film and video cameras may be used to view and record the resultant fringe patterns. 7 figs.

  4. Probability Analysis of the Wave-Slamming Pressure Values of the Horizontal Deck with Elastic Support

    NASA Astrophysics Data System (ADS)

    Zuo, Weiguang; Liu, Ming; Fan, Tianhui; Wang, Pengtao

    2018-06-01

    This paper presents the probability distribution of the slamming pressure from an experimental study of regular wave slamming on an elastically supported horizontal deck. The time series of the slamming pressure during the wave impact were first obtained through statistical analyses on experimental data. The exceeding probability distribution of the maximum slamming pressure peak and distribution parameters were analyzed, and the results show that the exceeding probability distribution of the maximum slamming pressure peak accords with the three-parameter Weibull distribution. Furthermore, the range and relationships of the distribution parameters were studied. The sum of the location parameter D and the scale parameter L was approximately equal to 1.0, and the exceeding probability was more than 36.79% when the random peak was equal to the sample average during the wave impact. The variation of the distribution parameters and slamming pressure under different model conditions were comprehensively presented, and the parameter values of the Weibull distribution of wave-slamming pressure peaks were different due to different test models. The parameter values were found to decrease due to the increased stiffness of the elastic support. The damage criterion of the structure model caused by the wave impact was initially discussed, and the structure model was destroyed when the average slamming time was greater than a certain value during the duration of the wave impact. The conclusions of the experimental study were then described.

  5. Design of a Continuous Blood Pressure Measurement System Based on Pulse Wave and ECG Signals.

    PubMed

    Li, Jian-Qiang; Li, Rui; Chen, Zhuang-Zhuang; Deng, Gen-Qiang; Wang, Huihui; Mavromoustakis, Constandinos X; Song, Houbing; Ming, Zhong

    2018-01-01

    With increasingly fierce competition for jobs, the pressures on people have risen in recent years, leading to lifestyle and diet disorders that result in significantly higher risks of cardiovascular disease. Hypertension is one of the common chronic cardiovascular diseases; however, mainstream blood pressure measurement devices are relatively heavy. When multiple measurements are required, the user experience and the measurement results may be unsatisfactory. In this paper, we describe the design of a signal collection module that collects pulse waves and electrocardiograph (ECG) signals. The collected signals are input into a signal processing module to filter the noise and amplify the useful physiological signals. Then, we use a wavelet transform to eliminate baseline drift noise and detect the feature points of the pulse waves and ECG signals. We propose the concept of detecting the wave shape associated with an instance, an approach that minimizes the impact of atypical pulse waves on blood pressure measurements. Finally, we propose an improved method for measuring blood pressure based on pulse wave velocity that improves the accuracy of blood pressure measurements by 58%. Moreover, the results meet the american medical instrument promotion association standards, which demonstrate the feasibility of our measurement system.

  6. Design of a Continuous Blood Pressure Measurement System Based on Pulse Wave and ECG Signals

    PubMed Central

    Li, Jian-Qiang; Li, Rui; Chen, Zhuang-Zhuang; Deng, Gen-Qiang; Wang, Huihui; Mavromoustakis, Constandinos X.; Ming, Zhong

    2018-01-01

    With increasingly fierce competition for jobs, the pressures on people have risen in recent years, leading to lifestyle and diet disorders that result in significantly higher risks of cardiovascular disease. Hypertension is one of the common chronic cardiovascular diseases; however, mainstream blood pressure measurement devices are relatively heavy. When multiple measurements are required, the user experience and the measurement results may be unsatisfactory. In this paper, we describe the design of a signal collection module that collects pulse waves and electrocardiograph (ECG) signals. The collected signals are input into a signal processing module to filter the noise and amplify the useful physiological signals. Then, we use a wavelet transform to eliminate baseline drift noise and detect the feature points of the pulse waves and ECG signals. We propose the concept of detecting the wave shape associated with an instance, an approach that minimizes the impact of atypical pulse waves on blood pressure measurements. Finally, we propose an improved method for measuring blood pressure based on pulse wave velocity that improves the accuracy of blood pressure measurements by 58%. Moreover, the results meet the american medical instrument promotion association standards, which demonstrate the feasibility of our measurement system. PMID:29541556

  7. Preliminary Investigation on the Effects of Shockwaves on Water Samples Using a Portable Semi-Automatic Shocktube

    NASA Astrophysics Data System (ADS)

    Wessley, G. Jims John

    2017-10-01

    The propagation of shock waves through any media results in an instantaneous increase in pressure and temperature behind the shockwave. The scope of utilizing this sudden rise in pressure and temperature in new industrial, biological and commercial areas has been explored and the opportunities are tremendous. This paper presents the design and testing of a portable semi-automatic shock tube on water samples mixed with salt. The preliminary analysis shows encouraging results as the salinity of water samples were reduced up to 5% when bombarded with 250 shocks generated using a pressure ratio of 2. 5. Paper used for normal printing is used as the diaphragm to generate the shocks. The impact of shocks of much higher intensity obtained using different diaphragms will lead to more reduction in the salinity of the sea water, thus leading to production of potable water from saline water, which is the need of the hour.

  8. Two-dimensional global hybrid simulation of pressure evolution and waves in the magnetosheath

    NASA Astrophysics Data System (ADS)

    Lin, Y.; Denton, R. E.; Lee, L. C.; Chao, J. K.

    2001-06-01

    A two-dimensional hybrid simulation is carried out for the global structure of the magnetosheath. Quasi-perpendicular magnetosonic/fast mode waves with large-amplitude in-phase oscillations of the magnetic field and the ion density are seen near the bow shock transition. Alfvén/ion-cyclotron waves are observed along the streamlines in the magnetosheath, and the wave power peaks in the middle magnetosheath. Antiphase oscillations in the magnetic field and density are present away from the shock transition. Transport ratio analysis suggests that these oscillations result from mirror mode waves. Since fluid simulations are currently best able to model the global magnetosphere and the pressure in the magnetosphere is inherently anisotropic (parallel pressure p∥≠perpendicular pressure p⊥), it is of some interest to see if a fluid model can be used to predict the anisotropic pressure evolution of a plasma. Here the predictions of double adiabatic theory, the bounded anisotropy model, and the double polytropic model are tested using the two-dimensional hybrid simulation of the magnetosheath. Inputs to the models from the hybrid simulation are the initial post bow shock pressures and the time-dependent density and magnetic field strength along streamlines of the plasma. The success of the models is evaluated on the basis of how well they predict the subsequent evolution of p∥ and p⊥. The bounded anisotropy model, which encorporates a bound on p⊥/p∥ due to the effect of ion cyclotron pitch angle scattering, does a very good job of predicting the evolution of p⊥ this is evidence that local transfer of energy due to waves is occurring. Further evidence is the positive identification of ion-cyclotron waves in the simulation. The lack of such a good prediction for the evolution of p∥ appears to be due to the model's lack of time dependence for the wave-particle interaction and its neglect of the parallel heat flux. Estimates indicate that these effects will

  9. Portable Hyperbaric Chamber

    NASA Technical Reports Server (NTRS)

    Schneider, William C. (Inventor); Locke, James P. (Inventor); DeLaFuente, Horacio (Inventor)

    2001-01-01

    A portable, collapsible hyperbaric chamber was developed. A toroidal inflatable skeleton provides initial structural support for the chamber, allowing the attendant and/or patient to enter the chamber. Oval hatches mate against bulkhead rings, and the hyperbaric chamber is pressurized. The hatches seal against an o-ring, and the internal pressure of the chamber provides the required pressure against the hatch to maintain an airtight seal. In the preferred embodiment, the hyperbaric chamber has an airlock to allow the attendant to enter and exit the patient chamber during treatment. Visual communication is provided through portholes in the patient and/or airlock chamber. Life monitoring and support systems are in communication with the interior of the hyperbaric chamber and/or airlock chamber through conduits and/or sealed feed-through connectors into the hyperbaric chamber.

  10. Propagation of Pressure Waves, Caused by a Thermal Shock, in Liquid Metals Containing Gas Bubbles

    NASA Astrophysics Data System (ADS)

    Okita, Kohei; Takagi, Shu; Matsumoto, Yoichiro

    The propagation of pressure waves caused by a thermal shock in liquid mercury containing micro gas bubbles has been simulated numerically. In the present study, we clarify the influences of the introduced bubble size and void fraction on the absorption of thermal expansion of liquid mercury and attenuation of pressure waves. The mass, momentum and energy conservation equations for both bubbly mixture and gas inside each bubble are solved, in which the bubble dynamics is represented by the Keller equation. The results show that when the initial void fraction is larger than the rate of the thermal expansion of liquid mercury, the pressure rise caused by the thermal expansion decreases with decreasing the bubble radius, because of the increase of the natural frequency of bubbly mixture. On the other hand, as the bubble radius increases, the peak of pressure waves which propagate at the sound speed of mixture decreases gradually due to the dispersion effect of mixture. When the natural frequency of the mixture with large bubbles is lower than that of the thremal shock, the peak pressure at the wall increases because the pressure waves propagate through the mixture at the sound speed of liquid mercury. The comparison of the results with and without heat transfer through the gas liquid interface shows that the pressure waves are attenuated greatly by the thermal damping effect with the decrease of the void fraction which enhances the nonlinearity of bubble oscillation.

  11. Radiation-pressure-driven dust waves inside bursting interstellar bubbles

    NASA Astrophysics Data System (ADS)

    Ochsendorf, B. B.; Verdolini, S.; Cox, N. L. J.; Berné, O.; Kaper, L.; Tielens, A. G. G. M.

    2014-06-01

    Massive stars drive the evolution of the interstellar medium through their radiative and mechanical energy input. After their birth, they form "bubbles" of hot gas surrounded by a dense shell. Traditionally, the formation of bubbles is explained through the input of a powerful stellar wind, even though direct evidence supporting this scenario is lacking. Here we explore the possibility that interstellar bubbles seen by the Spitzer- and Herschel space telescopes, blown by stars with log (L/L⊙) ≲ 5.2, form and expand because of the thermal pressure that accompanies the ionization of the surrounding gas. We show that density gradients in the natal cloud or a puncture in the swept-up shell lead to an ionized gas flow through the bubble into the general interstellar medium, which is traced by a dust wave near the star, which demonstrates the importance of radiation pressure during this phase. Dust waves provide a natural explanation for the presence of dust inside H II bubbles, offer a novel method to study dust in H II regions and provide direct evidence that bubbles are relieving their pressure into the interstellar medium through a champagne flow, acting as a probe of the radiative interaction of a massive star with its surroundings. We explore a parameter space connecting the ambient density, the ionizing source luminosity, and the position of the dust wave, while using the well studied H II bubbles RCW 120 and RCW 82 as benchmarks of our model. Finally, we briefly examine the implications of our study for the environments of super star clusters formed in ultraluminous infrared galaxies, merging galaxies, and the early Universe, which occur in very luminous and dense environments and where radiation pressure is expected to dominate the dynamical evolution.

  12. Contributions of aortic pulse wave velocity and backward wave pressure to variations in left ventricular mass are independent of each other.

    PubMed

    Bello, Hamza; Norton, Gavin R; Ballim, Imraan; Libhaber, Carlos D; Sareli, Pinhas; Woodiwiss, Angela J

    2017-05-01

    Aortic pulse wave velocity (PWV) and backward waves, as determined from wave separation analysis, predict cardiovascular events beyond brachial blood pressure. However, the extent to which these aortic hemodynamic variables contribute independent of each other is uncertain. In 749 randomly selected participants of African ancestry, we therefore assessed the extent to which relationships between aortic PWV or backward wave pressures (Pb) (and hence central aortic pulse pressure [PPc]) and left ventricular mass index (LVMI) occur independent of each other. Aortic PWV, PPc, forward wave pressure (Pf), and Pb were determined using radial applanation tonometry and SphygmoCor software and LVMI using echocardiography; 44.5% of participants had an increased left ventricular mass indexed to height 1.7 . With adjustments for age, brachial systolic blood pressure or PP, and additional confounders, PPc and Pb, but not Pf, were independently related to LVMI and left ventricular hypertrophy (LVH) in both men and women. However, PWV was independently associated with LVMI in women (partial r = 0.16, P < .001), but not in men (partial r = 0.03), and PWV was independently associated with LVH in women (P < .05), but not in men (P = .07). With PWV and Pb included in the same multivariate regression models, PWV (partial r = 0.14, P < .005) and Pb (partial r = 0.10, P < .05) contributed to a similar extent to variations in LVMI in women. In addition, with PWV and Pb included in the same multivariate regression models, PWV (P < .05) and Pb (P < .02) contributed to LVH in women. In conclusion, aortic PWV and Pb (and hence pulse pressure) although both associated with LVMI and LVH produce effects which are independent of each other. Copyright © 2017 American Society of Hypertension. Published by Elsevier Inc. All rights reserved.

  13. The effects of pressure, temperature, and pore water on velocities in Westerly granite. [for seismic wave propagation

    NASA Technical Reports Server (NTRS)

    Spencer, J. W., Jr.; Nur, A. M.

    1976-01-01

    A description is presented of an experimental assembly which has been developed to conduct concurrent measurements of compressional and shear wave velocities in rocks at high temperatures and confining pressures and with independent control of the pore pressure. The apparatus was used in studies of the joint effects of temperature, external confining pressure, and internal pore water on sonic velocities in Westerly granite. It was found that at a given temperature, confining pressure has a larger accelerating effect on compressional waves in dry rock, whereas at a given confining pressure, temperature has a larger retarding effect on shear waves.

  14. Transient response of a liquid injector to a steep-fronted transverse pressure wave

    NASA Astrophysics Data System (ADS)

    Lim, D.; Heister, S.; Stechmann, D.; Kan, B.

    2017-12-01

    Motivated by the dynamic injection environment posed by unsteady pressure gain combustion processes, an experimental apparatus was developed to visualize the dynamic response of a transparent liquid injector subjected to a single steep-fronted transverse pressure wave. Experiments were conducted at atmospheric pressure with a variety of acrylic injector passage designs using water as the working fluid. High-speed visual observations were made of the injector exit near field, and the extent of backflow and the time to refill the orifice passage were characterized over a range of injection pressures. A companion transient one-dimensional model was developed for interpretation of the results and to elucidate the trends with regard to the strength of the transverse pressure wave. Results from the model were compared with the experimental observations.

  15. Transient response of a liquid injector to a steep-fronted transverse pressure wave

    NASA Astrophysics Data System (ADS)

    Lim, D.; Heister, S.; Stechmann, D.; Kan, B.

    2018-07-01

    Motivated by the dynamic injection environment posed by unsteady pressure gain combustion processes, an experimental apparatus was developed to visualize the dynamic response of a transparent liquid injector subjected to a single steep-fronted transverse pressure wave. Experiments were conducted at atmospheric pressure with a variety of acrylic injector passage designs using water as the working fluid. High-speed visual observations were made of the injector exit near field, and the extent of backflow and the time to refill the orifice passage were characterized over a range of injection pressures. A companion transient one-dimensional model was developed for interpretation of the results and to elucidate the trends with regard to the strength of the transverse pressure wave. Results from the model were compared with the experimental observations.

  16. [Determination of fat, protein and DM in raw milk by portable short-wave near infrared spectrometer].

    PubMed

    Li, Xiao-yun; Wang, Jia-hua; Huang, Ya-wei; Han, Dong-hai

    2011-03-01

    Near infrared diffuse reflectance spectroscopy calibrations of fat, protein and DM in raw milk were studied with partial least-squares (PLS) regression using portable short-wave near infrared spectrometer. The results indicated that good calibrations of fat and DM were found, the correlation coefficients were all 0.98, the RMSEC were 0.187 and 0.217, RMSEP were 0.187 and 0.296, the RPDs were 5.02 and 3.20 respectively; the calibration of protein needed to be improved but can be used for practice, the correlation coefficient was 0.95, RMSEC was 0.105, RMSEP was 0.120, and RPD was 2.60. Furthermore, the measuring accuracy was improved by analyzing the correction relation of fat and DM in raw milk This study will probably provide a new on-site method for nondestructive and rapid measurement of milk.

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

    NASA Astrophysics Data System (ADS)

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

    2017-06-01

    Horizontal and vertical pressure gradients may be important physical mechanisms contributing to onshore sediment transport beneath steep, near-breaking waves in the surf zone. A barred beach was constructed in a large-scale laboratory wave flume with a fixed profile containing a mobile sediment layer on the crest of the sandbar. Horizontal and vertical pore pressure gradients were obtained by finite differences of measurements from an array of pressure transducers buried within the upper several centimeters of the bed. Colocated observations of erosion depth were made during asymmetric wave trials with wave heights between 0.10 and 0.98 m, consistently resulting in onshore sheet flow sediment transport. The pore pressure gradient vector within the bed exhibited temporal rotations during each wave cycle, directed predominantly upward under the trough and then rapidly rotating onshore and downward as the wavefront passed. The magnitude of the pore pressure gradient during each phase of rotation was correlated with local wave steepness and relative depth. Momentary bed failures as deep as 20 grain diameters were coincident with sharp increases in the onshore-directed pore pressure gradients, but occurred at horizontal pressure gradients less than theoretical critical values for initiation of the motion for compact beds. An expression combining the effects of both horizontal and vertical pore pressure gradients with bed shear stress and soil stability is used to determine that failure of the bed is initiated at nonnegligible values of both forces.Plain Language SummaryThe <span class="hlt">pressure</span> gradient present within the seabed beneath breaking <span class="hlt">waves</span> may be an important physical mechanism transporting sediment. A large-scale laboratory was used to replicate realistic surfzone conditions in controlled tests, allowing for horizontal and vertical <span class="hlt">pressure</span> gradient magnitudes and the resulting sediment bed response to be observed with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ShWav..23...25B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ShWav..23...25B"><span>Macro-mechanical modeling of blast-<span class="hlt">wave</span> mitigation in foams. Part II: reliability of <span class="hlt">pressure</span> measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Britan, A.; Liverts, M.; Shapiro, H.; Ben-Dor, G.</p> <p>2013-02-01</p> <p>A phenomenological study of the process occurring when a plane shock <span class="hlt">wave</span> reflected off an aqueous foam column filling the test section of a vertical shock tube has been undertaken. The experiments were conducted with initial shock <span class="hlt">wave</span> Mach numbers in the range 1.25le {M}_s le 1.7 and foam column heights in the range 100-450 mm. Miniature piezotrone circuit electronic <span class="hlt">pressure</span> transducers were used to record the <span class="hlt">pressure</span> histories upstream and alongside the foam column. The aim of these experiments was to find a simple way to eliminate a spatial averaging as an artifact of the <span class="hlt">pressure</span> history recorded by the side-on transducer. For this purpose, we discuss first the common behaviors of the <span class="hlt">pressure</span> traces in extended time scales. These observations evidently quantify the low frequency variations of the <span class="hlt">pressure</span> field within the different flow domains of the shock tube. Thereafter, we focus on the fronts of the <span class="hlt">pressure</span> signals, which, in turn, characterize the high-frequency response of the foam column to the shock <span class="hlt">wave</span> impact. Since the front shape and the amplitude of the <span class="hlt">pressure</span> signal most likely play a significant role in the foam destruction, phase changes and/or other physical factors, such as high capacity, viscosity, etc., the common practice of the data processing is revised and discussed in detail. Generally, side-on <span class="hlt">pressure</span> measurements must be used with great caution when performed in wet aqueous foams, because the low sound speed is especially prone to this effect. Since the spatial averaged recorded <span class="hlt">pressure</span> signals do not reproduce well the real behaviors of the <span class="hlt">pressure</span> rise, the recorded shape of the shock <span class="hlt">wave</span> front in the foam appears much thicker. It is also found that when a thin liquid film wet the sensing membrane, the transducer sensitivity was changed. As a result, the <span class="hlt">pressure</span> recorded in the foam could exceed the real amplitude of the post-shock <span class="hlt">wave</span> flow. A simple procedure, which allows correcting this imperfection, is discussed in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23958590','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23958590"><span>Budget-<span class="hlt">makers</span> and health care systems.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>White, Joseph</p> <p>2013-10-01</p> <p>Health programs are shaped by the decisions made in budget processes, so how budget-<span class="hlt">makers</span> view health programs is an important part of making health policy. Budgeting in any country involves its own policy community, with key players including budgeting professionals and political authorities. This article reviews the typical <span class="hlt">pressures</span> on and attitudes of these actors when they address health policy choices. The worldview of budget professionals includes attitudes that are congenial to particular policy perspectives, such as the desire to select packages of programs that maximize population health. The <span class="hlt">pressures</span> on political authorities, however, are very different: most importantly, public demand for health care services is stronger than for virtually any other government activity. The norms and procedures of budgeting also tend to discourage adoption of some of the more enthusiastically promoted health policy reforms. Therefore talk about rationalizing systems is not matched by action; and action is better explained by the need to minimize blame. The budget-<span class="hlt">maker</span>'s perspective provides insight about key controversies in healthcare policy such as decentralization, competition, health service systems as opposed to health insurance systems, and dedicated vs. general revenue finance. It also explains the frequency of various "gaming" behaviors. Copyright © 2013 Elsevier Ireland Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004ASAJ..116..417A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004ASAJ..116..417A"><span>Prediction of the characteristics of two types of <span class="hlt">pressure</span> <span class="hlt">waves</span> in the cochlea: Theoretical considerations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Andoh, Masayoshi; Wada, Hiroshi</p> <p>2004-07-01</p> <p>The aim of this study was to predict the characteristics of two types of cochlear <span class="hlt">pressure</span> <span class="hlt">waves</span>, so-called fast and slow <span class="hlt">waves</span>. A two-dimensional finite-element model of the organ of Corti (OC), including fluid-structure interaction with the surrounding lymph fluid, was constructed. The geometry of the OC at the basal turn was determined from morphological measurements of others in the gerbil hemicochlea. As far as mechanical properties of the materials within the OC are concerned, previously determined mechanical properties of portions within the OC were adopted, and unknown mechanical features were determined from the published measurements of static stiffness. Time advance of the fluid-structure scheme was achieved by a staggered approach. Using the model, the magnitude and phase of the fast and slow <span class="hlt">waves</span> were predicted so as to fit the numerically obtained <span class="hlt">pressure</span> distribution in the scala tympani with what is known about intracochlear <span class="hlt">pressure</span> measurement. When the predicted <span class="hlt">pressure</span> <span class="hlt">waves</span> were applied to the model, the numerical result of the velocity of the basilar membrane showed good agreement with the experimentally obtained velocity of the basilar membrane documented by others. Thus, the predicted <span class="hlt">pressure</span> <span class="hlt">waves</span> appeared to be reliable. Moreover, it was found that the fluid-structure interaction considerably influences the dynamic behavior of the OC at frequencies near the characteristic frequency.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li class="active"><span>6</span></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_6 --> <div id="page_7" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="121"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950015988','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950015988"><span><span class="hlt">Wave</span> Journal Bearing. Part 2: Experimental <span class="hlt">Pressure</span> Measurements and Fractional Frequency Whirl Threshold for <span class="hlt">Wave</span> and Plain Journal Bearings</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Walker, James F.; Dimofte, Florin; Addy, Harold E., Jr.</p> <p>1995-01-01</p> <p>A new hydrodynamic bearing concept, the <span class="hlt">wave</span> journal bearing, is being developed because it has better stability characteristics than plain journal bearings while maintaining similar load capacity. An analysis code to predict the steady state and dynamic performance of the <span class="hlt">wave</span> journal bearing is also part of the development. To verify numerical predictions and contrast the <span class="hlt">wave</span> journal bearing's stability characteristics to a plain journal bearing, tests were conducted at NASA Lewis Research Center using an air bearing test rig. Bearing film <span class="hlt">pressures</span> were measured at 16 ports located around the bearing circumference at the middle of the bearing length. The <span class="hlt">pressure</span> measurements for both a plain journal bearing and a <span class="hlt">wave</span> journal bearing compared favorably with numerical predictions. Both bearings were tested with no radial load to determine the speed threshold for self-excited fractional frequency whirl. The plain journal bearing started to whirl immediately upon shaft start-up. The <span class="hlt">wave</span> journal did not incur self-excited whirl until 800 to 900 rpm as predicted by the analysis. Furthermore, the <span class="hlt">wave</span> bearing's geometry limited the whirl orbit to less than the bearing's clearance. In contrast, the plain journal bearing did not limit the whirl orbit, causing it to rub.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002AGUFMMR72B1045M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002AGUFMMR72B1045M"><span>Elastic <span class="hlt">Wave</span> Velocity Measurements on Mantle Peridotite at High <span class="hlt">Pressure</span> and Temperature</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mistler, G. W.; Ishikawa, M.; Li, B.</p> <p>2002-12-01</p> <p>With the success of conducting ultrasonic measurements at high <span class="hlt">pressure</span> and high temperature in large volume high <span class="hlt">pressure</span> apparatus with in-situ measurement of the sample length by X-ray imaging, it is now possible to measure elastic <span class="hlt">wave</span> velocities on aggregate samples with candidate compositions of the mantle to the conditions of the Earth's transition zone in the laboratory. These data can be directly compared with seismic data to distinguish the compositional models in debate. In this work, we carried out velocity measurements on natural peridotite KLB-1 at the conditions of the Earth's upper mantle. Fine powered sample of natural KLB-1 was used as starting material. Specimens for ultrasonic measurements were hot-pressed and equilibrated at various <span class="hlt">pressure</span> and temperature conditions along geotherm up to the transition zone. The recovered samples were characterized with density measurement, X-ray diffraction and microprobe analysis. Bench top P and S <span class="hlt">wave</span> velocities of KLB-1 sample sintered at 3-4 GPa and 1400 degree centigrade showed a very good agreement with the VRH average of pyrolite. High <span class="hlt">pressure</span> and high temperature measurements was conducted up to 7 GPa and 800 degree centigrade using ultrasonic interferometric method in a DIA-type high <span class="hlt">pressure</span> apparatus in conjunction with X-ray diffraction and X-ray imaging. The utilization of X-ray imaging technique provides direct measurements of sample lengths at high <span class="hlt">pressure</span> and high temperature, ensuring a precise determination of velocities. The results of P and S <span class="hlt">wave</span> velocities at high <span class="hlt">pressure</span> and high temperature as well as their comparison with calculated pyrolite model will be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMNH51C..07L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMNH51C..07L"><span>Inverting Coseismic TEC Disturbances for Neutral Atmosphere <span class="hlt">Pressure</span> <span class="hlt">Wave</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, R. F.; Mikesell, D.; Rolland, L.</p> <p>2017-12-01</p> <p>Research from the past 20 years has shown that we can detect coseismic disturbances in the total electron content (TEC) using global navigation space systems (GNSS). In the near field, TEC disturbances are created by the direct <span class="hlt">wave</span> from rupture on the surface. This <span class="hlt">pressure</span> <span class="hlt">wave</span> travels through the neutral atmosphere to the ionosphere within about 10 minutes. This provides the opportunity to almost immediately characterize the source of the acoustic disturbance on the surface using methods from seismology. In populated areas, this could provide valuable information to first responders. To retrieve the surface motion amplitude information we must account for changes in the waveform caused by the geomagnetic field, motion of the satellites and the geometry of the satellites and receivers. One method is to use a transfer function to invert for the neutral atmosphere <span class="hlt">pressure</span> <span class="hlt">wave</span>. Gómez et al (2015) first employed an analytical model to invert for acoustic <span class="hlt">waves</span> produced by Rayleigh <span class="hlt">waves</span> propagating along the Earth's surface. Here, we examine the same model in the near field using the TEC disturbances from the direct <span class="hlt">wave</span> produced by rupture at the surface. We compare results from the forward model against a numerical model that has been shown to be in good agreement with observations from the 2011 Van (Turkey) earthquake. We show the forward model predictions using both methods for the Van earthquake. We then analyze results for hypothetical events at different latitudes and discuss the reliability of the analytical model in each scenario. Gómez, D., R. Jr. Smalley, C. A. Langston, T. J. Wilson, M. Bevis, I. W. D. Dalziel, E. C. Kendrick, S. A. Konfal, M. J. Willis, D. A. Piñón, et al. (2015), Virtual array beamforming of GPS TEC observations of coseismic ionospheric disturbances near the Geomagnetic South Pole triggered by teleseismic megathrusts, J. Geophys. Res. Space Physics, 120, 9087-9101, doi:10.1002/2015JA021725.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6278791-quantification-abnormal-intracranial-pressure-waves-isotope-cisternography-diagnosis-occult-communicating-hydrocephalus','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6278791-quantification-abnormal-intracranial-pressure-waves-isotope-cisternography-diagnosis-occult-communicating-hydrocephalus"><span>Quantification of abnormal intracranial <span class="hlt">pressure</span> <span class="hlt">waves</span> and isotope cisternography for diagnosis of occult communicating hydrocephalus</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>Cardoso, E.R.; Piatek, D.; Del Bigio, M.R.</p> <p>1989-01-01</p> <p>Nineteen consecutive patients with suspected occult communicating hydrocephalus were investigated by means of clinical evaluation, neuropsychological testing, isotope cisternography, computed tomography scanning, and continuous intracranial <span class="hlt">pressure</span> monitoring. Semi-quantitative grading systems were used in the evaluation of the clinical, neuropsychological, and cisternographic assessments. Clinical examination, neuropsychological testing, and computed tomography scanning were repeated 3 months after ventriculoperitoneal shunting. All patients showed abnormal intracranial <span class="hlt">pressure</span> <span class="hlt">waves</span> and all improved after shunting. There was close correlation between number, peak, and pulse <span class="hlt">pressures</span> of B <span class="hlt">waves</span> and the mean intracranial <span class="hlt">pressure</span>. However, quantification of B <span class="hlt">waves</span> by means of number, frequency, and amplitude didmore » not help in predicting the degree of clinical improvement postshunting. The most sensitive predictor of favorable response to shunting was enlargement of the temporal horns on computed tomography scan. Furthermore, the size of temporal horns correlated with mean intracranial <span class="hlt">pressure</span>. There was no correlation between abnormalities on isotope cisternography and clinical improvement.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20050000433&hterms=artificial+heart&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dartificial%2Bheart','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20050000433&hterms=artificial+heart&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dartificial%2Bheart"><span>Development of a piezopolymer <span class="hlt">pressure</span> sensor for a <span class="hlt">portable</span> fetal heart rate monitor</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zuckerwar, A. J.; Pretlow, R. A.; Stoughton, J. W.; Baker, D. A.</p> <p>1993-01-01</p> <p>A piezopolymer <span class="hlt">pressure</span> sensor has been developed for service in a <span class="hlt">portable</span> fetal heart rate monitor, which will permit an expectant mother to perform the fetal nonstress test, a standard predelivery test, in her home. Several sensors are mounted in an array on a belt worn by the mother. The sensor design conforms to the distinctive features of the fetal heart tone, namely, the acoustic signature, frequency spectrum, signal amplitude, and localization. The components of a sensor serve to fulfill five functions: signal detection, acceleration cancellation, acoustical isolation, electrical shielding, and electrical isolation of the mother. A theoretical analysis of the sensor response yields a numerical value for the sensor sensitivity, which is compared to experiment in an in vitro sensor calibration. Finally, an in vivo test on patients within the last six weeks of term reveals that nonstress test recordings from the acoustic monitor compare well with those obtained from conventional ultrasound.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/869249','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/869249"><span><span class="hlt">Portable</span> high precision <span class="hlt">pressure</span> transducer system</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Piper, Thomas C.; Morgan, John P.; Marchant, Norman J.; Bolton, Steven M.</p> <p>1994-01-01</p> <p>A high precision <span class="hlt">pressure</span> transducer system for checking the reliability of a second <span class="hlt">pressure</span> transducer system used to monitor the level of a fluid confined in a holding tank. Since the response of the <span class="hlt">pressure</span> transducer is temperature sensitive, it is continually housed in an battery powered oven which is configured to provide a temperature stable environment at specified temperature for an extended period of time. Further, a high precision temperature stabilized oscillator and counter are coupled to a single board computer to accurately determine the <span class="hlt">pressure</span> transducer oscillation frequency and convert it to an applied <span class="hlt">pressure</span>. All of the components are powered by the batteries which during periods of availability of line power are charged by an on board battery charger. The <span class="hlt">pressure</span> readings outputs are transmitted to a line printer and a vacuum florescent display.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5033709','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/5033709"><span><span class="hlt">Portable</span> high precision <span class="hlt">pressure</span> transducer system</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Piper, T.C.; Morgan, J.P.; Marchant, N.J.; Bolton, S.M.</p> <p>1994-04-26</p> <p>A high precision <span class="hlt">pressure</span> transducer system is described for checking the reliability of a second <span class="hlt">pressure</span> transducer system used to monitor the level of a fluid confined in a holding tank. Since the response of the <span class="hlt">pressure</span> transducer is temperature sensitive, it is continually housed in an battery powered oven which is configured to provide a temperature stable environment at specified temperature for an extended period of time. Further, a high precision temperature stabilized oscillator and counter are coupled to a single board computer to accurately determine the <span class="hlt">pressure</span> transducer oscillation frequency and convert it to an applied <span class="hlt">pressure</span>. All of the components are powered by the batteries which during periods of availability of line power are charged by an on board battery charger. The <span class="hlt">pressure</span> readings outputs are transmitted to a line printer and a vacuum fluorescent display. 2 figures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22264111-comparison-actinide-production-traveling-wave-pressurized-water-reactors','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22264111-comparison-actinide-production-traveling-wave-pressurized-water-reactors"><span>Comparison of actinide production in traveling <span class="hlt">wave</span> and <span class="hlt">pressurized</span> water reactors</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>Osborne, A.G.; Smith, T.A.; Deinert, M.R.</p> <p></p> <p>The geopolitical problems associated with civilian nuclear energy production arise in part from the accumulation of transuranics in spent nuclear fuel. A traveling <span class="hlt">wave</span> reactor is a type of breed-burn reactor that could, if feasible, reduce the overall production of transuranics. In one possible configuration, a cylinder of natural or depleted uranium would be subjected to a fast neutron flux at one end. The neutrons would transmute the uranium, producing plutonium and higher actinides. Under the right conditions, the reactor could become critical, at which point a self-stabilizing fission <span class="hlt">wave</span> would form and propagate down the length of the reactormore » cylinder. The neutrons from the fission <span class="hlt">wave</span> would burn the fissile nuclides and transmute uranium ahead of the <span class="hlt">wave</span> to produce additional fuel. Fission <span class="hlt">waves</span> in uranium are driven largely by the production and fission of {sup 239}Pu. Simulations have shown that the fuel burnup can reach values greater than 400 MWd/kgIHM, before fission products poison the reaction. In this work we compare the production of plutonium and minor actinides produced in a fission <span class="hlt">wave</span> to that of a UOX fueled light water reactor, both on an energy normalized basis. The nuclide concentrations in the spent traveling <span class="hlt">wave</span> reactor fuel are computed using a one-group diffusion model and are verified using Monte Carlo simulations. In the case of the <span class="hlt">pressurized</span> water reactor, a multi-group collision probability model is used to generate the nuclide quantities. We find that the traveling <span class="hlt">wave</span> reactor produces about 0.187 g/MWd/kgIHM of transuranics compared to 0.413 g/MWd/kgIHM for a <span class="hlt">pressurized</span> water reactor running fuel enriched to 4.95 % and burned to 50 MWd/kgIHM. (authors)« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/875298','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/875298"><span><span class="hlt">Portable</span> wastewater flow meter</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Hunter, Robert M.</p> <p>1999-02-02</p> <p>A <span class="hlt">portable</span> wastewater flow meter particularly adapted for temporary use at a single location in measuring the rate of liquid flow in a circular entrance conduit of a sewer manhole both under free flow and submerged, open channel conditions and under fill pipe, surcharged conditions, comprising an apparatus having a cylindrical external surface and an inner surface that constricts the flow through the apparatus in such a manner that a relationship exists between (1) the difference between the static <span class="hlt">pressure</span> head of liquid flowing through the entrance of the apparatus and the static <span class="hlt">pressure</span> head of liquid flowing through the constriction, and (2) the rate of liquid flow through the apparatus.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/867254','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/867254"><span><span class="hlt">Portable</span> wastewater flow meter</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Hunter, Robert M.</p> <p>1990-01-01</p> <p>A <span class="hlt">portable</span> wastewater flow meter particularly adapted for temporary use at a single location in measuring the rate of liquid flow in a circular entrance conduit of a sewer manhole both under free flow and submerged, open channel conditions and under full pipe, surcharged conditions, comprising an apparatus having a cylindrical external surface and an inner surface that constricts the flow through the apparatus in such a manner that a relationship exists between (1) the difference between the static <span class="hlt">pressure</span> head of liquid flowing through the entrance of the apparatus and the static <span class="hlt">pressure</span> head of liquid flowing through the constriction, and (2) the rate of liquid flow through the apparatus.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18812829','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18812829"><span><span class="hlt">Portable</span> monitoring for the diagnosis of obstructive sleep apnea.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Collop, Nancy A</p> <p>2008-11-01</p> <p>The demand for expedient diagnosis of suspected obstructive sleep apnea (OSA) has increased due to improved awareness of sleep disorders. Polysomnography (PSG) is the current preferred diagnostic modality but is relatively inconvenient, expensive and inefficient. <span class="hlt">Portable</span> monitoring has been developed and is widely used in countries outside the United States as an alternative approach. A <span class="hlt">portable</span> monitor records fewer physiologic variables but is typically unattended and can be performed in the home. Numerous <span class="hlt">portable</span> monitor studies have been performed over the past two to three decades. The US government and medical societies have extensively reviewed this literature several times in an attempt to determine if <span class="hlt">portable</span> monitoring should be more broadly used for diagnosing OSA. In March 2008, the US Centers for Medicare and Medicaid Services released a statement allowing the use of <span class="hlt">portable</span> monitoring to diagnose OSA and prescribe continuous positive airway <span class="hlt">pressure</span>. This has potentially opened the door for more widespread use of these devices. This review will focus on the literature that has examined <span class="hlt">portable</span> monitoring as a diagnostic tool for OSA. It is anticipated that <span class="hlt">portable</span> monitoring as a diagnostic modality for OSA will be used more frequently in the United States following the Centers for Medicare and Medicaid Services ruling. Physicians and others considering the use of <span class="hlt">portable</span> monitors should thoroughly understand the advantages and limitations of this technology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820009988','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820009988"><span><span class="hlt">Portable</span> medical status and treatment system</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1981-01-01</p> <p>A <span class="hlt">portable</span> medical status and treatment system is discussed. The vital signs monitor includes electrocardiogram, respiration, temperature, blood <span class="hlt">pressure</span>, alarm, and power subsystems, which are described. A DC defibrillator module, a radio module, and their packaging are also described. These subsystems were evaluated and the results and recommendations are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011JFS....27..311H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011JFS....27..311H"><span>A review of <span class="hlt">wave</span> celerity in frictionless and axisymmetrical steel-lined <span class="hlt">pressure</span> tunnels</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hachem, F. E.; Schleiss, A. J.</p> <p>2011-02-01</p> <p>Generally applicable approaches for estimating the “quasi-static”, which means without fluid-structure interaction and frequency-dependent water-hammer <span class="hlt">wave</span> speed in steel-lined <span class="hlt">pressure</span> tunnels are analyzed. The external constraints and assumptions of these approaches are discussed in detail. The reformulated formulas are then compared to commonly used expressions. Some special cases of <span class="hlt">wave</span> speed calculation such as unlined <span class="hlt">pressure</span> tunnels and open-air penstocks are investigated. The quasi-static <span class="hlt">wave</span> speed is significantly influenced by the state of the backfill concrete and the near-field rock zone (cracked or uncracked). In the case when these two layers are cracked, the quasi-static <span class="hlt">wave</span> speed is overestimated in between 1% and 8% compared to uncracked concrete and near-field rock layers. Depending on the stiffness of steel liner and penstock, the fluid-structure interaction leads to significant difference in <span class="hlt">wave</span> speeds values. Compared to the quasi-static case, the fluid-structure interaction approach, applied to steel-lined tunnels, results up to 13% higher <span class="hlt">wave</span> speed values in the high-frequency range (higher than 600 Hz) and up to 150% lower values for frequencies between 150 and 300 Hz in the considered test case.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUFMMR31A0138K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUFMMR31A0138K"><span>New Experimental Setup for High-<span class="hlt">Pressure</span> High-Temperature Gigahertz Ultrasonic Interferometry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kantor, A. P.; Kantor, I. Y.; Dubrovinsky, L. S.; Jacobsen, S. D.</p> <p>2005-12-01</p> <p>The only direct information about Earth's interior comes from seismological observations of sound <span class="hlt">wave</span> velocities. In order to create compositional and mineralogical model from seismological data knowledge of the elastic properties and crystal chemistry of minerals is necessary. Gigahertz ultrasonic interferometry (GUI) is a relatively new tool used to measure single-crystal compressional and shear-<span class="hlt">wave</span> travel times, which are converted to sound velocities and elastic moduli for direct application to problems in geophysics. Although possibility of simultaneous high-<span class="hlt">pressure</span> and high-temperature GUI measurements in diamond anvil cell was demonstrated before up to temperature of 250°C, in situ <span class="hlt">pressure</span> measurements were not possible. We developed new experimental setup for simultaneous GUI and <span class="hlt">pressure</span> determination using a ruby fluorescence gouge. A diamond anvil cell is equipped with a miniature internal resistive heater with thermocouple fixed at a very small distance from the sample chamber. DAC is mounted at the rotating stage with 5 degrees of freedom (XYZ and two tilting degrees), that can be fixed in three different positions: on top of a P-buffer rod for compressional <span class="hlt">wave</span> velocities measurement, on top of S-buffer rod for shear <span class="hlt">wave</span> velocities measurement and under the microscope, equipped with laser and <span class="hlt">portable</span> high-resolution spectrometer for ruby fluorescence measurement. DAC under high temperature could be moved between these three positions, and independent <span class="hlt">pressure</span>, temperature, S and P <span class="hlt">wave</span> velocities measurements could be done simultaneously at each data point. In addition to single-crystal elasticity measurements, ability of GUI for elasticity measurements of liquids was demonstrated. Compressional <span class="hlt">wave</span> velocities in liquid argon were measured at high <span class="hlt">pressures</span> and temperatures, showing the ability of GUI for studies equation of state of a liquid.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25384042','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25384042"><span>Effects of blood <span class="hlt">pressure</span> and sex on the change of <span class="hlt">wave</span> reflection: evidence from Gaussian fitting method for radial artery <span class="hlt">pressure</span> waveform.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Chengyu; Zhao, Lina; Liu, Changchun</p> <p>2014-01-01</p> <p>An early return of the reflected component in the arterial pulse has been recognized as an important indicator of cardiovascular risk. This study aimed to determine the effects of blood <span class="hlt">pressure</span> and sex factor on the change of <span class="hlt">wave</span> reflection using Gaussian fitting method. One hundred and ninety subjects were enrolled. They were classified into four blood <span class="hlt">pressure</span> categories based on the systolic blood <span class="hlt">pressures</span> (i.e., ≤ 110, 111-120, 121-130 and ≥ 131 mmHg). Each blood <span class="hlt">pressure</span> category was also stratified for sex factor. Electrocardiogram (ECG) and radial artery <span class="hlt">pressure</span> waveforms (RAPW) signals were recorded for each subject. Ten consecutive pulse episodes from the RAPW signal were extracted and normalized. Each normalized pulse episode was fitted by three Gaussian functions. Both the peak position and peak height of the first and second Gaussian functions, as well as the peak position interval and peak height ratio, were used as the evaluation indices of <span class="hlt">wave</span> reflection. Two-way ANOVA results showed that with the increased blood <span class="hlt">pressure</span>, the peak position of the second Gaussian significantly shorten (P < 0.01), the peak height of the first Gaussian significantly decreased (P < 0.01) and the peak height of the second Gaussian significantly increased (P < 0.01), inducing the significantly decreased peak position interval and significantly increased peak height ratio (both P < 0.01). Sex factor had no significant effect on all evaluation indices (all P > 0.05). Moreover, the interaction between sex and blood <span class="hlt">pressure</span> factors also had no significant effect on all evaluation indices (all P > 0.05). These results showed that blood <span class="hlt">pressure</span> has significant effect on the change of <span class="hlt">wave</span> reflection when using the recently developed Gaussian fitting method, whereas sex has no significant effect. The results also suggested that the Gaussian fitting method could be used as a new approach for assessing the arterial <span class="hlt">wave</span> reflection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24216739','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24216739"><span>Characterization of laser-driven shock <span class="hlt">waves</span> in solids using a fiber optic <span class="hlt">pressure</span> probe.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cranch, Geoffrey A; Lunsford, Robert; Grün, Jacob; Weaver, James; Compton, Steve; May, Mark; Kostinski, Natalie</p> <p>2013-11-10</p> <p>Measurement of laser-driven shock <span class="hlt">wave</span> <span class="hlt">pressure</span> in solid blocks of polymethyl methacrylate is demonstrated using fiber optic <span class="hlt">pressure</span> probes. Three probes based on a fiber Fabry-Perot, fiber Bragg grating, and interferometric fiber tip sensor are tested and compared. Shock <span class="hlt">waves</span> are generated using a high-power laser focused onto a thin foil target placed in close proximity to the test blocks. The fiber Fabry-Perot sensor appears capable of resolving the shock front with a rise time of 91 ns. The peak <span class="hlt">pressure</span> is estimated, using a separate shadowgraphy measurement, to be 3.4 GPa.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1240062-characterization-laser-driven-shock-waves-solids-using-fiber-optic-pressure-probe','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1240062-characterization-laser-driven-shock-waves-solids-using-fiber-optic-pressure-probe"><span>Characterization of laser-driven shock <span class="hlt">waves</span> in solids using a fiber optic <span class="hlt">pressure</span> probe</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Cranch, Geoffrey A.; Lunsford, Robert; Grun, Jacob; ...</p> <p>2013-11-08</p> <p>Measurement of laser-driven shock <span class="hlt">wave</span> <span class="hlt">pressure</span> in solid blocks of polymethyl methacrylate is demonstrated using fiber optic <span class="hlt">pressure</span> probes. Three probes based on a fiber Fabry–Perot, fiber Bragg grating, and interferometric fiber tip sensor are tested and compared. Shock <span class="hlt">waves</span> are generated using a high-power laser focused onto a thin foil target placed in close proximity to the test blocks. The fiber Fabry–Perot sensor appears capable of resolving the shock front with a rise time of 91 ns. As a result, the peak <span class="hlt">pressure</span> is estimated, using a separate shadowgraphy measurement, to be 3.4 GPa.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18221105','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18221105"><span>Role of infrasound <span class="hlt">pressure</span> <span class="hlt">waves</span> in atherosclerotic plaque rupture: a theoretical approach.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tsatsaris, Athanasios; Koukounaris, Efstathios; Motsakos, Theodoros; Perrea, Despina</p> <p>2007-01-01</p> <p>To investigate the role of infrasound aortic <span class="hlt">pressure</span> <span class="hlt">waves</span> (IPW) in atherosclerotic plaque rupture. Atherosclerotic plaques have been simulated partly, in two dimensions, as being short or long Conical Intersections (CIS), that is to say elliptic, parabolic or hyperbolic surfaces. Consequently, the course and reflection of the generated aortic <span class="hlt">pressure</span> <span class="hlt">wave</span> (infrasound domain-less than 20Hz) has been examined around the simulated plaques. The incidence of IPW on plaque surface results both in reflection and "refraction" of the <span class="hlt">wave</span>. The IPW course within tissue, seems to be enhanced by high Cu-level presence at these areas according to recent evidence (US2003000388213). The "refracted", derived <span class="hlt">wave</span> travels through plaque tissue and is eventually accumulated to the foci of the respective CIS-plaque geometry. The foci location within or underneath atheroma declares zones where infrasound energy is mostly absorbed. This process, among other mechanisms may contribute to plaque rupture through the development of local hemorrhage and inflammation in foci areas. In future, detection of foci areas and repair (i.e. via Laser Healing Microtechnique) may attenuate atherosclerotic plaque rupture behavior.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title49-vol3/pdf/CFR-2013-title49-vol3-sec178-255-12.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title49-vol3/pdf/CFR-2013-title49-vol3-sec178-255-12.pdf"><span>49 CFR 178.255-12 - <span class="hlt">Pressure</span> test.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... 49 Transportation 3 2013-10-01 2013-10-01 false <span class="hlt">Pressure</span> test. 178.255-12 Section 178.255-12... <span class="hlt">Portable</span> Tanks § 178.255-12 <span class="hlt">Pressure</span> test. (a) Each completed <span class="hlt">portable</span> tank prior to application of lining... the test, and applying a <span class="hlt">pressure</span> of 60 psig. The tank shall be capable of holding the prescribed...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22287201','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22287201"><span><span class="hlt">Pressure-wave</span> energy relationship during IABP counterpulsation in a mock circulation: changes with angle and assisting frequency.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Biglino, Giovanni; Kolyva, Christina; Khir, Ashraf W</p> <p>2012-01-01</p> <p>Despite decades of successful clinical use of the intra aortic balloon pump (IABP), certain aspects of its operation are not yet fully understood. This work aims to investigate in vitro the mechanism underlying balloon inflation and deflation with varying assisting frequency and operating angle with respect to the horizontal, by studying the corresponding <span class="hlt">pressure</span> and <span class="hlt">wave</span> energy changes. A mock circulatory system (MCS), with physiological distribution of peripheral resistance and compliance, presented a controllable test bed. We used <span class="hlt">Wave</span> Intensity Analysis (WIA) to identify balloon-generated <span class="hlt">waves</span> and quantify their energy. Conventional hemodynamic parameters were also calculated. Tests were repeated at varying operating angles (0°-45°), resembling the semi-recumbent position in the ICU, and at different assisting frequencies (1:1, 1:2, 1:3). Two balloons (25 cc and 40 cc in volume) were tested. The main <span class="hlt">waves</span> associated with counterpulsation were identified as a backward compression <span class="hlt">wave</span> associated with balloon inflation and a backward expansion <span class="hlt">wave</span> associated with balloon deflation. Results showed that the IABP inflation and deflation benefits are reduced with increasing angle, in terms of the size of the inflation and deflation <span class="hlt">waves</span> as well as in terms of diastolic <span class="hlt">pressure</span> augmentation and end-diastolic <span class="hlt">pressure</span> reduction. Both WIA findings and <span class="hlt">pressure</span> parameters indicated 1:1 as the most effective mode of pumping. This study shows that, in vitro, a greater benefit of counterpulsation can be achieved in the horizontal position at 1:1 assisting frequency, with a good correlation between <span class="hlt">wave</span> and <span class="hlt">pressure</span> results.</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('http://hdl.handle.net/2060/19800002736','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19800002736"><span>Propagation of <span class="hlt">waves</span> in a medium with high 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>Bisnovatyy-Kogan, G. S.; Blinnikov, S. I.</p> <p>1979-01-01</p> <p>The propagation and mutual transformation of acoustic and thermal <span class="hlt">waves</span> are investigated in media with a high radiative <span class="hlt">pressure</span>. The equations of hydrodynamics for matter and the radiative transfer equations in a moving medium in the Eddington approximation are used in the investigation. Model problems of <span class="hlt">waves</span> in a homogeneous medium with an abrupt jump in opacity and in a medium of variable opacity are presented. The characteristic and the times of variability are discussed. Amplitude for the brightness fluctuations for very massive stars are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730001594','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730001594"><span>Finite-amplitude <span class="hlt">pressure</span> <span class="hlt">waves</span> in the radial mode of a cylinder</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kubo, I.; Moore, F. K.</p> <p>1972-01-01</p> <p>A numerical study of finite-strength, isentropic <span class="hlt">pressure</span> <span class="hlt">waves</span> transverse to the axis of a circular cylinder was made for the radial resonant mode. The <span class="hlt">waves</span> occur in a gas otherwise at rest, filling the cylinder. A method of characteristics was used for the numerical solution. For small but finite amplitudes, calculations indicate the existence of <span class="hlt">waves</span> of permanent potential form. For larger amplitudes, a shock is indicated to occur. The critical value of the initial amplitude parameter in the power series is found to be 0.06 to 0.08, under various types of initial conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040182404','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040182404"><span>Numerical Investigations of High <span class="hlt">Pressure</span> Acoustic <span class="hlt">Waves</span> in Resonators</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Athavale, Mahesh; Pindera, Maciej; Daniels, Christopher C.; Steinetz, Bruce M.</p> <p>2004-01-01</p> <p>This presentation presents work on numerical investigations of nonlinear acoustic phenomena in resonators that can generate high-<span class="hlt">pressure</span> <span class="hlt">waves</span> 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 <span class="hlt">pressure</span> 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 <span class="hlt">pressure</span> increase.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008PhDT.......181K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008PhDT.......181K"><span>The effect of convection and shear on the damping and propagation of <span class="hlt">pressure</span> <span class="hlt">waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kiel, Barry Vincent</p> <p></p> <p>Combustion instability is the positive feedback between heat release and <span class="hlt">pressure</span> in a combustion system. Combustion instability occurs in the both air breathing and rocket propulsion devices, frequently resulting in high amplitude spinning <span class="hlt">waves</span>. If unchecked, the resultant <span class="hlt">pressure</span> fluctuations can cause significant damage. Models for the prediction of combustion instability typically include models for the heat release, the <span class="hlt">wave</span> propagation and damping. Many <span class="hlt">wave</span> propagation models for propulsion systems assume negligible flow, resulting in the <span class="hlt">wave</span> equation. In this research the effect of flow on <span class="hlt">wave</span> propagation was studied both numerically and experimentally. Two experiential rigs were constructed, one with axial flow to study the longitudinal <span class="hlt">waves</span>, the other with swirling flow to study circumferential <span class="hlt">waves</span>. The rigs were excited with speakers and the resultant <span class="hlt">pressure</span> was measured simultaneously at many locations. Models of the rig were also developed. Equations for <span class="hlt">wave</span> propagation were derived from the Euler Equations. The resultant resembled the <span class="hlt">wave</span> equation with three additional terms, two for the effect of the convection and a one for the effect of shear of the mean flow on <span class="hlt">wave</span> propagation. From the experimental and numerical data several conclusions were made. First, convection and shear both act as damping on the <span class="hlt">wave</span> propagation, reducing the magnitude of the Frequency Response Function and the resonant frequency of the modes. Second, the energy extracted from the mean flow as a result of turbulent shear for a given condition is frequency dependent, decreasing with increasing frequency. The damping of the modes, measured for the same shear flow, also decreased with frequency. Finally, the two convective terms cause the anti-nodes of the modes to no longer be stationary. For both the longitudinal and circumferential <span class="hlt">waves</span>, the anti-nodes move through the domain even for mean flow Mach numbers less than 0.10. It was concluded that convection</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-acoustic <span class="hlt">waves</span> 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-acoustic (DPDMNA) <span class="hlt">waves</span> 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 <span class="hlt">waves</span> (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 <span class="hlt">waves</span> 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 <span class="hlt">waves</span> 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.ncbi.nlm.nih.gov/pubmed/23927207','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23927207"><span>Acoustic field characterization of the Duolith: measurements and modeling of a clinical shock <span class="hlt">wave</span> therapy device.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Perez, Camilo; Chen, Hong; Matula, Thomas J; Karzova, Maria; Khokhlova, Vera A</p> <p>2013-08-01</p> <p>Extracorporeal shock <span class="hlt">wave</span> therapy (ESWT) uses acoustic pulses to treat certain musculoskeletal disorders. In this paper the acoustic field of a clinical <span class="hlt">portable</span> ESWT device (Duolith SD1) was characterized. Field mapping was performed in water for two different standoffs of the electromagnetic head (15 or 30 mm) using a fiber optic probe hydrophone. Peak positive <span class="hlt">pressures</span> at the focus ranged from 2 to 45 MPa, while peak negative <span class="hlt">pressures</span> ranged from -2 to -11 MPa. Pulse rise times ranged from 8 to 500 ns; shock formation did not occur for any machine settings. The maximum standard deviation in peak <span class="hlt">pressure</span> at the focus was 1.2%, indicating that the Duolith SD1 generates stable pulses. The results compare qualitatively, but not quantitatively with manufacturer specifications. Simulations were carried out for the short standoff by matching a Khokhlov-Zabolotskaya-Kuznetzov equation to the measured field at a plane near the source, and then propagating the <span class="hlt">wave</span> outward. The results of modeling agree well with experimental data. The model was used to analyze the spatial structure of the peak <span class="hlt">pressures</span>. Predictions from the model suggest that a true shock <span class="hlt">wave</span> could be obtained in water if the initial <span class="hlt">pressure</span> output of the device were doubled.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3745538','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3745538"><span>Acoustic field characterization of the Duolith: Measurements and modeling of a clinical shock <span class="hlt">wave</span> therapy 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>Perez, Camilo; Chen, Hong; Matula, Thomas J.; Karzova, Maria; Khokhlova, Vera A.</p> <p>2013-01-01</p> <p>Extracorporeal shock <span class="hlt">wave</span> therapy (ESWT) uses acoustic pulses to treat certain musculoskeletal disorders. In this paper the acoustic field of a clinical <span class="hlt">portable</span> ESWT device (Duolith SD1) was characterized. Field mapping was performed in water for two different standoffs of the electromagnetic head (15 or 30 mm) using a fiber optic probe hydrophone. Peak positive <span class="hlt">pressures</span> at the focus ranged from 2 to 45 MPa, while peak negative <span class="hlt">pressures</span> ranged from −2 to −11 MPa. Pulse rise times ranged from 8 to 500 ns; shock formation did not occur for any machine settings. The maximum standard deviation in peak <span class="hlt">pressure</span> at the focus was 1.2%, indicating that the Duolith SD1 generates stable pulses. The results compare qualitatively, but not quantitatively with manufacturer specifications. Simulations were carried out for the short standoff by matching a Khokhlov-Zabolotskaya-Kuznetzov equation to the measured field at a plane near the source, and then propagating the <span class="hlt">wave</span> outward. The results of modeling agree well with experimental data. The model was used to analyze the spatial structure of the peak <span class="hlt">pressures</span>. Predictions from the model suggest that a true shock <span class="hlt">wave</span> could be obtained in water if the initial <span class="hlt">pressure</span> output of the device were doubled. PMID:23927207</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24997065','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24997065"><span>[P <span class="hlt">wave</span> dispersion increased in childhood depending on blood <span class="hlt">pressure</span>, weight, height, and cardiac structure and function].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chávez-González, Elibet; González-Rodríguez, Emilio; Llanes-Camacho, María Del Carmen; Garí-Llanes, Merlin; García-Nóbrega, Yosvany; García-Sáez, Julieta</p> <p>2014-01-01</p> <p>Increased P <span class="hlt">wave</span> dispersion are identified as a predictor of atrial fibrillation. There are associations between hypertension, P <span class="hlt">wave</span> dispersion, constitutional and echocardiographic variables. These relationships have been scarcely studied in pediatrics. The aim of this study was to determine the relationship between P <span class="hlt">wave</span> dispersion, blood <span class="hlt">pressure</span>, echocardiographic and constitutional variables, and determine the most influential variables on P <span class="hlt">wave</span> dispersion increases in pediatrics. In the frame of the PROCDEC II project, children from 8 to 11 years old, without known heart conditions were studied. Arterial blood <span class="hlt">pressure</span> was measured in all the children; a 12-lead surface electrocardiogram and an echocardiogram were done as well. Left ventricular mass index mean values for normotensive (25.91±5.96g/m(2.7)) and hypertensive (30.34±8.48g/m(2.7)) showed significant differences P=.000. When we add prehypertensive and hypertensive there are 50.38% with normal left ventricular mass index and P <span class="hlt">wave</span> dispersion was increased versus 13.36% of normotensive. Multiple regression demonstrated that the mean blood <span class="hlt">pressure</span>, duration of A <span class="hlt">wave</span> of mitral inflow, weight and height have a value of r=0.88 as related to P <span class="hlt">wave</span> dispersion. P <span class="hlt">wave</span> dispersion is increased in pre- and hypertensive children compared to normotensive. There are pre- and hypertensive patients with normal left ventricular mass index and increased P <span class="hlt">wave</span> dispersion. Mean arterial <span class="hlt">pressure</span>, duration of the A <span class="hlt">wave</span> of mitral inflow, weight and height are the variables with the highest influence on increased P <span class="hlt">wave</span> dispersion. Copyright © 2013 Instituto Nacional de Cardiología Ignacio Chávez. Published by Masson Doyma México S.A. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21994066','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21994066"><span>Mild neurotrauma indicates a range-specific <span class="hlt">pressure</span> response to low level shock <span class="hlt">wave</span> exposure.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Vandevord, Pamela J; Bolander, Richard; Sajja, Venkata Siva Sai Sujith; Hay, Kathryn; Bir, Cynthia A</p> <p>2012-01-01</p> <p>Identifying the level of overpressure required to create physiological deficits is vital to advance prevention, diagnostic, and treatment strategies for individuals exposed to blasts. In this study, a rodent model of primary blast neurotrauma was employed to determine the <span class="hlt">pressure</span> at which acute neurological alterations occurred. Rats were exposed to a single low intensity shock <span class="hlt">wave</span> at a <span class="hlt">pressure</span> of 0, 97, 117, or 153 kPa. Following exposure, rats were assessed for acute cognitive alterations using the Morris water maze and motor dysfunction using the horizontal ladder test. Subsequently, histological analyses of three brain regions (primary motor cortex, the hippocampal dentate gyrus region, and the posteromedial cortical amygdala) were conducted. Histological parameters included measuring the levels of glial fibrillary acidic protein (GFAP) to identify astrocyte activation, cleaved caspase-3 for early apoptosis identification and Fluoro-Jade B (FJB) which labels degenerating neurons within the brain tissue. The results demonstrated that an exposure to a single 117 kPa shock <span class="hlt">wave</span> revealed a significant change in overall neurological deficits when compared to controls and the other <span class="hlt">pressures</span>. The animals showed significant alterations in water maze parameters and a histological increase in the number of GFAP, caspase-3, and FJB-positive cells. It is suggested that when exposed to a low level shock <span class="hlt">wave</span>, there may be a biomechanical response elicited by a specific <span class="hlt">pressure</span> range which can cause low level neurological deficits within the rat. These data indicate that neurotrauma induced from a shock <span class="hlt">wave</span> may lead to cognitive deficits in short-term learning and memory of rats. Additional histological evidence supports significant and diffuse glial activation and cellular damage. Further investigation into the biomechanical aspects of shock <span class="hlt">wave</span> exposure is required to elucidate this <span class="hlt">pressure</span> range-specific phenomenon.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001AGUFM.V31A0934N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001AGUFM.V31A0934N"><span>Bulk Viscosity of Bubbly Magmas and the Amplification of <span class="hlt">Pressure</span> <span class="hlt">Waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Navon, O.; Lensky, N. G.; Neuberg, J. W.; Lyakhovsky, V.</p> <p>2001-12-01</p> <p>The bulk viscosity of magma is needed in order to describe the dynamics of a compressible bubbly magma flowing in conduits and to follow the attenuation of <span class="hlt">pressure</span> <span class="hlt">waves</span> travelling through a compressible magma. We developed a model for the bulk viscosity of a suspension of gas bubbles in an incompressible Newtonian liquid that exsolves volatiles (e.g. magma). The suspension is modeled as a close pack of spherical cells, consisting of gas bubbles centered in spherical shells of a volatile-bearing liquid. Following a drop in the ambient <span class="hlt">pressure</span> the resulting dilatational motion and driving <span class="hlt">pressure</span> are obtained in terms of the two-phase cell parameters, i.e. bubble radius and gas <span class="hlt">pressure</span>. By definition, the bulk viscosity of a fluid is the relation between changes of the driving <span class="hlt">pressure</span> with respect to changes in the resulted expansion strain-rate. Thus, we can use the two-phase solution to define the bulk viscosity of a hypothetical cell, composed of a homogeneously compressible, one-phase, continuous fluid. The resulted bulk viscosity is highly non-linear. At the beginning of the expansion process, when gas exsolution is efficient, the expansion rate grows exponentially while the driving <span class="hlt">pressure</span> decreases slightly. That means that bulk viscosity is formally negative. The negative value reflects the release of the energy stored in the supersaturated liquid (melt) and its conversion to mechanical work during exsolution. Later, when bubbles are large enough and the gas influx decreases significantly, the strain rate decelerates and the bulk viscosity becomes positive as expected in a dissipative system. We demonstrate that amplification of seismic <span class="hlt">wave</span> travelling through a volcanic conduit filled with a volatile saturated magma may be attributed to the negative bulk viscosity of the compressible magma. Amplification of an expansion <span class="hlt">wave</span> may, at some level in the conduit, damage the conduit walls and initiate opening of new pathways for magma to erupt.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29335669','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29335669"><span><span class="hlt">Portable</span> FAIMS: Applications and Future Perspectives.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Costanzo, Michael T; Boock, Jared J; Kemperman, Robin H J; Wei, Michael S; Beekman, Christopher R; Yost, Richard A</p> <p>2017-11-01</p> <p>Miniaturized mass spectrometry (MMS) is optimal for a wide variety of applications that benefit from field-<span class="hlt">portable</span> instrumentation. Like MMS, field asymmetric ion mobility spectrometry (FAIMS) has proven capable of providing in situ analysis, allowing researchers to bring the lab to the sample. FAIMS compliments MMS very well, but has the added benefit of operating at atmospheric <span class="hlt">pressure</span>, unlike MS. This distinct advantage makes FAIMS uniquely suited for <span class="hlt">portability</span>. Since its inception, FAIMS has been envisioned as a field-<span class="hlt">portable</span> device, as it affords less expense and greater simplicity than many similar methods. Ideally, these are simple, robust devices that may be operated by non-professional personnel, yet still provide adequate data when in the field. While reducing the size and complexity tends to bring with it a loss of performance and accuracy, this is made up for by the incredibly high throughput and overall convenience of the instrument. Moreover, the FAIMS device used in the field can be brought back to the lab, and coupled to a conventional mass spectrometer to provide any necessary method development and compound validation. This work discusses the various considerations, uses, and applications for <span class="hlt">portable</span> FAIMS instrumentation, and how the future of each applicable field may benefit from the development and acceptance of such a device.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/115055','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/115055"><span>Thermal-hydraulic behaviors of vapor-liquid interface due to arrival of a <span class="hlt">pressure</span> <span class="hlt">wave</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>Inoue, Akira; Fujii, Yoshifumi; Matsuzaki, Mitsuo</p> <p></p> <p>In the vapor explosion, a <span class="hlt">pressure</span> <span class="hlt">wave</span> (shock <span class="hlt">wave</span>) plays a fundamental role for triggering, propagation and enhancement of the explosion. Energy of the explosion is related to the magnitude of heat transfer rate from hot liquid to cold volatile one. This is related to an increasing rate of interface area and to an amount of transient heat flux between the liquids. In this study, the characteristics of transient heat transfer and behaviors of vapor film both on the platinum tube and on the hot melt tin drop, under same boundary conditions have been investigated. It is considered that theremore » exists a fundamental mechanism of the explosion in the initial expansion process of the hot liquid drop immediately after arrival of <span class="hlt">pressure</span> <span class="hlt">wave</span>. The growth rate of the vapor film is much faster on the hot liquid than that on the solid surface. Two kinds of roughness were observed, one due to the Taylor instability, by rapid growth of the explosion bubble, and another, nucleation sites were observed at the vapor-liquid interface. Based on detailed observation of early stage interface behaviors after arrival of a <span class="hlt">pressure</span> <span class="hlt">wave</span>, the thermal fragmentation mechanism is proposed.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800067239&hterms=sensors+pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dsensors%2Bpressure','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800067239&hterms=sensors+pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dsensors%2Bpressure"><span>Comparisons between <span class="hlt">wave</span> directional spectra from SAR and <span class="hlt">pressure</span> sensor arrays</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pawka, S. S.; Inman, D. L.; Hsiao, S. V.; Shemdin, O. H.</p> <p>1980-01-01</p> <p>Simultaneous directional <span class="hlt">wave</span> measurements were made at Torrey Pines Beach, California, by a synthetic aperture radar (SAR) and a linear array of <span class="hlt">pressure</span> sensors. The measurements were conducted during the West Coast Experiment in March 1977. Quantitative comparisons of the normalized directional spectra from the two systems were made for <span class="hlt">wave</span> periods of 6.9-17.0 s. The comparison results were variable but generally showed good agreement of the primary mode of the normalized directional energy. An attempt was made to quantify the physical criteria for good <span class="hlt">wave</span> imaging in the SAR. A frequency band analysis of <span class="hlt">wave</span> parameters such as band energy, slope, and orbital velocity did not show good correlation with the directional comparisons. It is noted that absolute values of the <span class="hlt">wave</span> height spectrum cannot be derived from the SAR images yet and, consequently, no comparisons of absolute energy levels with corresponding array measurements were intended.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AIPC.1060..106P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AIPC.1060..106P"><span>Two Dimensional Finite Element Analysis for the Effect of a <span class="hlt">Pressure</span> <span class="hlt">Wave</span> in the Human Brain</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ponce L., Ernesto; Ponce S., Daniel</p> <p>2008-11-01</p> <p>Brain injuries in people of all ages is a serious, world-wide health problem, with consequences as varied as attention or memory deficits, difficulties in problem-solving, aggressive social behavior, and neuro degenerative diseases such as Alzheimer's and Parkinson's. Brain injuries can be the result of a direct impact, but also <span class="hlt">pressure</span> <span class="hlt">waves</span> and direct impulses. The aim of this work is to develop a predictive method to calculate the stress generated in the human brain by <span class="hlt">pressure</span> <span class="hlt">waves</span> such as high power sounds. The finite element method is used, combined with elastic <span class="hlt">wave</span> theory. The predictions of the generated stress levels are compared with the resistance of the arterioles that pervade the brain. The problem was focused to the Chilean mining where there are some accidents happen by detonations and high sound level. There are not formal medical investigation, however these <span class="hlt">pressure</span> <span class="hlt">waves</span> could produce human brain damage.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/EJ1131332.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/EJ1131332.pdf"><span>Making Leaders: Leadership Characteristics of <span class="hlt">Makers</span> and Engineers in the <span class="hlt">Maker</span> Community</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>Oplinger, James; Lande, Micah; Jordan, Shawn; Camarena, Leonor</p> <p>2016-01-01</p> <p>This study examines the emergence of leadership characteristics within a new organizational community of individuals: the <span class="hlt">Maker</span> community. The <span class="hlt">Maker</span> community is a group of individuals that classify themselves as "<span class="hlt">Makers</span>" and have become innovators and entrepreneurs through the creation of technological gadgets, artistic projects, and…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21870376','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21870376"><span><span class="hlt">Pressure</span> <span class="hlt">waves</span> in the aorta during isolated abdominal belt loading: the magnitude, phasing, and attenuation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Arregui-Dalmases, C; Del Pozo, E; Stacey, S; Kindig, M; Lessley, D; Lopez-Valdes, F; Forman, J; Kent, R</p> <p>2011-07-01</p> <p>While rupture of the aorta is a leading cause of sudden death following motor vehicle crashes, the specific mechanism that causes this injury is not currently well understood. Aortic ruptures occurring in the field are likely due to a complex combination of contributing factors such as acceleration, compression of the chest, and increased <span class="hlt">pressure</span> within the aorta. The objective of the current study was to investigate one of these factors in more detail than has been done previously; specifically, to investigate the in situ intra-aortic <span class="hlt">pressure</span> generated during isolated belt loading to the abdomen. Ten juvenile swine were subjected to dynamic belt loads applied to the abdomen. Intraaortic <span class="hlt">pressure</span> was measured at multiple locations to assess the magnitude and propagation of the resulting blood <span class="hlt">pressure</span> <span class="hlt">wave</span>. The greatest average peak <span class="hlt">pressure</span> (113.6 +/- 43.5 kPa) was measured in the abdominal aorta. <span class="hlt">Pressures</span> measured in the thoracic aorta and aortic arch were 70 per cent and 50 per cent, respectively, that measured in the abdominal aorta. No macroscopic aortic trauma was observed. To the authors' knowledge the present study is the first one to document the presence, propagation, and attenuation of a transient <span class="hlt">pressure</span> <span class="hlt">wave</span> in the aorta generated by abdominal belt loading. The superiorly moving <span class="hlt">wave</span> is sufficient to generate hydrostatic and intimal shear stress in the aorta, possibly contributing to the hypothesized mechanisms of traumatic aortic rupture.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28438216','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28438216"><span>Improved <span class="hlt">pressure</span> contour analysis for estimating cardiac stroke volume using pulse <span class="hlt">wave</span> velocity measurement.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kamoi, Shun; Pretty, Christopher; Balmer, Joel; Davidson, Shaun; Pironet, Antoine; Desaive, Thomas; Shaw, Geoffrey M; Chase, J Geoffrey</p> <p>2017-04-24</p> <p><span class="hlt">Pressure</span> contour analysis is commonly used to estimate cardiac performance for patients suffering from cardiovascular dysfunction in the intensive care unit. However, the existing techniques for continuous estimation of stroke volume (SV) from <span class="hlt">pressure</span> measurement can be unreliable during hemodynamic instability, which is inevitable for patients requiring significant treatment. For this reason, <span class="hlt">pressure</span> contour methods must be improved to capture changes in vascular properties and thus provide accurate conversion from <span class="hlt">pressure</span> to flow. This paper presents a novel <span class="hlt">pressure</span> contour method utilizing pulse <span class="hlt">wave</span> velocity (PWV) measurement to capture vascular properties. A three-element Windkessel model combined with the reservoir-<span class="hlt">wave</span> concept are used to decompose the <span class="hlt">pressure</span> contour into components related to storage and flow. The model parameters are identified beat-to-beat from the water-hammer equation using measured PWV, <span class="hlt">wave</span> component of the <span class="hlt">pressure</span>, and an estimate of subject-specific aortic dimension. SV is then calculated by converting <span class="hlt">pressure</span> to flow using identified model parameters. The accuracy of this novel method is investigated using data from porcine experiments (N = 4 Pietrain pigs, 20-24.5 kg), where hemodynamic properties were significantly altered using dobutamine, fluid administration, and mechanical ventilation. In the experiment, left ventricular volume was measured using admittance catheter, and aortic <span class="hlt">pressure</span> waveforms were measured at two locations, the aortic arch and abdominal aorta. Bland-Altman analysis comparing gold-standard SV measured by the admittance catheter and estimated SV from the novel method showed average limits of agreement of ±26% across significant hemodynamic alterations. This result shows the method is capable of estimating clinically acceptable absolute SV values according to Critchely and Critchely. The novel <span class="hlt">pressure</span> contour method presented can accurately estimate and track SV even when hemodynamic properties</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C51B0970C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C51B0970C"><span>Ocean <span class="hlt">Wave</span>-to-Ice Energy Transfer Determined from Seafloor <span class="hlt">Pressure</span> and Ice Shelf Seismic Observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Z.; Bromirski, P. D.; Gerstoft, P.; Stephen, R. A.; Wiens, D.; Aster, R. C.; Nyblade, A.</p> <p>2017-12-01</p> <p>Ice shelves play an important role in buttressing land ice from reaching the sea, thus restraining the rate of sea level rise. Long-period gravity <span class="hlt">wave</span> impacts excite vibrations in ice shelves that may trigger tabular iceberg calving and/or ice shelf collapse events. Three kinds of seismic plate <span class="hlt">waves</span> were continuously observed by broadband seismic arrays on the Ross Ice Shelf (RIS) and on the Pine Island Glacier (PIG) ice shelf: (1) flexural-gravity <span class="hlt">waves</span>, (2) flexural <span class="hlt">waves</span>, and (3) extensional Lamb <span class="hlt">waves</span>, suggesting that all West Antarctic ice shelves are subjected to similar gravity <span class="hlt">wave</span> excitation. Ocean gravity <span class="hlt">wave</span> heights were estimated from <span class="hlt">pressure</span> perturbations recorded by an ocean bottom differential <span class="hlt">pressure</span> gauge at the RIS front, water depth 741 m, about 8 km north of an on-ice seismic station that is 2 km from the shelf front. Combining the plate <span class="hlt">wave</span> spectrum, the frequency-dependent energy transmission and reflection at the ice-water interface were determined. In addition, Young's modulus and Poisson's ratio of the RIS are estimated from the plate <span class="hlt">wave</span> motions, and compared with the widely used values. Quantifying these ice shelf parameters from observations will improve modeling of ice shelf response to ocean forcing, and ice shelf evolution.</p> </li> <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 acoustic <span class="hlt">wave</span> 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 acoustic <span class="hlt">wave</span> (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('https://www.ncbi.nlm.nih.gov/pubmed/29289063','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29289063"><span><span class="hlt">Pressure</span> and tension <span class="hlt">waves</span> from bubble collapse near a solid boundary: A numerical approach.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lechner, Christiane; Koch, Max; Lauterborn, Werner; Mettin, Robert</p> <p>2017-12-01</p> <p>The acoustic <span class="hlt">waves</span> being generated during the motion of a bubble in water near a solid boundary are calculated numerically. The open source package OpenFOAM is used for solving the Navier-Stokes equation and extended to include nonlinear acoustic <span class="hlt">wave</span> effects via the Tait equation for water. A bubble model with a small amount of gas is chosen, the gas obeying an adiabatic law. A bubble starting from a small size with high internal <span class="hlt">pressure</span> near a flat, solid boundary is studied. The sequence of events from bubble growth via axial microjet formation, jet impact, annular nanojet formation, torus-bubble collapse, and bubble rebound to second collapse is described. The different <span class="hlt">pressure</span> and tension <span class="hlt">waves</span> with their propagation properties are demonstrated.</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/2017EGUGA..1916834T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1916834T"><span>Planar time-resolved PIV for velocity and <span class="hlt">pressure</span> retrieval in atmospheric boundary layer over surface <span class="hlt">waves</span>.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Troitskaya, Yuliya; Kandaurov, Alexander; Sergeev, Daniil; Bopp, Maximilian; Caulliez, Guillemette</p> <p>2017-04-01</p> <p>Air-sea coupling in general is important for weather, climate, fluxes. Wind <span class="hlt">wave</span> source is crucially important for surface <span class="hlt">waves</span>' modeling. But the wind-<span class="hlt">wave</span> growth rate is strongly uncertain. Using direct measurements of <span class="hlt">pressure</span> by <span class="hlt">wave</span>-following Elliott probe [1] showed, weak and indefinite dependence of wind-<span class="hlt">wave</span> growth rate on the <span class="hlt">wave</span> steepness, while Grare et.al. [2] discuss the limitations of direct measurements of <span class="hlt">pressure</span> associated with the inability to measure the <span class="hlt">pressure</span> close to the surface by contact methods. Recently non-invasive methods for determining the <span class="hlt">pressure</span> on the basis of technology of time-resolved PIV are actively developed [3]. Retrieving air flow velocities by 2D PIV techniques was started from Reul et al [4]. The first attempt for retrieving wind <span class="hlt">pressure</span> field of <span class="hlt">waves</span> in the laboratory tank from the time-resolved PIV measurements was done in [5]. The experiments were performed at the Large Air-Sea Interaction Facility (LASIF) - MIO/Luminy (length 40 m, cross section of air channel 3.2 x 1.6 m). For 18 regimes with wind speed up to 14 m/s including presence of puddle <span class="hlt">waves</span>, a combination of time resolved PIV technique and optical measurements of water surface form was applied to detailed investigation of the characteristics of the wind flow over the water surface. Ammonium chloride smoke was used for flow visualization illuminated by two 6 Wt blue diode lasers combined into a vertical laser plane. Particle movement was captured with high-speed camera using Scheimpflug technique (up to 20 kHz frame rate with 4-frame bursts, spatial resolution about 190 μm, field of view 314x12 mm). Velocity air flow field was retrieved by PIV images processing with adaptive cross-correlation method on the curvilinear grid following surface <span class="hlt">wave</span> form. The resulting time resolved instantaneous velocity fields on regular grid allowed us to obtain momentum fluxes directly from measured air velocity fluctuations. The average wind velocity patterns were</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26213717','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26213717"><span>Cuff-Free Blood <span class="hlt">Pressure</span> Estimation Using Pulse Transit Time and Heart Rate.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Ruiping; Jia, Wenyan; Mao, Zhi-Hong; Sclabassi, Robert J; Sun, Mingui</p> <p>2014-10-01</p> <p>It has been reported that the pulse transit time (PTT), the interval between the peak of the R-<span class="hlt">wave</span> in electrocardiogram (ECG) and the fingertip photoplethysmogram (PPG), is related to arterial stiffness, and can be used to estimate the systolic blood <span class="hlt">pressure</span> (SBP) and diastolic blood <span class="hlt">pressure</span> (DBP). This phenomenon has been used as the basis to design <span class="hlt">portable</span> systems for continuously cuff-less blood <span class="hlt">pressure</span> measurement, benefiting numerous people with heart conditions. However, the PTT-based blood <span class="hlt">pressure</span> estimation may not be sufficiently accurate because the regulation of blood <span class="hlt">pressure</span> within the human body is a complex, multivariate physiological process. Considering the negative feedback mechanism in the blood <span class="hlt">pressure</span> control, we introduce the heart rate (HR) and the blood <span class="hlt">pressure</span> estimate in the previous step to obtain the current estimate. We validate this method using a clinical database. Our results show that the PTT, HR and previous estimate reduce the estimated error significantly when compared to the conventional PTT estimation approach (p<0.05).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160005390','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160005390"><span><span class="hlt">Portable</span> Cathode-Air Vapor-Feed Electrochemical Medical Oxygen Concentrator (OC)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Balasubramanian, Ashwin</p> <p>2015-01-01</p> <p>Missions on the International Space Station and future space exploration will present significant challenges to crew health care capabilities, particularly in the efficient utilization of onboard oxygen resources. Exploration vehicles will require lightweight, compact, and <span class="hlt">portable</span> oxygen concentrators that can provide medical-grade oxygen from the ambient cabin air. Current <span class="hlt">pressure</span>-swing adsorption OCs are heavy and bulky, require significant start-up periods, operate in narrow temperature ranges, and require a liquid water feed. Lynntech, Inc., has developed an electrochemical OC that operates with a cathode-air vapor feed, eliminating the need for a bulky onboard water supply. Lynntech's OC is smaller and lighter than conventional <span class="hlt">pressure</span>-swing OCs, is capable of instant start-up, and operates over a temperature range of 5-80 C. Accomplished through a unique nanocomposite proton exchange membrane and catalyst technology, the unit delivers 4 standard liters per minute of humidified oxygen at 60 percent concentration. The technology enables both ambient-<span class="hlt">pressure</span> operating devices for <span class="hlt">portable</span> applications and <span class="hlt">pressurized</span> (up to 3,600 psi) OC devices for stationary applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002ASAJ..112.2240T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002ASAJ..112.2240T"><span>Radiation <span class="hlt">pressure</span> of standing <span class="hlt">waves</span> on liquid columns and small diffusion flames</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Thiessen, David B.; Marr-Lyon, Mark J.; Wei, Wei; Marston, Philip L.</p> <p>2002-11-01</p> <p>The radiation <span class="hlt">pressure</span> of standing ultrasonic <span class="hlt">waves</span> in air is demonstrated in this investigation to influence the dynamics of liquid columns and small flames. With the appropriate choice of the acoustic amplitude and wavelength, the natural tendency of long columns to break because of surface tension was suppressed in reduced gravity [M. J. Marr-Lyon, D. B. Thiessen, and P. L. Marston, Phys. Rev. Lett. 86, 2293-2296 (2001); 87(20), 9001(E) (2001)]. Evaluation of the radiation force shows that narrow liquid columns are attracted to velocity antinodes. The response of a small vertical diffusion flame to ultrasonic radiation <span class="hlt">pressure</span> in a horizontal standing <span class="hlt">wave</span> was observed in normal gravity. In agreement with our predictions of the distribution of ultrasonic radiation stress on the flame, the flame is attracted to a <span class="hlt">pressure</span> antinode and becomes slightly elliptical with the major axis in the plane of the antinode. The radiation <span class="hlt">pressure</span> distribution and the direction of the radiation force follow from the dominance of the dipole scattering for small flames. Understanding radiation stress on flames is relevant to the control of hot fluid objects. [Work supported by NASA.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920006759','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920006759"><span><span class="hlt">Pressure</span> <span class="hlt">wave</span> propagation studies for oscillating cascades</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Huff, Dennis L.</p> <p>1992-01-01</p> <p>The unsteady flow field around an oscillating cascade of flat plates is studied using a time marching Euler code. Exact solutions based on linear theory serve as model problems to study <span class="hlt">pressure</span> <span class="hlt">wave</span> propagation in the numerical solution. The importance of using proper unsteady boundary conditions, grid resolution, and time step is demonstrated. Results show that an approximate non-reflecting boundary condition based on linear theory does a good job of minimizing reflections from the inflow and outflow boundaries and allows the placement of the boundaries to be closer than cases using reflective boundary conditions. Stretching the boundary to dampen the unsteady <span class="hlt">waves</span> is another way to minimize reflections. Grid clustering near the plates does a better job of capturing the unsteady flow field than cases using uniform grids as long as the CFL number is less than one for a sufficient portion of the grid. Results for various stagger angles and oscillation frequencies show good agreement with linear theory as long as the grid is properly resolved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1821h0001Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1821h0001Z"><span>Simulations of nonlinear continuous <span class="hlt">wave</span> <span class="hlt">pressure</span> fields in FOCUS</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Xiaofeng; Hamilton, Mark F.; McGough, Robert J.</p> <p>2017-03-01</p> <p>The Khokhlov - Zabolotskaya - Kuznetsov (KZK) equation is a parabolic approximation to the Westervelt equation that models the effects of diffraction, attenuation, and nonlinearity. Although the KZK equation is only valid in the far field of the paraxial region for mildly focused or unfocused transducers, the KZK equation is widely applied in medical ultrasound simulations. For a continuous <span class="hlt">wave</span> input, the KZK equation is effectively modeled by the Bergen Code [J. Berntsen, Numerical Calculations of Finite Amplitude Sound Beams, in M. F. Hamilton and D. T. Blackstock, editors, Frontiers of Nonlinear Acoustics: Proceedings of 12th ISNA, Elsevier, 1990], which is a finite difference model that utilizes operator splitting. Similar C++ routines have been developed for FOCUS, the `Fast Object-Oriented C++ Ultrasound Simulator' (http://www.egr.msu.edu/˜fultras-web) to calculate nonlinear <span class="hlt">pressure</span> fields generated by axisymmetric flat circular and spherically focused ultrasound transducers. This new routine complements an existing FOCUS program that models nonlinear ultrasound propagation with the angular spectrum approach [P. T. Christopher and K. J. Parker, J. Acoust. Soc. Am. 90, 488-499 (1991)]. Results obtained from these two nonlinear ultrasound simulation approaches are evaluated and compared for continuous <span class="hlt">wave</span> linear simulations. The simulation results match closely in the farfield of the paraxial region, but the results differ in the nearfield. The nonlinear <span class="hlt">pressure</span> field generated by a spherically focused transducer with a peak surface <span class="hlt">pressure</span> of 0.2MPa radiating in a lossy medium with β = 3.5 is simulated, and the computation times are also evaluated. The nonlinear simulation results demonstrate acceptable agreement in the focal zone. These two related nonlinear simulation approaches are now included with FOCUS to enable convenient simulations of nonlinear <span class="hlt">pressure</span> fields on desktop and laptop computers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017RSPTA.37670087B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017RSPTA.37670087B"><span><span class="hlt">Wave</span> height estimates from <span class="hlt">pressure</span> and velocity data at an intermediate depth in the presence of uniform currents</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Basu, Biswajit</p> <p>2017-12-01</p> <p>Bounds on estimates of <span class="hlt">wave</span> heights (valid for large amplitudes) from <span class="hlt">pressure</span> and flow measurements at an arbitrary intermediate depth have been provided. Two-dimensional irrotational steady water <span class="hlt">waves</span> over a flat bed with a finite depth in the presence of underlying uniform currents have been considered in the analysis. Five different upper bounds based on a combination of <span class="hlt">pressure</span> and velocity field measurements have been derived, though there is only one available lower bound on the <span class="hlt">wave</span> height in the case of the speed of current greater than or less than the <span class="hlt">wave</span> speed. This article is part of the theme issue 'Nonlinear water <span class="hlt">waves</span>'.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25150924','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25150924"><span>Treadmill walking with load carriage increases aortic <span class="hlt">pressure</span> <span class="hlt">wave</span> reflection.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ribeiro, Fernando; Oliveira, Nórton L; Pires, Joana; Alves, Alberto J; Oliveira, José</p> <p>2014-01-01</p> <p>The study examined the effects of treadmill walking with load carriage on derived measures of central <span class="hlt">pressure</span> and augmentation index in young healthy subjects. Fourteen male subjects (age 31.0 ± 1.0 years) volunteered in this study. Subjects walked 10 minutes on a treadmill at a speed of 5 km/h carrying no load during one session and a load of 10% of their body weight on both upper limbs in two water carboys with handle during the other session. Pulse <span class="hlt">wave</span> analysis was performed at rest and immediately after exercise in the radial artery of the right upper limb by applanation tonometry. The main result indicates that walking with load carriage sharply increased augmentation index at 75 bpm (-5.5 ± 2.2 to -1.4 ± 2.2% vs. -5.2 ± 2.8 to -5.5 ± 2.1%, p<0.05), and also induced twice as high increments in central pulse <span class="hlt">pressure</span> (7.4 ± 1.5 vs. 3.1 ± 1.4 mmHg, p<0.05) and peripheral (20.5 ± 2.7 vs. 10.3 ± 2.5 mmHg, p<0.05) and central systolic <span class="hlt">pressure</span> (14.7 ± 2.1 vs. 7.4 ± 2.0 mmHg, p<0.05). Walking with additional load of 10% of their body weight (aerobic exercise accompanied by upper limb isometric contraction) increases derived measures of central <span class="hlt">pressure</span> and augmentation index, an index of <span class="hlt">wave</span> reflection and arterial stiffness. Copyright © 2013 Sociedade Portuguesa de Cardiologia. Published by Elsevier España. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JPhCS.774a2054S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JPhCS.774a2054S"><span>Superconductivity of Cu/CuOx interface formed by shock-<span class="hlt">wave</span> <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>Shakhray, D. V.; Avdonin, V. V.; Palnichenko, A. V.</p> <p>2016-11-01</p> <p>A mixture of powdered Cu and CuO has been subjected to shock-<span class="hlt">wave</span> <span class="hlt">pressure</span> of 350 kbar with following quenching of the vacuum-encapsulated product to 77 K. The ac magnetic susceptibility measurements of the samples have revealed metastable superconductivity with Tc ≈ 19 K, characterized by glassy dynamics of the shielding currents below Tc . Comparison of the ac susceptibility and the DC magnetization measurements infers that the superconductivity arises within the granular interfacial layer formed between metallic Cu and its oxides due to the shock-<span class="hlt">wave</span> treatment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.V43A3092J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.V43A3092J"><span><span class="hlt">Pressure</span> <span class="hlt">Wave</span> Propagation along the Décollement of the Nankai Accretionary Wedge: Implications for Aseismic Slip Events</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Joshi, A.; Appold, M. S.</p> <p>2015-12-01</p> <p>Seismic and hydrologic observations of the Nankai subduction zone made by the Ocean Drilling Program suggest that pore fluid <span class="hlt">pressures</span> within the accretionary wedge décollement are highly overpressured to near lithostatic values below depths of 2 km beneath the sea floor as a result of sediment diagenesis and dehydration of the subducting oceanic plate. This overpressured zone is also observed to discharge pulses of high fluid <span class="hlt">pressure</span> that migrate up-dip along the décollement at rates of 1's of km/day. These high <span class="hlt">pressure</span> pulses along the décollement may cause large enough reductions in the local effective stress to account for aseismic slip events that have been found to propagate also at rates of 1's of km/day. Because elevated fluid <span class="hlt">pressure</span> and correspondingly decreased effective stress can lead to a dilation of porosity, the <span class="hlt">pressure</span> <span class="hlt">waves</span> may become effective agents of fluid transport that can travel more quickly than fluids flowing in the background Darcian flow regime. The purpose of the present study was to seek theoretical confirmation that <span class="hlt">pressure</span> <span class="hlt">waves</span> are able to travel quickly enough to account for the seismic and hydrological observations documented. This confirmation was sought through a transient one-dimensional numerical solution to the differential fluid mass conservation equation for an elastic porous medium. Results of the numerical simulations show that when overpressures at depths greater than 2 km in the décollement exceed lithostatic <span class="hlt">pressure</span> by at least 3%, <span class="hlt">pressure</span> <span class="hlt">waves</span> are formed that migrate up-dip at rates fast enough to account for aseismic slip over a broad range of geologic conditions. <span class="hlt">Pressure</span> <span class="hlt">waves</span> spawned from these depths in the décollement may travel fast enough to account for aseismic slip when overpressures there are as low as 99% of lithostatic <span class="hlt">pressure</span>, but require low specific storage of 3×10-6 m-1, high sensitivity of permeability to effective stress, low permeability no higher than about 10-21 m2 at depths below</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>Acoustic propagation operators for <span class="hlt">pressure</span> <span class="hlt">waves</span> 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 acoustic 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> <span class="hlt">waves</span> are measured exhibit some curvature. In this paper we derive a theoretically rigorous way of building propagation operators for <span class="hlt">pressure</span> <span class="hlt">waves</span> 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> <span class="hlt">waves</span> 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://hdl.handle.net/2060/20100011237','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100011237"><span><span class="hlt">Portable</span> Unit for Metabolic Analysis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dietrich, Daniel L.; Pitch, Nancy D.; Lewis, Mark E.; Juergens, Jeffrey R.; Lichter, Michael J.; Stuk, Peter M.; Diedrick, Dale M.; Valentine, Russell W.; Pettegrew, Richard D.</p> <p>2007-01-01</p> <p>The <span class="hlt">Portable</span> Unit for Metabolic Analysis (PUMA) is an instrument that measures several quantities indicative of human metabolic function. Specifically, this instrument makes time-resolved measurements of temperature, <span class="hlt">pressure</span>, flow, and the partial <span class="hlt">pressures</span> of oxygen and carbon dioxide in breath during both inhalation and exhalation. <span class="hlt">Portable</span> instruments for measuring these quantities have been commercially available, but the response times of those instruments are too long to enable temporal resolution of phenomena on the time scales of human respiration cycles. In contrast, the response time of the PUMA is significantly shorter than characteristic times of human respiration phenomena, making it possible to analyze varying metabolic parameters, not only on sequential breath cycles but also at successive phases of inhalation and exhalation within the same breath cycle. In operation, the PUMA is positioned to sample breath near the subject s mouth. Commercial off-the-shelf sensors are used for three of the measurements: a miniature <span class="hlt">pressure</span> transducer for <span class="hlt">pressure</span>, a thermistor for temperature, and an ultrasonic sensor for flow. Sensors developed at Glenn Research Center are used for measuring the partial <span class="hlt">pressures</span> of oxygen and carbon dioxide: The carbon dioxide sensor exploits the relatively strong absorption of infrared light by carbon dioxide. Light from an infrared source passes through the stream of inhaled or exhaled gas and is focused on an infrared- sensitive photodetector. The oxygen sensor exploits the effect of oxygen in quenching the fluorescence of ruthenium-doped organic molecules in a dye on the tip of an optical fiber. A blue laser diode is used to excite the fluorescence, and the optical fiber carries the fluorescent light to a photodiode, the temporal variation of the output of which bears a known relationship with the rate of quenching of fluorescence and, hence, with the partial <span class="hlt">pressure</span> of oxygen. The outputs of the sensors are digitized</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/2911086','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/2911086"><span><span class="hlt">Pressure</span> <span class="hlt">wave</span> injuries to rat dorsal root ganglion cells in culture caused by high-energy missiles.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Suneson, A; Hansson, H A; Lycke, E; Seeman, T</p> <p>1989-01-01</p> <p>A high-energy missile impact in an extremity of an animal creates a shock <span class="hlt">wave</span> which is rapidly dispersed as a burst of oscillating <span class="hlt">pressure</span> <span class="hlt">waves</span> that traverses the entire body causing local, regional, and distant injuries. The present study was performed on dorsal root ganglion (DRG) cells, cultured for 3 weeks, to elucidate the cellular mechanism for damage of nerve cells, using a simplified test system. A model system was developed allowing exposure of DRG cultures to a burst of high-frequency oscillating <span class="hlt">pressure</span> <span class="hlt">waves</span>, comparable to those recorded in animals after high-energy missile extremity impact. The <span class="hlt">pressure</span> <span class="hlt">waves</span> were induced by impact of a high-energy missile in a rubber tube filled with water, in which nerve cell cultures were kept in a closed rubber glove filled with tissue culture medium. The <span class="hlt">pressure</span> <span class="hlt">waves</span> had a duration of 0.5-1.5 ms and a frequency spectrum ranging from 0-250 kHz. Within minutes the neurites showed changes in their microtubules. In addition, varicosities, enriched with tubulin immunoreactive material, became irregularly studded along the nerve cell processes. Scattered DRG cells were initially permeable to the marker complex Evans-blue albumin (EBA), used as an indicator of the ability of the plasma membranes to exclude proteins. After 6 hr, however, almost every DRG neuron was intensely stained by EBA. Concomitantly, there was swelling of the nerve cell cytoplasm and organelles, and, to a variable extent, neurofilament tangles were observed.(ABSTRACT TRUNCATED AT 250 WORDS)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMMR13A2242H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMMR13A2242H"><span>Influence of Pore-Fluid <span class="hlt">Pressure</span> on Elastic <span class="hlt">Wave</span> Velocity and Electrical Conductivity in Water-Saturated Rocks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Higuchi, A.; Watanabe, T.</p> <p>2013-12-01</p> <p>Pore-fluid <span class="hlt">pressure</span> in seismogenic zones can play a key role in the occurrence of earthquakes (e.g., Sibson, 2009). Its evaluation via geophysical observations can lead to a good understanding of seismic activities. The evaluation requires a thorough understanding of the influence of the pore-fluid <span class="hlt">pressure</span> on geophysical observables like seismic velocity and electrical conductivity. We have studied the influence of pore-fluid <span class="hlt">pressure</span> on elastic <span class="hlt">wave</span> velocity and electrical conductivity in water-saturated rocks. Fine grained (100-500μm) biotite granite (Aji, Kagawa pref., Japan) was used as rock samples. The density is 2.658-2.668 g/cm3, and the porosity 0.68-0.87%. The sample is composed of 52.8% plagioclase, 36.0% Quartz, 3.0% K-feldspar, 8.2% biotite. SEM images show that a lot of grain boundaries are open. Few intracrystalline cracks were observed. Following the method proposed by David and Zimmerman (2012), the distribution function of crack aspect ratio was evaluated from the <span class="hlt">pressure</span> dependence of compressional and shear <span class="hlt">wave</span> velocities in a dry sample. Cylindrical sample has dimensions of 25 mm in diameter and 30 mm in length, and saturated with 0.01 mol/l KCl aqueous solution. Compressional and shear <span class="hlt">wave</span> velocities were measured with the pulse transmission technique (PZT transducers, f=2 MHz), and electrical conductivity the two-electrode method (Ag-AgCl electrodes, f=1 Hz-100 kHz). Simultaneous measurements of velocities and conductivity were made using a 200 MPa hydrostatic <span class="hlt">pressure</span> vessel, in which confining and pore-fluid <span class="hlt">pressures</span> can be separately controlled. The pore-fluid is electrically insulated from the metal work of the <span class="hlt">pressure</span> vessel by using a newly designed plastic device (Watanabe and Higuchi, 2013). The confining <span class="hlt">pressure</span> was progressively increased up to 25 MPa, while the pore-fluid <span class="hlt">pressure</span> was kept at 0.1 MPa. It took five days or longer for the electrical conductivity to become stationary after increasing the confining <span class="hlt">pressure</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27388527','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27388527"><span>Changes in Central Aortic <span class="hlt">Pressure</span> Levels, <span class="hlt">Wave</span> Components and Determinants Associated with High Peripheral Blood <span class="hlt">Pressure</span> States in Childhood: Analysis of Hypertensive Phenotype.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>García-Espinosa, Victoria; Curcio, Santiago; Marotta, Marco; Castro, Juan M; Arana, Maite; Peluso, Gonzalo; Chiesa, Pedro; Giachetto, Gustavo; Bia, Daniel; Zócalo, Yanina</p> <p>2016-10-01</p> <p>The aims were to determine whether children's high peripheral blood <span class="hlt">pressure</span> states (HBP) are associated with increased central aortic blood <span class="hlt">pressure</span> (BP) and to characterize hemodynamic and vascular changes associated with HBP in terms of changes in cardiac output (stroke volume, SV), arterial stiffness (aortic pulse <span class="hlt">wave</span> velocity, PWV), peripheral vascular resistances (PVR) and net and relative contributions of reflected <span class="hlt">waves</span> to the aortic pulse amplitude. We included 154 subjects (mean age 11; range 4-16 years) assigned to one of two groups: normal peripheral BP (NBP, n = 101), defined as systolic and diastolic BP < 90th percentile, or high BP (HBP, n = 53), defined as average systolic and/or diastolic BP levels ≥90th percentile (curves for sex, age and body height). The HBP group included children with hypertensive and pre-hypertensive BP levels. After a first analysis, groups were compared excluding obese and dyslipidemic children. Peripheral and central aortic BP, PWV and pulse <span class="hlt">wave</span>-derived parameters (augmentation index, forward and backward <span class="hlt">wave</span> components' amplitude) were measured using gold-standard techniques, applanation tonometry (SphygmoCor) and oscillometry (Mobil-O-Graph). Independent of the presence of dyslipidemia and/or obesity, aortic systolic and pulse BP were higher in HBP than in NBP children. The increase in central BP could not be explained by an increase in the relative contribution of reflections to the aortic <span class="hlt">pressure</span> <span class="hlt">wave</span>, higher PVR or by an augmented peripheral reflection coefficient. Instead, the rise in central BP would be explained by an increase in the amplitude of both incident and reflected <span class="hlt">wave</span> components.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AIPC..955.1186O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AIPC..955.1186O"><span>New Experimental Capabilities and Theoretical Insights of High <span class="hlt">Pressure</span> Compression <span class="hlt">Waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Orlikowski, Daniel; Nguyen, Jeffrey H.; Patterson, J. Reed; Minich, Roger; Martin, L. Peter; Holmes, Neil C.</p> <p>2007-12-01</p> <p>Currently there are three platforms that offer quasi-isentropic compression or ramp-<span class="hlt">wave</span> compression (RWC): light-gas gun, magnetic flux (Z-pinch), and laser. We focus here on the light-gas gun technique and on some current theoretical insights from experimental data. An impedance gradient through the length of the impactor provides the <span class="hlt">pressure</span> pulse upon impact to the subject material. Applications and results are given concerning high-<span class="hlt">pressure</span> strength and the liquid-to-solid, phase transition of water giving its first associated phase fraction history. We also introduce the Korteweg-deVries-Burgers equation as a means to understand the evolution of these RWC <span class="hlt">waves</span> as they propagate through the thickness of the subject material. This model equation has the necessary competition between non-linear, dispersion, and dissipation processes, which is shown through observed structures that are manifested in the experimental particle velocity histories. Such methodology points towards a possibility of quantifying dissipation, through which RWC experiments may be analyzed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24158293','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24158293"><span>Experimental study on the <span class="hlt">pressure</span> and pulse <span class="hlt">wave</span> propagation in viscoelastic vessel tubes-effects of liquid viscosity and tube stiffness.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ikenaga, Yuki; Nishi, Shohei; Komagata, Yuka; Saito, Masashi; Lagrée, Pierre-Yves; Asada, Takaaki; Matsukawa, Mami</p> <p>2013-11-01</p> <p>A pulse <span class="hlt">wave</span> is the displacement <span class="hlt">wave</span> which arises because of ejection of blood from the heart and reflection at vascular bed and distal point. The investigation of <span class="hlt">pressure</span> <span class="hlt">waves</span> leads to understanding the propagation characteristics of a pulse <span class="hlt">wave</span>. To investigate the pulse <span class="hlt">wave</span> behavior, an experimental study was performed using an artificial polymer tube and viscous liquid. A polyurethane tube and glycerin solution were used to simulate a blood vessel and blood, respectively. In the case of the 40 wt% glycerin solution, which corresponds to the viscosity of ordinary blood, the attenuation coefficient of a <span class="hlt">pressure</span> <span class="hlt">wave</span> in the tube decreased from 4.3 to 1.6 dB/m because of the tube stiffness (Young's modulus: 60 to 200 kPa). When the viscosity of liquid increased from approximately 4 to 10 mPa·s (the range of human blood viscosity) in the stiff tube, the attenuation coefficient of the <span class="hlt">pressure</span> <span class="hlt">wave</span> changed from 1.6 to 3.2 dB/m. The hardening of the blood vessel caused by aging and the increase of blood viscosity caused by illness possibly have opposite effects on the intravascular <span class="hlt">pressure</span> <span class="hlt">wave</span>. The effect of the viscosity of a liquid on the amplitude of a <span class="hlt">pressure</span> <span class="hlt">wave</span> was then considered using a phantom simulating human blood vessels. As a result, in the typical range of blood viscosity, the amplitude ratio of the <span class="hlt">waves</span> obtained by the experiments with water and glycerin solution became 1:0.83. In comparison with clinical data, this value is much smaller than that seen from blood vessel hardening. Thus, it can be concluded that the blood viscosity seldom affects the attenuation of a pulse <span class="hlt">wave</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16011801','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16011801"><span>Smart <span class="hlt">portable</span> rehabilitation devices.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mavroidis, Constantinos; Nikitczuk, Jason; Weinberg, Brian; Danaher, Gil; Jensen, Katherine; Pelletier, Philip; Prugnarola, Jennifer; Stuart, Ryan; Arango, Roberto; Leahey, Matt; Pavone, Robert; Provo, Andrew; Yasevac, Dan</p> <p>2005-07-12</p> <p>The majority of current <span class="hlt">portable</span> orthotic devices and rehabilitative braces provide stability, apply precise <span class="hlt">pressure</span>, or help maintain alignment of the joints with out the capability for real time monitoring of the patient's motions and forces and without the ability for real time adjustments of the applied forces and motions. Improved technology has allowed for advancements where these devices can be designed to apply a form of tension to resist motion of the joint. These devices induce quicker recovery and are more effective at restoring proper biomechanics and improving muscle function. However, their shortcoming is in their inability to be adjusted in real-time, which is the most ideal form of a device for rehabilitation. This introduces a second class of devices beyond passive orthotics. It is comprised of "active" or powered devices, and although more complicated in design, they are definitely the most versatile. An active or powered orthotic, usually employs some type of actuator(s). In this paper we present several new advancements in the area of smart rehabilitation devices that have been developed by the Northeastern University Robotics and Mechatronics Laboratory. They are all compact, wearable and <span class="hlt">portable</span> devices and boast re-programmable, real time computer controlled functions as the central theme behind their operation. The sensory information and computer control of the three described devices make for highly efficient and versatile systems that represent a whole new breed in wearable rehabilitation devices. Their applications range from active-assistive rehabilitation to resistance exercise and even have applications in gait training. The three devices described are: a transportable continuous passive motion elbow device, a wearable electro-rheological fluid based knee resistance device, and a wearable electrical stimulation and biofeedback knee device. Laboratory tests of the devices demonstrated that they were able to meet their design</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1180467','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1180467"><span>Smart <span class="hlt">portable</span> rehabilitation devices</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Mavroidis, Constantinos; Nikitczuk, Jason; Weinberg, Brian; Danaher, Gil; Jensen, Katherine; Pelletier, Philip; Prugnarola, Jennifer; Stuart, Ryan; Arango, Roberto; Leahey, Matt; Pavone, Robert; Provo, Andrew; Yasevac, Dan</p> <p>2005-01-01</p> <p>Background The majority of current <span class="hlt">portable</span> orthotic devices and rehabilitative braces provide stability, apply precise <span class="hlt">pressure</span>, or help maintain alignment of the joints with out the capability for real time monitoring of the patient's motions and forces and without the ability for real time adjustments of the applied forces and motions. Improved technology has allowed for advancements where these devices can be designed to apply a form of tension to resist motion of the joint. These devices induce quicker recovery and are more effective at restoring proper biomechanics and improving muscle function. However, their shortcoming is in their inability to be adjusted in real-time, which is the most ideal form of a device for rehabilitation. This introduces a second class of devices beyond passive orthotics. It is comprised of "active" or powered devices, and although more complicated in design, they are definitely the most versatile. An active or powered orthotic, usually employs some type of actuator(s). Methods In this paper we present several new advancements in the area of smart rehabilitation devices that have been developed by the Northeastern University Robotics and Mechatronics Laboratory. They are all compact, wearable and <span class="hlt">portable</span> devices and boast re-programmable, real time computer controlled functions as the central theme behind their operation. The sensory information and computer control of the three described devices make for highly efficient and versatile systems that represent a whole new breed in wearable rehabilitation devices. Their applications range from active-assistive rehabilitation to resistance exercise and even have applications in gait training. The three devices described are: a transportable continuous passive motion elbow device, a wearable electro-rheological fluid based knee resistance device, and a wearable electrical stimulation and biofeedback knee device. Results Laboratory tests of the devices demonstrated that they were able to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040141697&hterms=Diabetes&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DDiabetes','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040141697&hterms=Diabetes&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DDiabetes"><span>Patients' choice of <span class="hlt">portable</span> folding chairs to reduce symptoms of orthostatic hypotension</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Smit, A. A.; Wieling, W.; Opfer-Gehrking, T. L.; van Emmerik-Levelt, H. M.; Low, P. A.</p> <p>1999-01-01</p> <p>Patients with neurogenic orthostatic hypotension may use <span class="hlt">portable</span> folding chairs to prevent or reduce symptoms of low blood <span class="hlt">pressure</span>. However, a concomitant movement disorder may limit the use of these chairs in daily living. In this prospective study, 13 patients with orthostatic hypotension, balance disturbance associated with motor disability, or both examined three commercially available <span class="hlt">portable</span> folding chairs. A questionnaire was used to document the characteristics in chair design that were relevant for satisfactory use to these patients. Armrests, seat width, and an adjustable sitting height were found to be important features of a <span class="hlt">portable</span> folding chair. One chair was selected by 11 of 13 patients to fit most needs.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_9 --> <div id="page_10" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="181"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/526572','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/526572"><span>A <span class="hlt">portable</span> smoking pattern recorder.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Creighton, D E; Noble, M J; Whewell, R T</p> <p>1979-01-01</p> <p>An instrument has been developed which can be used to record the smoking patterns of human smokers in almost any location. The smoker is required to smoke the cigarette through an orifice plate cigarette holder connected to the recorder. The smoking pattern data are recorded onto a standard audio cassette as <span class="hlt">pressure</span> and flow signals together with timing impulses and speech. The instrument is battery powered and can be built into a small brief case. The four channels of data are decoded on a separate instrument, which uses the timing signals to synchronise a data logger, thus making the whole system independent of tape speed errors. The speech channel is used to identify the smoker, cigarette, location, etc. Comparisons have been made of the performance of the <span class="hlt">portable</span> recorder and a laboratory smoking analyser and data logger. It was found that data decoded from the <span class="hlt">portable</span> recorder are generally within 1% of the values recorded directly on the laboratory instrument.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014CEJE....4..110G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014CEJE....4..110G"><span>Internal combustion engine supercharging: turbocharger vs. <span class="hlt">pressure</span> <span class="hlt">wave</span> compressor. Performance comparison</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>George, Atanasiu Catalin; Chiru, Anghel</p> <p>2014-06-01</p> <p>This paper aims on comparison between a turbocharged engine and a <span class="hlt">pressure</span> <span class="hlt">wave</span> charged engine. The comparison was accomplished using the engine simulation software AVL Boost, version 2010. The grahps were extracted using AVL Impress, version 2010. The performance increase is limited by the mechanical side of the simulated engine.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title49-vol2/pdf/CFR-2010-title49-vol2-sec178-255-12.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title49-vol2/pdf/CFR-2010-title49-vol2-sec178-255-12.pdf"><span>49 CFR 178.255-12 - <span class="hlt">Pressure</span> test.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... Specifications for <span class="hlt">Portable</span> Tanks § 178.255-12 <span class="hlt">Pressure</span> test. (a) Each completed <span class="hlt">portable</span> tank prior to application of lining shall be tested before being put into transportation service by completely filling the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040004324','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040004324"><span>Investigation of <span class="hlt">Pressurized</span> <span class="hlt">Wave</span> Bearings</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Keith, Theo G., Jr.; Dimofte, Florin</p> <p>2003-01-01</p> <p>The <span class="hlt">wave</span> bearing has been pioneered and developed by Dr. Dimofte over the past several years. This bearing will be the main focus of this research. It is believed that the <span class="hlt">wave</span> bearing offers a number of advantages over the foil bearing, which is the bearing that NASA is currently pursuing for turbomachinery applications. The <span class="hlt">wave</span> bearing is basically a journal bearing whose film thickness varies around the circumference approximately sinusoidally, with usually 3 or 4 <span class="hlt">waves</span>. Being a rigid geometry bearing, it provides precise control of shaft centerlines. The <span class="hlt">wave</span> profile also provides good load capacity and makes the bearing very stable. Manufacturing techniques have been devised that should allow the production of <span class="hlt">wave</span> bearings almost as cheaply as conventional full-circular bearings.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoRL..44.1384C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoRL..44.1384C"><span>A new climate index controlling winter <span class="hlt">wave</span> activity along the Atlantic coast of Europe: The West Europe <span class="hlt">Pressure</span> Anomaly</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Castelle, Bruno; Dodet, Guillaume; Masselink, Gerd; Scott, Tim</p> <p>2017-02-01</p> <p>A pioneering and replicable method based on a 66-year numerical weather and <span class="hlt">wave</span> hindcast is developed to optimize a climate index based on the sea level <span class="hlt">pressure</span> (SLP) that best explains winter <span class="hlt">wave</span> height variability along the coast of western Europe, from Portugal to UK (36-52°N). The resulting so-called Western Europe <span class="hlt">Pressure</span> Anomaly (WEPA) is based on the sea level <span class="hlt">pressure</span> gradient between the stations Valentia (Ireland) and Santa Cruz de Tenerife (Canary Islands). The WEPA positive phase reflects an intensified and southward shifted SLP difference between the Icelandic low and the Azores high, driving severe storms that funnel high-energy <span class="hlt">waves</span> toward western Europe southward of 52°N. WEPA outscores by 25-150% the other leading atmospheric modes in explaining winter-averaged significant <span class="hlt">wave</span> height, and even by a largest amount the winter-averaged extreme <span class="hlt">wave</span> heights. WEPA is also the only index capturing the 2013/2014 extreme winter that caused widespread coastal erosion and flooding in western Europe.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22490925-effect-anisotropic-dust-pressure-superthermal-electrons-propagation-stability-dust-acoustic-solitary-waves','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22490925-effect-anisotropic-dust-pressure-superthermal-electrons-propagation-stability-dust-acoustic-solitary-waves"><span>Effect of anisotropic dust <span class="hlt">pressure</span> and superthermal electrons on propagation and stability of dust acoustic solitary <span class="hlt">waves</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>Bashir, M. F., E-mail: frazbashir@yahoo.com; Behery, E. E., E-mail: eebehery@gmail.com; Department of Physics, Faculty of Science, Damietta University, P.O. 34517, New Damietta</p> <p>2015-06-15</p> <p>Employing the reductive perturbation technique, Zakharov–Kuznetzov (ZK) equation is derived for dust acoustic (DA) solitary <span class="hlt">waves</span> in a magnetized plasma which consists the effects of dust anisotropic <span class="hlt">pressure</span>, arbitrary charged dust particles, Boltzmann distributed ions, and Kappa distributed superthermal electrons. The ZK solitary <span class="hlt">wave</span> solution is obtained. Using the small-k expansion method, the stability analysis for DA solitary <span class="hlt">waves</span> is also discussed. The effects of the dust <span class="hlt">pressure</span> anisotropy and the electron superthermality on the basic characteristics of DA <span class="hlt">waves</span> as well as on the three-dimensional instability criterion are highlighted. It is found that the DA solitary <span class="hlt">wave</span> is rarefactivemore » (compressive) for negative (positive) dust. In addition, the growth rate of instability increases rapidly as the superthermal spectral index of electrons increases with either positive or negative dust grains. A brief discussion for possible applications is included.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhTea..54..118M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhTea..54..118M"><span>Tunnel <span class="hlt">pressure</span> <span class="hlt">waves</span> - A smartphone inquiry on rail travel</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Müller, Andreas; Hirth, Michael; Kuhn, Jochen</p> <p>2016-02-01</p> <p>When traveling by rail, you might have experienced the following phenomenon: The train enters a tunnel, and after some seconds a noticeable <span class="hlt">pressure</span> change occurs, as perceived by your ears or even by a rapid wobbling of the train windows. The basic physics is that <span class="hlt">pressure</span> <span class="hlt">waves</span> created by the train travel down the tunnel, are reflected at its other end, and travel back until they meet the train again. Here we will show (i) how this effect can be well understood as a kind of large-scale outdoor case of a textbook paradigm, and (ii) how, e.g., a prediction of the tunnel length from the inside of a moving train on the basis of this model can be validated by means of a mobile phone measurement.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvF...3e3904B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvF...3e3904B"><span>Instability <span class="hlt">waves</span> and transition in adverse-<span class="hlt">pressure</span>-gradient boundary layers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bose, Rikhi; Zaki, Tamer A.; Durbin, Paul A.</p> <p>2018-05-01</p> <p>Transition to turbulence in incompressible adverse-<span class="hlt">pressure</span>-gradient (APG) boundary layers is investigated by direct numerical simulations. Purely two-dimensional instability <span class="hlt">waves</span> develop on the inflectional base velocity profile. When the boundary layer is perturbed by isotropic turbulence from the free stream, streamwise elongated streaks form and may interact with the instability <span class="hlt">waves</span>. Subsequent mechanisms that trigger transition depend on the intensity of the free-stream disturbances. All evidence from the present simulations suggest that the growth rate of instability <span class="hlt">waves</span> is sufficiently high to couple with the streaks. Under very low levels of free-stream turbulence (˜0.1 % ), transition onset is highly sensitive to the inlet disturbance spectrum and is accelerated if the spectrum contains frequency-<span class="hlt">wave</span>-number combinations that are commensurate with the instability <span class="hlt">waves</span>. Transition onset and completion in this regime is characterized by formation and breakdown of Λ vortices, but they are more sporadic than in natural transition. Beneath free-stream turbulence with higher intensity (1-2 % ), bypass transition mechanisms are dominant, but instability <span class="hlt">waves</span> are still the most dominant disturbances in wall-normal and spanwise perturbation spectra. Most of the breakdowns were by disturbances with critical layers close to the wall, corresponding to inner modes. On the other hand, the propensity of an outer mode to occur increases with the free-stream turbulence level. Higher intensity free-stream disturbances induce strong streaks that favorably distort the boundary layer and suppress the growth of instability <span class="hlt">waves</span>. But the upward displacement of high amplitude streaks brings them to the outer edge of the boundary layer and exposes them to ambient turbulence. Consequently, high-amplitude streaks exhibit an outer-mode secondary instability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19840025864&hterms=flower&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dflower','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19840025864&hterms=flower&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dflower"><span>Experimental validation of a millimeter <span class="hlt">wave</span> radar technique to remotely sense atmospheric <span class="hlt">pressure</span> at the Earth's surface</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Flower, D. A.; Peckham, G. E.; Bradford, W. J.</p> <p>1984-01-01</p> <p>Experiments with a millimeter <span class="hlt">wave</span> radar operating on the NASA CV-990 aircraft which validate the technique for remotely sensing atmospheric <span class="hlt">pressure</span> at the Earth's surface are described. Measurements show that the precise millimeter <span class="hlt">wave</span> observations needed to deduce <span class="hlt">pressure</span> from space with an accuracy of 1 mb are possible, that sea surface reflection properties agree with theory and that the measured variation of differential absorption with altitude corresponds to that expected from spectroscopic models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20020091962','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20020091962"><span><span class="hlt">Portable</span> Welder</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1984-01-01</p> <p>A low cost, low power, self-contained <span class="hlt">portable</span> welding gun designed for joining thermoplastics which become soft when heated and harden when cooled was developed originally by NASA's Langley Research Center for repairing helicopter windshields. Welder has a broad range of applications for joining both thermoplastic materials in the aerospace, automotive, appliance, and construction industries. Welders <span class="hlt">portability</span> and low power requirement allow its use on-site in any type of climate, with power supplied by a variety of <span class="hlt">portable</span> sources.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22492644-cavitation-inception-backscattering-pressure-waves-from-bubble-interface','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22492644-cavitation-inception-backscattering-pressure-waves-from-bubble-interface"><span>Cavitation inception by the backscattering of <span class="hlt">pressure</span> <span class="hlt">waves</span> from a bubble interface</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>Takahira, Hiroyuki, E-mail: takahira@me.osakafu-u.ac.jp; Ogasawara, Toshiyuki, E-mail: oga@me.osakafu-u.ac.jp; Mori, Naoto, E-mail: su101064@edu.osakafu-u.ac.jp</p> <p>2015-10-28</p> <p>The secondary cavitation that occurs by the backscattering of focused ultrasound from a primary cavitation bubble caused by the negative <span class="hlt">pressure</span> part of the ultrasound (Maxwell, et al., 2011) might be useful for the energy exchange due to bubble oscillations in High Intensity Focused Ultrasound (HIFU). The present study is concerned with the cavitation inception by the backscattering of ultrasound from a bubble. In the present experiment, a laser-induced bubble which is generated by a pulsed focused laser beam with high intensity is utilized as a primary cavitation bubble. After generating the bubble, focused ultrasound is emitted to the bubble.more » The acoustic field and the bubble motion are observed with a high-speed video camera. It is confirmed that the secondary cavitation bubble clouds are generated by the backscattering from the laser-induced bubble. The growth of cavitation bubble clouds is analyzed with the image processing method. The experimental results show that the height and width of the bubble clouds grow in stepwise during their evolution. The direct numerical simulations are also conducted for the backscattering of incident <span class="hlt">pressure</span> <span class="hlt">waves</span> from a bubble in order to evaluate a <span class="hlt">pressure</span> field near the bubble. It is shown that the ratio of a bubble collapse time t{sub 0} to a characteristic time of <span class="hlt">wave</span> propagation t{sub S}, η = t{sub 0}/t{sub s}, is an important determinant for generating negative <span class="hlt">pressure</span> region by backscattering. The minimum <span class="hlt">pressure</span> location by the backscattering in simulations is in good agreement with the experiment.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/EJ1103434.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/EJ1103434.pdf"><span>Communicating <span class="hlt">Wave</span> Energy: An Active Learning Experience for Students</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Huynh, Trongnghia; Hou, Gene; Wang, Jin</p> <p>2016-01-01</p> <p>We have conducted an education project to communicate the <span class="hlt">wave</span> energy concept to high school students. A virtual reality system that combines both hardware and software is developed in this project to simulate the buoy-<span class="hlt">wave</span> interaction. This first-of-its-kind <span class="hlt">wave</span> energy unit is <span class="hlt">portable</span> and physics-based, allowing students to conduct a number of…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AIPC.1592..341C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AIPC.1592..341C"><span>Investigation on the generation characteristic of <span class="hlt">pressure</span> pulse <span class="hlt">wave</span> signal during the measurement-while-drilling process</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Changqing, Zhao; Kai, Liu; Tong, Zhao; Takei, Masahiro; Weian, Ren</p> <p>2014-04-01</p> <p>The mud-pulse logging instrument is an advanced measurement-while-drilling (MWD) tool and widely used by the industry in the world. In order to improve the signal transmission rate, ensure the accurate transmission of information and address the issue of the weak signal on the ground of oil and gas wells, the signal generator should send out the strong mud-pulse signals with the maximum amplitude. With the rotary valve pulse generator as the study object, the three-dimensional Reynolds NS equations and standard k - ɛ turbulent model were used as a mathematical model. The speed and <span class="hlt">pressure</span> coupling calculation was done by simple algorithms to get the amplitudes of different rates of flow and axial clearances. Tests were done to verify the characteristics of the <span class="hlt">pressure</span> signals. The <span class="hlt">pressure</span> signal was captured by the standpiece <span class="hlt">pressure</span> monitoring system. The study showed that the axial clearances grew bigger as the <span class="hlt">pressure</span> <span class="hlt">wave</span> amplitude value decreased and caused the weakening of the pulse signal. As the rate of flow got larger, the <span class="hlt">pressure</span> <span class="hlt">wave</span> amplitude would increase and the signal would be enhanced.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015OcMod..86...36D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015OcMod..86...36D"><span>A Boussinesq-scaled, <span class="hlt">pressure</span>-Poisson water <span class="hlt">wave</span> model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Donahue, Aaron S.; Zhang, Yao; Kennedy, Andrew B.; Westerink, Joannes J.; Panda, Nishant; Dawson, Clint</p> <p>2015-02-01</p> <p>Through the use of Boussinesq scaling we develop and test a model for resolving non-hydrostatic <span class="hlt">pressure</span> profiles in nonlinear <span class="hlt">wave</span> systems over varying bathymetry. A Green-Nagdhi type polynomial expansion is used to resolve the <span class="hlt">pressure</span> profile along the vertical axis, this is then inserted into the <span class="hlt">pressure</span>-Poisson equation, retaining terms up to a prescribed order and solved using a weighted residual approach. The model shows rapid convergence properties with increasing order of polynomial expansion which can be greatly improved through the application of asymptotic rearrangement. Models of Boussinesq scaling of the fully nonlinear O (μ2) and weakly nonlinear O (μN) are presented, the analytical and numerical properties of O (μ2) and O (μ4) models are discussed. Optimal basis functions in the Green-Nagdhi expansion are determined through manipulation of the free-parameters which arise due to the Boussinesq scaling. The optimal O (μ2) model has dispersion accuracy equivalent to a Padé [2,2] approximation with one extra free-parameter. The optimal O (μ4) model obtains dispersion accuracy equivalent to a Padé [4,4] approximation with two free-parameters which can be used to optimize shoaling or nonlinear properties. In comparison to experimental results the O (μ4) model shows excellent agreement to experimental data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25000237','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25000237"><span>Pizza <span class="hlt">makers</span>' contact dermatitis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lembo, Serena; Lembo, Claudio; Patruno, Cataldo; Balato, Anna; Balato, Nicola; Ayala, Fabio</p> <p>2014-01-01</p> <p>Contact eczema to foods, spices, and food additives can occur in occupational and nonoccupational settings in those who grow, handle, prepare, or cook food. Pizza is one of the most eaten foods in every continent, and pizza making is a common work in many countries. We aimed to evaluate the occurrence and the causes of contact dermatitis in pizza <span class="hlt">makers</span> in Naples. We performed an observational study in 45 pizza <span class="hlt">makers</span>: all the enrolled subjects had to answer a questionnaire designed to detect personal history of respiratory or cutaneous allergy, atopy; work characteristics and timing were also investigated. Every subject attended the dermatology clinic for a complete skin examination, and when needed, patients were patch tested using the Italian baseline series of haptens integrated with an arbitrary pizza <span class="hlt">makers</span> series. Our results reported that 13.3% of the enrolled pizza <span class="hlt">makers</span> (6/45) presented hand eczema, and that 8.9% (4/45) were affected by occupational allergic contact dermatitis. Diallyl disulfide and ammonium persulfate were the responsible substances. Performing patch tests in pizza <span class="hlt">makers</span> and food handlers affected by hand contact dermatitis is useful. We propose a specific series of haptens for this wide working category.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5508003','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5508003"><span>Defects in Vascular Mechanics Due to Aging in Rats: Studies on Arterial <span class="hlt">Wave</span> Properties from a Single Aortic <span class="hlt">Pressure</span> Pulse</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Chang, Chun-Yi; Chang, Ru-Wen; Hsu, Shu-Hsien; Wu, Ming-Shiou; Cheng, Ya-Jung; Kao, Hsien-Li; Lai, Liang-Chuan; Wang, Chih-Hsien; Chang, Kuo-Chu</p> <p>2017-01-01</p> <p>Changes in vascular mechanics due to aging include elevated vascular impedance, diminished aorta distensibility, and an accelerated return of pulse <span class="hlt">wave</span> reflection, which may increase the systolic workload on the heart. Classically, the accurate measurement of vascular mechanics requires the simultaneous recording of aortic <span class="hlt">pressure</span> and flow signals. In practice, it is feasible to estimate arterial <span class="hlt">wave</span> properties in terms of <span class="hlt">wave</span> transit time (τw) and <span class="hlt">wave</span> reflection index (RI) by using aortic <span class="hlt">pressure</span> signal alone. In this study, we determined the τw and magnitudes of the forward (∣Pf∣) and backward (∣Pb∣) <span class="hlt">pressure</span> <span class="hlt">waves</span> in Long–Evans male rats aged 4 (n = 14), 6 (n = 17), 12 (n = 17), and 18 (n = 24) months, based on the measured aortic <span class="hlt">pressure</span> and an assumed triangular flow (Qtri). The pulsatile <span class="hlt">pressure</span> <span class="hlt">wave</span> was the only signal recorded in the ascending aorta by using a high-fidelity <span class="hlt">pressure</span> sensor. The base of the unknown Qtri was constructed using a duration, which equals to the ejection time. The timing at the peak of the triangle was derived using the fourth-order derivative of the aortic <span class="hlt">pressure</span> waveform. In the 18-month-old rats, the ratio of τw to left ventricular ejection time (LVET) decreased, indicating a decline in the distensibility of the aorta. The increased ∣Pb∣ associated with unaltered ∣Pf∣ enhanced the RI in the older rats. The augmentation index (AI) also increased significantly with age. A significant negative correlation between the AI and τw/LVET was observed: AI = −0.7424 − 0.9026 × (τw/LVET) (r = 0.4901; P < 0.0001). By contrast, RI was positively linearly correlated with the AI as follows: AI = −0.4844 + 2.3634 × RI (r = 0.8423; P < 0.0001). Both the decreased τw/LVET and increased RI suggested that the aging process may increase the AI, thereby increasing the systolic hydraulic load on the heart. The novelty of the study is that Qtri is constructed using the measured aortic <span class="hlt">pressure</span> <span class="hlt">wave</span> to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28751867','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28751867"><span>Defects in Vascular Mechanics Due to Aging in Rats: Studies on Arterial <span class="hlt">Wave</span> Properties from a Single Aortic <span class="hlt">Pressure</span> Pulse.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chang, Chun-Yi; Chang, Ru-Wen; Hsu, Shu-Hsien; Wu, Ming-Shiou; Cheng, Ya-Jung; Kao, Hsien-Li; Lai, Liang-Chuan; Wang, Chih-Hsien; Chang, Kuo-Chu</p> <p>2017-01-01</p> <p>Changes in vascular mechanics due to aging include elevated vascular impedance, diminished aorta distensibility, and an accelerated return of pulse <span class="hlt">wave</span> reflection, which may increase the systolic workload on the heart. Classically, the accurate measurement of vascular mechanics requires the simultaneous recording of aortic <span class="hlt">pressure</span> and flow signals. In practice, it is feasible to estimate arterial <span class="hlt">wave</span> properties in terms of <span class="hlt">wave</span> transit time (τ w ) and <span class="hlt">wave</span> reflection index (RI) by using aortic <span class="hlt">pressure</span> signal alone. In this study, we determined the τ w and magnitudes of the forward (∣ P f ∣) and backward (∣ P b ∣) <span class="hlt">pressure</span> <span class="hlt">waves</span> in Long-Evans male rats aged 4 ( n = 14), 6 ( n = 17), 12 ( n = 17), and 18 ( n = 24) months, based on the measured aortic <span class="hlt">pressure</span> and an assumed triangular flow ( Q tri ). The pulsatile <span class="hlt">pressure</span> <span class="hlt">wave</span> was the only signal recorded in the ascending aorta by using a high-fidelity <span class="hlt">pressure</span> sensor. The base of the unknown Q tri was constructed using a duration, which equals to the ejection time. The timing at the peak of the triangle was derived using the fourth-order derivative of the aortic <span class="hlt">pressure</span> waveform. In the 18-month-old rats, the ratio of τ w to left ventricular ejection time (LVET) decreased, indicating a decline in the distensibility of the aorta. The increased ∣ P b ∣ associated with unaltered ∣ P f ∣ enhanced the RI in the older rats. The augmentation index (AI) also increased significantly with age. A significant negative correlation between the AI and τ w /LVET was observed: AI = -0.7424 - 0.9026 × (τ w /LVET) ( r = 0.4901; P < 0.0001). By contrast, RI was positively linearly correlated with the AI as follows: AI = -0.4844 + 2.3634 × RI ( r = 0.8423; P < 0.0001). Both the decreased τ w /LVET and increased RI suggested that the aging process may increase the AI, thereby increasing the systolic hydraulic load on the heart. The novelty of the study is that Q tri is constructed using the measured aortic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/969241','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/969241"><span><span class="hlt">Pressure</span> Dependence of the Charge-Density-<span class="hlt">Wave</span> Gap in Rare-Earth Tri-Tellurides</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>Sacchetti, A.; /Zurich, ETH; Arcangeletti, E.</p> <p>2009-12-14</p> <p>We investigate the <span class="hlt">pressure</span> dependence of the optical properties of CeTe{sub 3}, which exhibits an incommensurate charge-density-<span class="hlt">wave</span> (CDW) state already at 300 K. Our data are collected in the mid-infrared spectral range at room temperature and at <span class="hlt">pressures</span> between 0 and 9 GPa. The energy for the single particle excitation across the CDW gap decreases upon increasing the applied <span class="hlt">pressure</span>, similarly to the chemical <span class="hlt">pressure</span> by rare-earth substitution. The broadening of the bands upon lattice compression removes the perfect nesting condition of the Fermi surface and therefore diminishes the impact of the CDW transition on the electronic properties of RTe{submore » 3}.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5659212','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5659212"><span>Statins: antimicrobial resistance breakers or <span class="hlt">makers</span>?</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Lareu, Ricky R.; Dix, Brett R.; Hughes, Jeffery D.</p> <p>2017-01-01</p> <p>Introduction The repurposing of non-antibiotic drugs as adjuvant antibiotics may help break antimicrobial resistance (AMR). Statins are commonly prescribed worldwide to lower cholesterol. They also possess qualities of AMR “breakers”, namely direct antibacterial activity, synergism with antibiotics, and ability to stimulate the host immune system. However, statins’ role as AMR breakers may be limited. Their current extensive use for cardiovascular protection might result in selective <span class="hlt">pressures</span> for resistance, ironically causing statins to be AMR “makers” instead. This review examines statins’ potential as AMR breakers, probable AMR <span class="hlt">makers</span>, and identifies knowledge gaps in a statin-bacteria-human-environment continuum. The most suitable statin for repurposing is identified, and a mechanism of antibacterial action is postulated based on structure-activity relationship analysis. Methods A literature search using keywords “statin” or “statins” combined with “minimum inhibitory concentration” (MIC) was performed in six databases on 7th April 2017. After screening 793 abstracts, 16 relevant studies were identified. Unrelated studies on drug interactions; antifungal or antiviral properties of statins; and antibacterial properties of mevastatin, cerivastatin, antibiotics, or natural products were excluded. Studies involving only statins currently registered for human use were included. Results Against Gram-positive bacteria, simvastatin generally exerted the greatest antibacterial activity (lowest MIC) compared to atorvastatin, rosuvastatin, and fluvastatin. Against Gram-negative bacteria, atorvastatin generally exhibited similar or slightly better activity compared to simvastatin, but both were more potent than rosuvastatin and fluvastatin. Discussion Statins may serve as AMR breakers by working synergistically with existing topical antibiotics, attenuating virulence factors, boosting human immunity, or aiding in wound healing. It is probable that</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPC.1949k0008S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPC.1949k0008S"><span><span class="hlt">Portable</span> vibro-acoustic testing system for in situ microstructure characterization and metrology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smith, James A.; Nichol, Corrie I.; Zuck, Larry D.; Fatemi, Mostafa</p> <p>2018-04-01</p> <p>There is a need in research reactors like the one at INL to inspect irradiated materials and structures. The goal of this work is to develop a <span class="hlt">portable</span> scanning infrastructure for a material characterization technique called vibro-acoustography (VA) that has been developed by the Idaho National laboratory for nuclear applications to characterize fuel, cladding materials, and structures. The proposed VA technology is based on ultrasound and acoustic <span class="hlt">waves</span>; however, it provides information beyond what is available from the traditional ultrasound techniques and can expand the knowledge on nuclear material characterization and microstructure evolution. This paper will report on the development of a <span class="hlt">portable</span> scanning system that will be set up to characterize materials and components in open water reactors and canals in situ. We will show some initial laboratory results of images generated by vibro-acoustics of surrogate fuel plates and graphite structures and discuss the design of the <span class="hlt">portable</span> system.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_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.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3341626','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3341626"><span>RELATIONS BETWEEN DAIRY FOOD INTAKE AND ARTERIAL STIFFNESS: PULSE <span class="hlt">WAVE</span> VELOCITY AND PULSE <span class="hlt">PRESSURE</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Crichton, Georgina E.; Elias, Merrrill F.; Dore, Gregory A.; Abhayaratna, Walter P.; Robbins, Michael A.</p> <p>2012-01-01</p> <p>Modifiable risk factors, such as diet, are becomingly increasingly important in the management of cardiovascular disease, one of the greatest major causes of death and disease burden. Few studies have examined the role of diet as a possible means of reducing arterial stiffness, as measured by pulse <span class="hlt">wave</span> velocity, an independent predictor of cardiovascular events and all-cause mortality. The aim of this study was to investigate whether dairy food intake is associated with measures of arterial stiffness including carotid-femoral pulse <span class="hlt">wave</span> velocity and pulse <span class="hlt">pressure</span>. A cross-sectional analysis of a subset of the Maine Syracuse Longitudinal Study sample was performed. A linear decrease in pulse <span class="hlt">wave</span> velocity was observed across increasing intakes of dairy food consumption (ranging from never/rarely to daily dairy food intake). The negative linear relationship between pulse <span class="hlt">wave</span> velocity and intake of dairy food was independent of demographic variables, other cardiovascular disease risk factors and nutrition variables. The pattern of results was very similar for pulse <span class="hlt">pressure</span>, while no association between dairy food intake and lipid levels was found. Further intervention studies are needed to ascertain whether dairy food intake may be an appropriate dietary intervention for the attenuation of age-related arterial stiffening and reduction of cardiovascular disease risk. PMID:22431583</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012SPIE.8366E..0DZ','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012SPIE.8366E..0DZ"><span>Rapid prototyping of solar-powered, battery-operated, atmospheric-<span class="hlt">pressure</span>, sugar-cube size microplasma on hybrid, 3D chips for elemental analysis of liquid microsamples using a <span class="hlt">portable</span> optical emission spectrometer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, X.; Karanassios, V.</p> <p>2012-06-01</p> <p>A solar-powered, battery-operated, atmospheric-<span class="hlt">pressure</span>, self-igniting microplasma the size of a sugar-cube developed on a hybrid, 3d-chip is described. Rapid prototyping of the 3d-chip; some fundamental aspects and a brief characterization of its background spectral emission using a <span class="hlt">portable</span>, fiber-optic spectrometer are discussed.</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 acoustic <span class="hlt">waves</span> 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 acoustic <span class="hlt">waves</span> 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 acoustic <span class="hlt">waves</span> 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/2017AGUFMSM51B2454L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM51B2454L"><span>Generation of EMIC <span class="hlt">Waves</span> and Effects on Particle Precipitation During a Solar Wind <span class="hlt">Pressure</span> Intensification with Bz > 0</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lessard, M.; Engebretson, M. J.; Spence, H. E.; Paulson, K. W.; Halford, A. J.; Millan, R. M.; Rodger, C. J.; Hendry, A.</p> <p>2017-12-01</p> <p>During geomagnetic storms, solar wind energy couples to the magnetosphere and drives the generation of electromagnetic ion cyclotron (EMIC) <span class="hlt">waves</span>, which can then scatter energetic electrons and ions from the radiation belts. In the event described in this paper, the interplanetary magnetic field remained northward throughout the duration, a condition unfavorable for solar wind energy coupling through low latitude reconnection. While this resulted in SYM/H remaining positive, <span class="hlt">pressure</span> fluctuations were directly transferred into and then propagated throughout the magnetosphere, generating EMIC <span class="hlt">waves</span> on global scales. The generation mechanism presumably involved the development of temperature anisotropies via perpendicular <span class="hlt">pressure</span> perturbations, as evidenced by strong correlations between the <span class="hlt">pressure</span> variations and the intensifications of the <span class="hlt">waves</span> globally. Electron precipitation was recorded by the BARREL balloons, although it did not have the same widespread signatures as the <span class="hlt">waves</span> and, in fact, appears to have been quite patchy in character. Observations from Van Allen Probe-A (RBSP-A) satellite (at post midnight local time), showed clear butterfly distributions and it may be possible that the EMIC <span class="hlt">waves</span> contributed to the development of these distribution functions. Ion precipitation was also recorded by the Polar-orbiting Operational Environmental Satellite (POES) satellites, though tended to be confined to the dawn-dusk meridians.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/866800','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/866800"><span>Instantaneous and efficient surface <span class="hlt">wave</span> excitation of a low <span class="hlt">pressure</span> gas or gases</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Levy, Donald J.; Berman, Samuel M.</p> <p>1988-01-01</p> <p>A system for instantaneously ionizing and continuously delivering energy in the form of surface <span class="hlt">waves</span> to a low <span class="hlt">pressure</span> gas or mixture of low <span class="hlt">pressure</span> gases, comprising a source of rf energy, a discharge container, (such as a fluorescent lamp discharge tube), an rf shield, and a coupling device responsive to rf energy from the source to couple rf energy directly and efficiently to the gas or mixture of gases to ionize at least a portion of the gas or gases and to provide energy to the gas or gases in the form of surface <span class="hlt">waves</span>. The majority of the rf power is transferred to the gas or gases near the inner surface of the discharge container to efficiently transfer rf energy as excitation energy for at least one of the gases. The most important use of the invention is to provide more efficient fluorescent and/or ultraviolet lamps.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA095342','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA095342"><span>Charge Design Considerations and Their Effect on <span class="hlt">Pressure</span> <span class="hlt">Waves</span> in Guns</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1980-12-01</p> <p>Interior Ballistic Analysis of Guns", "Interior Ballistics of Guns Ed, M. Summerfield and H. Krier, Progress in Astro - nautics and Aeronautics, Vol. 66...8217 • - -O.8 - Fx " • 0.48 S0.2 U G 00 2 4 64_ . -APi (kpsi) Figure 28. Distribution of <span class="hlt">Pressure-Wave</span> Amplitudes f r the 175-mm, M107 Gun (M86A2, Zone 3</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19970010414','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19970010414"><span><span class="hlt">Wave</span> Engine Topping Cycle Assessment</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Welch, Gerard E.</p> <p>1996-01-01</p> <p>The performance benefits derived by topping a gas turbine engine with a <span class="hlt">wave</span> engine are assessed. The <span class="hlt">wave</span> engine is a <span class="hlt">wave</span> rotor that produces shaft power by exploiting gas dynamic energy exchange and flow turning. The <span class="hlt">wave</span> engine is added to the baseline turboshaft engine while keeping high-<span class="hlt">pressure</span>-turbine inlet conditions, compressor <span class="hlt">pressure</span> ratio, engine mass flow rate, and cooling flow fractions fixed. Related work has focused on topping with <span class="hlt">pressure</span>-exchangers (i.e., <span class="hlt">wave</span> rotors that provide <span class="hlt">pressure</span> gain with zero net shaft power output); however, more energy can be added to a <span class="hlt">wave</span>-engine-topped cycle leading to greater engine specific-power-enhancement The energy addition occurs at a lower <span class="hlt">pressure</span> in the <span class="hlt">wave</span>-engine-topped cycle; thus the specific-fuel-consumption-enhancement effected by ideal <span class="hlt">wave</span> engine topping is slightly lower than that effected by ideal <span class="hlt">pressure</span>-exchanger topping. At a component level, however, flow turning affords the <span class="hlt">wave</span> engine a degree-of-freedom relative to the <span class="hlt">pressure</span>-exchanger that enables a more efficient match with the baseline engine. In some cases, therefore, the SFC-enhancement by <span class="hlt">wave</span> engine topping is greater than that by <span class="hlt">pressure</span>-exchanger topping. An ideal <span class="hlt">wave</span>-rotor-characteristic is used to identify key <span class="hlt">wave</span> engine design parameters and to contrast the <span class="hlt">wave</span> engine and <span class="hlt">pressure</span>-exchanger topping approaches. An aerodynamic design procedure is described in which <span class="hlt">wave</span> engine design-point performance levels are computed using a one-dimensional <span class="hlt">wave</span> rotor model. <span class="hlt">Wave</span> engines using various <span class="hlt">wave</span> cycles are considered including two-port cycles with on-rotor combustion (valved-combustors) and reverse-flow and through-flow four-port cycles with heat addition in conventional burners. A through-flow <span class="hlt">wave</span> cycle design with symmetric blading is used to assess engine performance benefits. The <span class="hlt">wave</span>-engine-topped turboshaft engine produces 16% more power than does a <span class="hlt">pressure</span>-exchanger-topped engine under the specified topping</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23999585','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23999585"><span>Comparison of noninvasive assessments of central blood <span class="hlt">pressure</span> using general transfer function and late systolic shoulder of the radial <span class="hlt">pressure</span> <span class="hlt">wave</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wohlfahrt, Peter; Krajcoviechová, Alena; Seidlerová, Jitka; Mayer, Otto; Filipovsky, Jan; Cífková, Renata</p> <p>2014-02-01</p> <p>Central systolic blood <span class="hlt">pressure</span> (cSBP) can be derived by the general transfer function of the radial <span class="hlt">pressure</span> <span class="hlt">wave</span>, as used in the SphygmoCor device, or by regression equation from directly measured late systolic shoulder of the radial <span class="hlt">pressure</span> <span class="hlt">wave</span> (pSBP2), as used in the Omron HEM-9000AI device. The aim of this study was to compare the SphygmoCor estimates of cSBP with 2 estimates of cSBP provided by the Omron HEM-9000AI (cSBP, pSBP2) in a large cohort of the white population. In 391 patients aged 52.3±13.5 years (46% men) from the Czech post-MONICA Study, cSBP was measured using the SphygmoCor and Omron HEM-9000AI devices in random order. Omron cSBP and pSBP2 were perfectly correlated (r = 1.0; P < 0.0001). There was a strong correlation (r = 0.97; P < 0.0001) between Omron and SphygmoCor cSBP estimates, but Omron estimate was 13.1±4.7mm Hg higher than SphygmoCor cSBP. On the other hand, Omron pSBP2 strongly correlated with SphygmoCor cSBP (r = 0.97; P < 0.0001) and was 1.7±4.2mm Hg lower than SphygmoCor cSBP. In multivariable analysis, anthropometric and cardiovascular risk factors explained only 10% of the variance of the cSBP difference between devices while explaining 52% of the systolic blood <span class="hlt">pressure</span> amplification variance. Estimation of cSBP based on the late systolic shoulder of the radial <span class="hlt">wave</span> provides a comparable accuracy with the validated general transfer function. When comparing Omron HEM-9000AI and SphygmoCor estimates of cSBP, Omron pSBP2 should be used. The difference between both devices in cSBP may be explained by differences in calibration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S12A..08I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S12A..08I"><span>Seismic <span class="hlt">waves</span> triggering slow slip event on the <span class="hlt">pressure</span> gauge records in the Hikurangi subducting margin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ito, Y.; Wallace, L. M.; Henrys, S. A.; Kaneko, Y.; Webb, S. C.; Muramoto, T.; Ohta, K.; Mochizuki, K.; Suzuki, S.; Kido, M.; Hino, R.</p> <p>2017-12-01</p> <p>The two M7-class earthquakes struck in New Zealand in 2016. One is the M7.1 Te Araroa earthquake on 1st September, and the other is the M7.8 Kaikoura earthquake on 14th November. The M7.1 earthquake struck offshore, following a sequence of the Hikurangi slow slip event on the northern Hikurangi Margin. The M7.8 Kaikoura earthquake has triggered a shallow slow slip event of northern Hikurangi subduction margin. We present seismic and tsunami <span class="hlt">waves</span> radiated from two large earthquakes of M7.8 Kaikoura and M7.1 Te Araroa earthquakes in 2016 using a network of absolute <span class="hlt">pressure</span> gauges (APG) deployed at the Hikurangi subduction margin offshore New Zealand. We deployed 5 APG on the accretionary wedge at the northen part of the Hikurangi margnin in June 2016 at the northern part of Hikurangi subducting margin, and were recovered in June 2015. The <span class="hlt">pressure</span> gauge recorded data continuously for one year, with a logging interval of 1 or 2 s. Our processing of the APG data to identify seismic is a band pass filter with a range of 10-100 s is applied for seismic signals. We observed seismic <span class="hlt">waves</span> radiated from both the M7.8 Kaikoura and M7.1 Te Araroa earthquakes. The <span class="hlt">pressure</span> fluctuation more than 20 hPa from the arrivals of seismic <span class="hlt">waves</span> was observed on two both earthquakes. It should be noted that marine <span class="hlt">pressure</span> records are nearly equivalent to vertical acceleration measurements [Webb, 1998]. Specifically, on the M7.8 Kaikoura earthquake, the characteristic seismic signals with large amplitude more than 20 hPa lasting more than 300 s was observed on the all of four APGs. The long duration seismic <span class="hlt">waves</span> with relatively large amplitude observed after the 7.8 Kaikoura earthquake would dynamically trigger the Hikurangi slow slip event; the dynamic triggering and characteristic seismic <span class="hlt">waves</span> in the accretionary wedge has been predicted from a <span class="hlt">wave</span>-field modeling using a 3D velocity model with a low-velocity sedimentary basin [Wallace et al., 2017].</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4214659','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4214659"><span><span class="hlt">Wave</span> reflections in the pulmonary arteries analysed with the reservoir–<span class="hlt">wave</span> model</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Bouwmeester, J Christopher; Belenkie, Israel; Shrive, Nigel G; Tyberg, John V</p> <p>2014-01-01</p> <p>Conventional haemodynamic analysis of <span class="hlt">pressure</span> and flow in the pulmonary circulation yields incident and reflected <span class="hlt">waves</span> throughout the cardiac cycle, even during diastole. The reservoir–<span class="hlt">wave</span> model provides an alternative haemodynamic analysis consistent with minimal <span class="hlt">wave</span> activity during diastole. <span class="hlt">Pressure</span> and flow in the main pulmonary artery were measured in anaesthetized dogs and the effects of hypoxia and nitric oxide, volume loading and positive end-expiratory <span class="hlt">pressure</span> were observed. The reservoir–<span class="hlt">wave</span> model was used to determine the reservoir contribution to <span class="hlt">pressure</span> and flow and once subtracted, resulted in ‘excess’ quantities, which were treated as <span class="hlt">wave</span>-related. <span class="hlt">Wave</span> intensity analysis quantified the contributions of <span class="hlt">waves</span> originating upstream (forward-going <span class="hlt">waves</span>) and downstream (backward-going <span class="hlt">waves</span>). In the pulmonary artery, negative reflections of incident <span class="hlt">waves</span> created by the right ventricle were observed. Overall, the distance from the pulmonary artery valve to this reflection site was calculated to be 5.7 ± 0.2 cm. During 100% O2 ventilation, the strength of these reflections increased 10% with volume loading and decreased 4% with 10 cmH2O positive end-expiratory <span class="hlt">pressure</span>. In the pulmonary arterial circulation, negative reflections arise from the junction of lobar arteries from the left and right pulmonary arteries. This mechanism serves to reduce peak systolic <span class="hlt">pressure</span>, while increasing blood flow. PMID:24756638</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JMiMi..20h7001W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JMiMi..20h7001W"><span>TECHNICAL NOTE: <span class="hlt">Portable</span> audio electronics for impedance-based measurements in microfluidics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wood, Paul; Sinton, David</p> <p>2010-08-01</p> <p>We demonstrate the use of audio electronics-based signals to perform on-chip electrochemical measurements. Cell phones and <span class="hlt">portable</span> music players are examples of consumer electronics that are easily operated and are ubiquitous worldwide. Audio output (play) and input (record) signals are voltage based and contain frequency and amplitude information. A cell phone, laptop soundcard and two compact audio players are compared with respect to frequency response; the laptop soundcard provides the most uniform frequency response, while the cell phone performance is found to be insufficient. The audio signals in the common <span class="hlt">portable</span> music players and laptop soundcard operate in the range of 20 Hz to 20 kHz and are found to be applicable, as voltage input and output signals, to impedance-based electrochemical measurements in microfluidic systems. Validated impedance-based measurements of concentration (0.1-50 mM), flow rate (2-120 µL min-1) and particle detection (32 µm diameter) are demonstrated. The prevailing, lossless, <span class="hlt">wave</span> audio file format is found to be suitable for data transmission to and from external sources, such as a centralized lab, and the cost of all hardware (in addition to audio devices) is ~10 USD. The utility demonstrated here, in combination with the ubiquitous nature of <span class="hlt">portable</span> audio electronics, presents new opportunities for impedance-based measurements in <span class="hlt">portable</span> microfluidic systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22308923-experimental-observation-standing-wave-effect-low-pressure-very-high-frequency-capacitive-discharges','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22308923-experimental-observation-standing-wave-effect-low-pressure-very-high-frequency-capacitive-discharges"><span>Experimental observation of standing <span class="hlt">wave</span> effect in low-<span class="hlt">pressure</span> very-high-frequency capacitive discharges</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Liu, Yong-Xin; Gao, Fei; Liu, Jia</p> <p>2014-07-28</p> <p>Radial uniformity measurements of plasma density were carried out by using a floating double probe in a cylindrical (21 cm in electrode diameter) capacitive discharge reactor driven over a wide range of frequencies (27–220 MHz). At low rf power, a multiple-node structure of standing <span class="hlt">wave</span> effect was observed at 130 MHz. The secondary density peak caused by the standing <span class="hlt">wave</span> effect became pronounced and shifts toward the axis as the driving frequency further to increase, indicative of a much more shortened standing-<span class="hlt">wave</span> wavelength. With increasing rf power, the secondary density peak shift toward the radial edge, namely, the standing-<span class="hlt">wave</span> wavelength was increased,more » in good qualitative agreement with the previous theory and simulation results. At higher <span class="hlt">pressures</span> and high frequencies, the rf power was primarily deposited at the periphery of the electrode, due to the fact that the <span class="hlt">waves</span> were strongly damped as they propagated from the discharge edge into the center.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DFDG14001W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DFDG14001W"><span>The Impact of a Deepwater <span class="hlt">Wave</span> on a Wall with Finite Vertical Extent</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, An; Duncan, James H.</p> <p>2016-11-01</p> <p>The impact of a dispersively focused 2D plunging breaker (average <span class="hlt">wave</span> frequency 1.15 Hz) on a 2D wall that is 45 cm high and 30 cm thick is studied experimentally. The temporal evolution of the water surface profile upstream of the wall is measured with a cinematic LIF technique using frame rates up to 4,500 Hz. Impact <span class="hlt">pressures</span> on the wall are measured simultaneously at sample rates up to 900 kHz. The wall is located horizontally 6.41 m from the <span class="hlt">wave</span> <span class="hlt">maker</span> in all cases and the submergence of the bottom surface of the wall is varied. It is found that the impact behavior varies dramatically with the wall submergence. When the bottom is submerged by 13.3 cm, a flip-through impact occurs. In this case, the impact evolves without <span class="hlt">wave</span> breaking and a vertical jet is formed. When the wall is submerged by less than 4.5 cm, small-amplitude components in the <span class="hlt">wave</span> packet interact with the bottom of the wall before the main crest arrives. Ripples reflected during this interaction modify the behavior of the incoming breaker significantly. When the bottom of the wall is located sufficiently high above the mean water level, the first interaction occurs when the undisturbed <span class="hlt">wave</span> crest collides with the wall. The highest <span class="hlt">pressures</span> are observed in this case. The support of the Office of Naval Research is gratefully acknowledged.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1400173-laser-induced-pressure-wave-barocaloric-effect-during-flash-diffusivity-measurements','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1400173-laser-induced-pressure-wave-barocaloric-effect-during-flash-diffusivity-measurements"><span>Laser-induced <span class="hlt">pressure-wave</span> and barocaloric effect during flash diffusivity 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>Wang, Hsin; Porter, Wallace D.; Dinwiddie, Ralph Barton</p> <p></p> <p>We report laser-induced <span class="hlt">pressure-wave</span> and barocaloric effect captured by an infrared detector during thermal diffusivity measurements. Very fast (< 1 ms) and negative transients during laser flash measurements were captured by the infrared detector on thin, high thermal conductivity samples. Standard thermal diffusivity analysis only focuses the longer time scale thermal transient measured from the back surface due to thermal conduction. These negative spikes are filtered out and ignored as noise or anomaly from instrument. This study confirmed that the initial negative signal was indeed a temperature drop induced by the laser pulse. The laser pulse induced instantaneous volume expansionmore » and the associated cooling in the specimen can be explained by the barocaloric effect. The initial cooling (< 100 microsecond) is also known as thermoelastic effect in which a negative temperature change is generated when the material is elastically deformed by volume expansion. A subsequent temperature oscillation in the sample was observed and only lasted about one millisecond. The <span class="hlt">pressure-wave</span> induced thermal signal was systematically studied and analyzed. In conclusion, the underlying physics of photon-mechanical-thermal energy conversions and the potential of using this signal to study barocaloric effects in solids are discussed.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1400173-laser-induced-pressure-wave-barocaloric-effect-during-flash-diffusivity-measurements','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1400173-laser-induced-pressure-wave-barocaloric-effect-during-flash-diffusivity-measurements"><span>Laser-induced <span class="hlt">pressure-wave</span> and barocaloric effect during flash diffusivity measurements</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Wang, Hsin; Porter, Wallace D.; Dinwiddie, Ralph Barton</p> <p>2017-08-01</p> <p>We report laser-induced <span class="hlt">pressure-wave</span> and barocaloric effect captured by an infrared detector during thermal diffusivity measurements. Very fast (< 1 ms) and negative transients during laser flash measurements were captured by the infrared detector on thin, high thermal conductivity samples. Standard thermal diffusivity analysis only focuses the longer time scale thermal transient measured from the back surface due to thermal conduction. These negative spikes are filtered out and ignored as noise or anomaly from instrument. This study confirmed that the initial negative signal was indeed a temperature drop induced by the laser pulse. The laser pulse induced instantaneous volume expansionmore » and the associated cooling in the specimen can be explained by the barocaloric effect. The initial cooling (< 100 microsecond) is also known as thermoelastic effect in which a negative temperature change is generated when the material is elastically deformed by volume expansion. A subsequent temperature oscillation in the sample was observed and only lasted about one millisecond. The <span class="hlt">pressure-wave</span> induced thermal signal was systematically studied and analyzed. In conclusion, the underlying physics of photon-mechanical-thermal energy conversions and the potential of using this signal to study barocaloric effects in solids are discussed.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JFS....33...44M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JFS....33...44M"><span>Water-hammer <span class="hlt">pressure</span> <span class="hlt">waves</span> interaction at cross-section changes in series in viscoelastic pipes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Meniconi, S.; Brunone, B.; Ferrante, M.</p> <p>2012-08-01</p> <p>In view of scarcity of both experimental data and numerical models concerning transient behavior of cross-section area changes in <span class="hlt">pressurized</span> liquid flow, the paper presents laboratory data and numerical simulation of the interaction of a surge <span class="hlt">wave</span> with a partial blockage by a valve, a single pipe contraction or expansion and a series of pipe contraction/expansion in close proximity.With regard to a single change of cross-section area, laboratory data point out the completely different behavior with respect to one of the partially closed in-line valves with the same area ratio. In fact, for the former the <span class="hlt">pressure</span> <span class="hlt">wave</span> interaction is not regulated by the steady-state local head loss. With regard to partial blockages, transient tests have shown that the smaller the length, the more intense the overlapping of <span class="hlt">pressure</span> <span class="hlt">waves</span> due to the expansion and contraction in series.Numerically, the need for taking into account both the viscoelasticity and unsteady friction is demonstrated, since the classical water-hammer theory does not simulate the relevant damping of <span class="hlt">pressure</span> peaks and gives rise to a time shifting between numerical and laboratory data. The transient behavior of a single local head loss has been checked by considering tests carried out in a system with a partially closed in-line valve. As a result, the reliability of the quasi steady-state approach for local head loss simulation has been demonstrated in viscoelastic pipes. The model parameters obtained on the basis of transients carried out in single pipe systems have then been used to simulate transients in the more complex pipe systems. These numerical experiments show the great importance of the length of the small-bore pipe with respect to one of the large-bore pipes. Precisely, until a gradually flow establishes in the small-bore pipe, the smaller such a length, the better the quality of the numerical simulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19672581','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19672581"><span>Exploring microdischarges for <span class="hlt">portable</span> sensing applications.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gianchandani, Y B; Wright, S A; Eun, C K; Wilson, C G; Mitra, B</p> <p>2009-10-01</p> <p>This paper describes the use of microdischarges as transducing elements in sensors and detectors. Chemical and physical sensing of gases, chemical sensing of liquids, and radiation detection are described. These applications are explored from the perspective of their use in <span class="hlt">portable</span> microsystems, with emphasis on compactness, power consumption, the ability to operate at or near atmospheric <span class="hlt">pressure</span> (to reduce pumping challenges), and the ability to operate in an air ambient (to reduce the need for reservoirs of carrier gases). Manufacturing methods and performance results are described for selected examples.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70032329','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70032329"><span>Landslide stability: Role of rainfall-induced, laterally propagating, pore-<span class="hlt">pressure</span> <span class="hlt">waves</span></span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Priest, G.R.; Schulz, W.H.; Ellis, W.L.; Allan, J.A.; Niem, A.R.; Niem, W.A.</p> <p>2011-01-01</p> <p>The Johnson Creek Landslide is a translational slide in seaward-dipping Miocene siltstone and sandstone (Astoria Formation) and an overlying Quaternary marine terrace deposit. The basal slide plane slopes sub-parallel to the dip of the Miocene rocks, except beneath the back-tilted toe block, where it slopes inland. Rainfall events raise pore-water <span class="hlt">pressure</span> in the basal shear zone in the form of pulses of water <span class="hlt">pressure</span> traveling laterally from the headwall graben down the axis of the slide at rates of 1-6 m/hr. Infiltration of meteoric water and vertical <span class="hlt">pressure</span> transmission through the unsaturated zone has been measured at ~50 mm/hr. Infiltration and vertical <span class="hlt">pressure</span> transmission were too slow to directly raise head at the basal shear zone prior to landslide movement. Only at the headwall graben was the saturated zone shallow enough for rainfall events to trigger lateral pulses of water <span class="hlt">pressure</span> through the saturated zone. When <span class="hlt">pressure</span> levels in the basal shear zone exceeded thresholds defined in this paper, the slide began slow, creeping movement as an intact block. As <span class="hlt">pressures</span> exceeded thresholds for movement in more of the slide mass, movement accelerated, and differential displacement between internal slide blocks became more pronounced. Rainfall-induced pore-<span class="hlt">pressure</span> <span class="hlt">waves</span> are probably a common landslide trigger wherever effective hydraulic conductivity is high and the saturated zone is located near the surface in some part of a slide. An ancillary finding is apparently greater accuracy of grouted piezometers relative to those in sand packs for measurement of pore <span class="hlt">pressures</span> at the installed depth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950058892&hterms=Magnetic+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DMagnetic%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950058892&hterms=Magnetic+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DMagnetic%2Benergy"><span>Radial energy transport by magnetospheric ULF <span class="hlt">waves</span>: Effects of magnetic curvature and plasma <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>Kouznetsov, Igor; Lotko, William</p> <p>1995-01-01</p> <p>The 'radial' transport of energy by internal ULF <span class="hlt">waves</span>, stimulated by dayside magnetospheric boundary oscillations, is analyzed in the framework of one-fluid magnetohydrodynamics. (the term radial is used here to denote the direction orthogonal to geomagnetic flux surfaces.) The model for the inhomogeneous magnetospheric plasma and background magnetic field is axisymmetric and includes radial and parallel variations in the magnetic field, magnetic curvature, plasma density, and low but finite plasma <span class="hlt">pressure</span>. The radial mode structure of the coupled fast and intermediate MHD <span class="hlt">waves</span> is determined by numerical solution of the inhomogeneous <span class="hlt">wave</span> equation; the parallel mode structure is characterized by a Wentzel-Kramer-Brillouin (WKB) approximation. Ionospheric dissipation is modeled by allowing the parallel <span class="hlt">wave</span> number to be complex. For boudnary oscillations with frequencies in the range from 10 to 48 mHz, and using a dipole model for the background magnetic field, the combined effects of magnetic curvature and finite plasma <span class="hlt">pressure</span> are shown to (1) enhance the amplitude of field line resonances by as much as a factor of 2 relative to values obtained in a cold plasma or box-model approximation for the dayside magnetosphere; (2) increase the energy flux delivered to a given resonance by a factor of 2-4; and (3) broaden the spectral width of the resonance by a factor of 2-3. The effects are attributed to the existence of an 'Alfven buoyancy oscillation,' which approaches the usual shear mode Alfven <span class="hlt">wave</span> at resonance, but unlike the shear Alfven mode, it is dispersive at short perpendicular wavelengths. The form of dispersion is analogous to that of an internal atmospheric gravity <span class="hlt">wave</span>, with the magnetic tension of the curved background field providing the restoring force and allowing radial propagation of the mode. For nominal dayside parameters, the propagation band of the Alfven buoyancy <span class="hlt">wave</span> occurs between the location of its (field line) resonance and that of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1295510-negative-pressures-spallation-water-drops-subjected-nanosecond-shock-waves','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1295510-negative-pressures-spallation-water-drops-subjected-nanosecond-shock-waves"><span>Negative <span class="hlt">pressures</span> and spallation in water drops subjected to nanosecond shock <span class="hlt">waves</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Stan, Claudiu A.; Willmott, Philip R.; Stone, Howard A.; ...</p> <p>2016-05-16</p> <p>Most experimental studies of cavitation in liquid water at negative <span class="hlt">pressures</span> reported cavitation at tensions significantly smaller than those expected for homogeneous nucleation, suggesting that achievable tensions are limited by heterogeneous cavitation. We generated tension pulses with nanosecond rise times in water by reflecting cylindrical shock <span class="hlt">waves</span>, produced by X-ray laser pulses, at the internal surface of drops of water. Depending on the X-ray pulse energy, a range of cavitation phenomena occurred, including the rupture and detachment, or spallation, of thin liquid layers at the surface of the drop. When spallation occurred, we evaluated that negative <span class="hlt">pressures</span> below –100 MPamore » were reached in the drops. As a result, we model the negative <span class="hlt">pressures</span> from shock reflection experiments using a nucleation-and-growth model that explains how rapid decompression could outrun heterogeneous cavitation in water, and enable the study of stretched water close to homogeneous cavitation <span class="hlt">pressures</span>.« less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_11 --> <div id="page_12" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="221"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvF...2k4802A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvF...2k4802A"><span>Three-<span class="hlt">wave</span> and four-<span class="hlt">wave</span> interactions in gravity <span class="hlt">wave</span> turbulence</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aubourg, Quentin; Campagne, Antoine; Peureux, Charles; Ardhuin, Fabrice; Sommeria, Joel; Viboud, Samuel; Mordant, Nicolas</p> <p>2017-11-01</p> <p>Weak-turbulence theory is a statistical framework to describe a large ensemble of nonlinearly interacting <span class="hlt">waves</span>. The archetypal example of such system is the ocean surface that is made of interacting surface gravity <span class="hlt">waves</span>. Here we describe a laboratory experiment dedicated to probe the statistical properties of turbulent gravity <span class="hlt">waves</span>. We set up an isotropic state of interacting gravity <span class="hlt">waves</span> in the Coriolis facility (13-m-diam circular <span class="hlt">wave</span> tank) by exciting <span class="hlt">waves</span> at 1 Hz by wedge <span class="hlt">wave</span> <span class="hlt">makers</span>. We implement a stereoscopic technique to obtain a measurement of the surface elevation that is resolved in both space and time. Fourier analysis shows that the laboratory spectra are systematically steeper than the theoretical predictions and the field observations in the Black Sea by Leckler et al. [F. Leckler et al., J. Phys. Oceanogr. 45, 2484 (2015), 10.1175/JPO-D-14-0237.1]. We identify a strong impact of surface dissipation on the scaling of the Fourier spectrum at the scales that are accessible in the experiments. We use bicoherence and tricoherence statistical tools in frequency and/or <span class="hlt">wave</span>-vector space to identify the active nonlinear coupling. These analyses are also performed on the field data by Leckler et al. for comparison with the laboratory data. Three-<span class="hlt">wave</span> coupling is characterized by and shown to involve mostly quasiresonances of <span class="hlt">waves</span> with second- or higher-order harmonics. Four-<span class="hlt">wave</span> coupling is not observed in the laboratory but is evidenced in the field data. We discuss temporal scale separation to explain our observations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5473523','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5473523"><span>Economic and organizational sustainability of a negative-<span class="hlt">pressure</span> <span class="hlt">portable</span> device for the prevention of surgical-site complications</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Foglia, Emanuela; Ferrario, Lucrezia; Garagiola, Elisabetta; Signoriello, Giuseppe; Pellino, Gianluca; Croce, Davide; Canonico, Silvestro</p> <p>2017-01-01</p> <p>Purpose Surgical-site complications (SSCs) affect patients’ clinical pathway, prolonging their hospitalization and incrementing their management costs. The present study aimed to assess the economic and organizational implications of a <span class="hlt">portable</span> device for negative-<span class="hlt">pressure</span> wound therapy (NPWT) implementation, compared with the administration of pharmacological therapies alone for preventing surgical complications in patients undergoing general, cardiac, obstetrical–gynecological, or orthopedic surgical procedures. Patients and methods A total of 8,566 hospital procedures, related to the year 2015 from one hospital, were evaluated considering infection risk index, occurrence rates of SSCs, drug therapies, and surgical, diagnostic, and specialist procedures and hematological exams. Activity-based costing and budget impact analyses were implemented for the economic assessment. Results Patients developing an SSC absorbed i) 64.27% more economic resources considering the length of stay (€ 8,269±2,096 versus € 5,034±2,901, p<0.05) and ii) 42.43% more economic resources related to hematological and diagnostic procedures (€ 639±117 versus € 449±72, p<0.05). If the innovative device had been used over the 12-month time period, it would have decreased the risk of developing SSCs; the hospital would have realized an average reduction in health care expenditure equal to −0.69% (−€ 483,787.92) and an organizational saving in terms of length of stay equal to −1.10% (−898 days), thus allowing 95 additional procedures. Conclusion The implementation of a <span class="hlt">portable</span> device for NPWT would represent an effective and sustainable strategy for reducing the management costs of patients. Economic and organizational savings could be reinvested, thus i) treating a wider population and ii) reducing waiting lists, with a higher effectiveness in terms of a decrease in complications. PMID:28652788</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1355142-investigation-energy-absorption-performance-fixed-bottom-pressure-differential-wave-energy-converter','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1355142-investigation-energy-absorption-performance-fixed-bottom-pressure-differential-wave-energy-converter"><span>Investigation on the energy absorption performance of a fixed-bottom <span class="hlt">pressure</span>-differential <span class="hlt">wave</span> energy converter</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>Babarit, A.; Wendt, F.; Yu, Y. -H.</p> <p>2017-04-01</p> <p>In this article, we investigate the energy absorption performance of a fixed-bottom <span class="hlt">pressure</span>-differential <span class="hlt">wave</span> energy converter. Two versions of the technology are considered: one has the moving surfaces on the bottom of the air chambers whereas the other has the moving surfaces on the top. We developed numerical models in the frequency domain, thereby enabling the power absorption of the two versions of the device to be assessed. It is observed that the moving surfaces on the top allow for easier tuning of the natural period of the system. Taking into account stroke limitations, the design is optimized. Results indicatemore » that the <span class="hlt">pressure</span>-differential <span class="hlt">wave</span> energy converter is a highly efficient technology both with respect to energy absorption and selected economic performance indicators.« less</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>Acoustic <span class="hlt">pressure</span> <span class="hlt">waves</span> 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> <span class="hlt">wave</span> inside the head. We report a computational study of the intensity and frequency of thermoelastic <span class="hlt">pressure</span> <span class="hlt">waves</span> 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 acoustic <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 acoustic <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 acoustic <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/29195423','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29195423"><span>Evaluation of an experimental electrohydraulic discharge device for extracorporeal shock <span class="hlt">wave</span> lithotripsy: <span class="hlt">Pressure</span> field of sparker array.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Guangyan; Connors, Bret A; Schaefer, Ray B; Gallagher, John J; Evan, Andrew P</p> <p>2017-11-01</p> <p>In this paper, an extracorporeal shock <span class="hlt">wave</span> source composed of small ellipsoidal sparker units is described. The sparker units were arranged in an array designed to produce a coherent shock <span class="hlt">wave</span> of sufficient strength to fracture kidney stones. The objective of this paper was to measure the acoustical output of this array of 18 individual sparker units and compare this array to commercial lithotripters. Representative waveforms acquired with a fiber-optic probe hydrophone at the geometric focus of the sparker array indicated that the sparker array produces a shock <span class="hlt">wave</span> (P + ∼40-47 MPa, P - ∼2.5-5.0 MPa) similar to shock <span class="hlt">waves</span> produced by a Dornier HM-3 or Dornier Compact S. The sparker array's <span class="hlt">pressure</span> field map also appeared similar to the measurements from a HM-3 and Compact S. Compared to the HM-3, the electrohydraulic technology of the sparker array produced a more consistent SW pulse (shot-to-shot positive <span class="hlt">pressure</span> value standard deviation of ±4.7 MPa vs ±3.3 MPa).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12108115','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12108115"><span>Public health privatization: proponents, registers, and decision-<span class="hlt">makers</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Keane, Christopher; Marx, John; Ricci, Edmund</p> <p>2002-01-01</p> <p>We previously documented the extent and consequences of the privatization of public health, using a nationally representative sample of 347 Local Health Department (LHD) directors. Here we present the directors' descriptions of the actors involved in the privatization of services. LHD top administrators are the most influential privatization decision-<span class="hlt">makers</span> in about half of LHDs. But other groups significantly influence privatization decisions, particularly state governments, state health departments, and local officials. Nearly two thirds of LHDs experienced <span class="hlt">pressures</span> to privatize, either from state legislatures, state health departments, funding organizations, or other source of political <span class="hlt">pressure</span>. Almost half of LHD directors reported resistance to privatization, often from employees. The majority of directors did not believe it was desirable to put employees on a temporary, contractual basis. Many directors believed that retaining permanent, full-time employees was fairer as well as necessary to maintain a cadre of experienced public health professionals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994PhDT........90G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994PhDT........90G"><span>A Experimental Study of Fluctuating <span class="hlt">Pressure</span> Loads Beneath Swept Shock <span class="hlt">Wave</span>/boundary Layer Interactions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Garg, Sanjay</p> <p></p> <p>An experimental research program providing basic knowledge and establishing a database on the fluctuating <span class="hlt">pressure</span> loads produced on aerodynamic surfaces beneath three-dimensional shock <span class="hlt">wave</span>/boundary layer interactions is described. Such loads constitute a fundamental problem of critical concern to future supersonic and hypersonic flight vehicles. A turbulent boundary layer on a flat plate is subjected to interactions with swept planar shock <span class="hlt">waves</span> generated by sharp fins. Fin angles from 10 ^circ to 20^circ at freestream Mach numbers of 3 and 4 produce a variety of interaction strengths from weak to very strong. Miniature <span class="hlt">pressure</span> transducers flush-mounted in the flat plate have been used to measure interaction-induced wall <span class="hlt">pressure</span> fluctuations. The distributions of properties of the <span class="hlt">pressure</span> fluctuations, such as their rms level, amplitude distribution and power spectra, are also determined. Measurements have been made for the first time in the aft regions of these interactions, revealing fluctuating <span class="hlt">pressure</span> levels as high as 155 dB, which places them in the category of significant aeroacoustic load generators. The fluctuations near the foot of the fin are dominated by low frequency (0-5 kHz) components, and are caused by a previously unrecognized random motion of the primary attachment line. This phenomenon is probably intimately linked to the unsteadiness of the separation shock at the start of the interaction. The characteristics of the <span class="hlt">pressure</span> fluctuations are explained in light of the features of the interaction flowfield. In particular, physical mechanisms responsible for the generation of high levels of surface <span class="hlt">pressure</span> fluctuations are proposed based on the results of the study. The unsteadiness of the flowfield of the surface is also examined via a novel, non-intrusive optical technique. Results show that the entire shock structure generated by the interaction undergoes relatively low-frequency oscillations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1027668','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1027668"><span>Use of a <span class="hlt">Portable</span> Stimulator to Treat GWI</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2016-10-01</p> <p>equilibrium in veterans during stochastic noise electrical stim. Electrical Stimulation Time (sec) 0 5 10 15 20 m A -1.0 -0.5 0.0 0.5 1.0 Center of <span class="hlt">Pressure</span>...AD______________ AWARD NUMBER: W81XWH-14-1-0598 TITLE: Use of a <span class="hlt">Portable</span> Stimulator to Treat GWI PRINCIPAL INVESTIGATOR: Jorge M... time for reviewing instructions, searching existing data sources, gathering and maintaining the data needed, and completing and reviewing this</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/18321','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/18321"><span>Operations manual for <span class="hlt">portable</span> profiler : installing and using the <span class="hlt">portable</span> profiler.</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2010-06-01</p> <p>This manual is divided into two sections. The first is using the UTA-Profiler Program : with the <span class="hlt">portable</span> profiler for generating surface profilers. The second is installing the : <span class="hlt">portable</span> profiler module on a typical van or truck. The calibration an...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3379524','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3379524"><span><span class="hlt">Portable</span> Bladder Ultrasound</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2006-01-01</p> <p>Executive Summary Objective The aim of this review was to assess the clinical utility of <span class="hlt">portable</span> bladder ultrasound. Clinical Need: Target Population and Condition Data from the National Population Health Survey indicate prevalence rates of urinary incontinence are 2.5% in women and 1.4 % in men in the general population. Prevalence of urinary incontinence is higher in women than men and prevalence increases with age. Identified risk factors for urinary incontinence include female gender, increasing age, urinary tract infections (UTI), poor mobility, dementia, smoking, obesity, consuming alcohol and caffeine beverages, physical activity, pregnancy, childbirth, forceps and vacuum-assisted births, episiotomy, abdominal resection for colorectal cancer, and hormone replacement therapy. For the purposes of this review, incontinence populations will be stratified into the following; the elderly, urology patients, postoperative patients, rehabilitation settings, and neurogenic bladder populations. Urinary incontinence is defined as any involuntary leakage of urine. Incontinence can be classified into diagnostic clinical types that are useful in planning evaluation and treatment. The major types of incontinence are stress (physical exertion), urge (overactive bladder), mixed (combined urge and stress urinary incontinence), reflex (neurological impairment of the central nervous system), overflow (leakage due to full bladder), continuous (urinary tract abnormalities), congenital incontinence, and transient incontinence (temporary incontinence). Postvoid residual (PVR) urine volume, which is the amount of urine in the bladder immediately after urination, represents an important component in continence assessment and bladder management to provide quantitative feedback to the patient and continence care team regarding the effectiveness of the voiding technique. Although there is no standardized definition of normal PVR urine volume, measurements greater than 100 mL to 150 m</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2578221','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2578221"><span><span class="hlt">Portable</span> Medical Laboratory Applications Software</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Silbert, Jerome A.</p> <p>1983-01-01</p> <p><span class="hlt">Portability</span> implies that a program can be run on a variety of computers with minimal software revision. The advantages of <span class="hlt">portability</span> are outlined and design considerations for <span class="hlt">portable</span> laboratory software are discussed. Specific approaches for achieving this goal are presented.</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> <span class="hlt">Waves</span> Within Open and Closed Acoustic 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 acoustic <span class="hlt">pressure</span> <span class="hlt">waves</span> 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 acoustic <span class="hlt">pressure</span> amplitudes varied little from baseline measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950004981','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950004981"><span><span class="hlt">Portable</span> seat lift</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Weddendorf, Bruce (Inventor)</p> <p>1994-01-01</p> <p>A <span class="hlt">portable</span> seat lift that can help individuals either (1) lower themselves to a sitting position or (2) raise themselves to a standing position is presented. The <span class="hlt">portable</span> seat lift consists of a seat mounted on a base with two levers, which are powered by a drive unit.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25503470','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25503470"><span>Analysis of polycyclic aromatic hydrocarbons using desorption atmospheric <span class="hlt">pressure</span> chemical ionization coupled to a <span class="hlt">portable</span> mass spectrometer.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jjunju, Fred P M; Maher, Simon; Li, Anyin; Badu-Tawiah, Abraham K; Taylor, Stephen; Cooks, R Graham</p> <p>2015-02-01</p> <p>Desorption atmospheric <span class="hlt">pressure</span> chemical ionization (DAPCI) is implemented on a <span class="hlt">portable</span> mass spectrometer and applied to the direct detection of polycyclic aromatic hydrocarbons (PAHs) and alkyl substituted benzenes. The presence of these compounds in the environment poses a significant threat to the health of both humans and wildlife because of their carcinogenic, toxic, and mutagenic properties. As such, instant detection outside of the laboratory is of particular importance to allow in-situ measurement at the source. Using a rapid, high throughput, miniature, handheld mass spectrometer, several alkyl substituted benzenes and PAHs (i.e., 1,2,3,5-tetramethylbenzene, pentamethylbenzene, hexamethylbenzene, fluoranthene, anthracene, benzo[k]fluoranthene, dibenz[a,h]anthracene, acenaphthene, indeno[1,2,3-c,d]pyrene, 9-ethylfluorene, and 1-benzyl-3-methyl-naphthalene) were identified and characterized using tandem mass spectrometry (MS/MS) from ambient surfaces, in the open air. This method can provide almost instantaneous information while minimizing sample preparation, which is advantageous in terms of both cost and simplicity of analysis. This MS-based technique is applicable to a wide range of environmental organic molecules.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-STS051-98-021.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-STS051-98-021.html"><span>Astronaut Carl Walz test <span class="hlt">portable</span> foot restraint in aft cargo bay</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>1993-09-16</p> <p>STS051-98-021 (16 Sept. 1993) --- In the Space Shuttle Discovery's aft cargo bay, astronaut Carl E. Walz gets his turn on the <span class="hlt">Portable</span> Foot Restraint (PFR). Astronauts Walz, <span class="hlt">waving</span> to his crew mates inside Discovery's cabin, and James H. Newman each put in some time evaluating the PFR, one of the pieces of gear to be used on the Hubble Space Telescope (HST) STS-61 servicing mission (scheduled later this year) and other Shuttle missions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhPl...25b3513X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhPl...25b3513X"><span>Propagation of atmospheric-<span class="hlt">pressure</span> ionization <span class="hlt">waves</span> along the tapered tube</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xia, Yang; Wang, Wenchun; Liu, Dongping; Yan, Wen; Bi, Zhenhua; Ji, Longfei; Niu, Jinhai; Zhao, Yao</p> <p>2018-02-01</p> <p>Gas discharge in a small radius dielectric tube may result in atmospheric <span class="hlt">pressure</span> plasma jets with high energy and density of electrons. In this study, the atmospheric <span class="hlt">pressure</span> ionization <span class="hlt">waves</span> (IWs) were generated inside a tapered tube. The propagation behaviors of IWs inside the tube were studied by using a spatially and temporally resolved optical detection system. Our measurements show that both the intensity and velocity of the IWs decrease dramatically when they propagate to the tapered region. After the taper, the velocity, intensity, and electron density of the IWs are improved with the tube inner diameter decreasing from 4.0 to 0.5 mm. Our analysis indicates that the local gas conductivity and surface charges may play a role in the propagation of the IWs under such a geometrical constraint, and the difference in the dynamics of the IWs after the taper can be related to the restriction in the size of IWs.</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 Acoustic <span class="hlt">Pressure</span> <span class="hlt">Wave</span> 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 <span class="hlt">waves</span> aid in penetration. This study evaluated in vivo if there is increased efficacy of fractional CO2 ablative laser with immediate acoustic <span class="hlt">pressure</span> <span class="hlt">wave</span> 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 acoustic <span class="hlt">pressure</span> <span class="hlt">wave</span> 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 acoustic <span class="hlt">pressure</span> <span class="hlt">wave</span> 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 acoustic <span class="hlt">pressure</span> <span class="hlt">wave</span> device was an order of magnitude greater. We found that our combined approach of fractional ablative CO2 laser paired with the transdermal acoustic <span class="hlt">pressure</span> <span class="hlt">wave</span> device increased the depth of penetration of ALA.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1038193-pressure-fluctuations-beneath-turbulent-spots-instability-wave-packets-hypersonic-boundary-layer','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1038193-pressure-fluctuations-beneath-turbulent-spots-instability-wave-packets-hypersonic-boundary-layer"><span><span class="hlt">Pressure</span> fluctuations beneath turbulent spots and instability <span class="hlt">wave</span> packets in a hypersonic boundary layer.</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>Beresh, Steven Jay; Casper, Katya M.; Schneider, Steven P.</p> <p>2010-12-01</p> <p>The development of turbulent spots in a hypersonic boundary layer was studied on the nozzle wall of the Boeing/AFOSR Mach-6 Quiet Tunnel. Under quiet flow conditions, the nozzle wall boundary layer remains laminar and grows very thick over the long nozzle length. This allows the development of large turbulent spots that can be readily measured with <span class="hlt">pressure</span> transducers. Measurements of naturally occurring <span class="hlt">wave</span> packets and developing turbulent spots were made. The peak frequencies of these natural <span class="hlt">wave</span> packets were in agreement with second-mode computations. For a controlled study, the breakdown of disturbances created by spark and glow perturbations were studiedmore » at similar freestream conditions. The spark perturbations were the most effective at creating large <span class="hlt">wave</span> packets that broke down into turbulent spots. The flow disturbances created by the controlled perturbations were analyzed to obtain amplitude criteria for nonlinearity and breakdown as well as the convection velocities of the turbulent spots. Disturbances first grew into linear instability <span class="hlt">waves</span> and then quickly became nonlinear. Throughout the nonlinear growth of the <span class="hlt">wave</span> packets, large harmonics are visible in the power spectra. As breakdown begins, the peak amplitudes of the instability <span class="hlt">waves</span> and harmonics decrease into the rising broad-band frequencies. Instability <span class="hlt">waves</span> are still visible on either side of the growing turbulent spots during this breakdown process.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title46-vol4/pdf/CFR-2013-title46-vol4-sec119-458.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title46-vol4/pdf/CFR-2013-title46-vol4-sec119-458.pdf"><span>46 CFR 119.458 - <span class="hlt">Portable</span> fuel systems.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... 46 Shipping 4 2013-10-01 2013-10-01 false <span class="hlt">Portable</span> fuel systems. 119.458 Section 119.458 Shipping... Machinery Requirements § 119.458 <span class="hlt">Portable</span> fuel systems. (a) <span class="hlt">Portable</span> fuel systems, including <span class="hlt">portable</span> tanks and related fuel lines and accessories, are prohibited except where used for <span class="hlt">portable</span> dewatering pumps...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol4/pdf/CFR-2010-title46-vol4-sec119-458.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol4/pdf/CFR-2010-title46-vol4-sec119-458.pdf"><span>46 CFR 119.458 - <span class="hlt">Portable</span> fuel systems.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 46 Shipping 4 2010-10-01 2010-10-01 false <span class="hlt">Portable</span> fuel systems. 119.458 Section 119.458 Shipping... Machinery Requirements § 119.458 <span class="hlt">Portable</span> fuel systems. (a) <span class="hlt">Portable</span> fuel systems, including <span class="hlt">portable</span> tanks and related fuel lines and accessories, are prohibited except where used for <span class="hlt">portable</span> dewatering pumps...</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_12 --> <div id="page_13" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="241"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2596633','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2596633"><span>Development of a <span class="hlt">portable</span> therapeutic and high intensity ultrasound system for military, medical, and research use</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Lewis, George K.; Olbricht, William L.</p> <p>2008-01-01</p> <p>We have developed a <span class="hlt">portable</span> high power ultrasound system with a very low output impedance amplifier circuit (less than 0.3 Ω) that can transfer more than 90% of the energy from a battery supply to the ultrasound transducer. The system can deliver therapeutic acoustical energy <span class="hlt">waves</span> at lower voltages than those in conventional ultrasound systems because energy losses owing to a mismatched impedance are eliminated. The system can produce acoustic power outputs over the therapeutic range (greater then 50 W) from a PZT-4, 1.54 MHz, and 0.75 in diameter piezoelectric ceramic. It is lightweight, <span class="hlt">portable</span>, and powered by a rechargeable battery. The <span class="hlt">portable</span> therapeutic ultrasound unit has the potential to replace “plug-in” medical systems and rf amplifiers used in research. The system is capable of field service on its internal battery, making it especially useful for military, ambulatory, and remote medical applications. PMID:19045903</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhDT.......249T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhDT.......249T"><span>Electrostatic actuators for <span class="hlt">portable</span> microfluidic systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tice, Joshua</p> <p></p> <p> minimize actuation potentials while eliminating stiction. Two strategies were developed to overcome challenges with electrode screening in the presence of aqueous fluids. First, instead of using the electrostatic actuators to interact directly with aqueous solutions, the actuators were used to regulate <span class="hlt">pressurized</span> control lines for pneumatic microvalves. Secondly, by adopting a normally-closed architecture, the actuators were converted into microvalves capable of directly interacting with aqueous solutions. The two strategies are complementary, and together should enable sophisticated microfluidic systems for applications ranging from point-of-care diagnostics to <span class="hlt">portable</span> chemical detection. To conclude the dissertation, I demonstrate a proof-of-principle microfluidic system that contained sixteen independently-operated electrostatic valves, operated with battery-operated electrical ancillaries in a hand-held format.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhCS1035a2009T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS1035a2009T"><span>Shock <span class="hlt">wave</span> structure in rarefied polyatomic gases with large relaxation time for the dynamic <span class="hlt">pressure</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Taniguchi, Shigeru; Arima, Takashi; Ruggeri, Tommaso; Sugiyama, Masaru</p> <p>2018-05-01</p> <p>The shock <span class="hlt">wave</span> structure in rarefied polyatomic gases is analyzed based on extended thermodynamics (ET). In particular, the case with large relaxation time for the dynamic <span class="hlt">pressure</span>, which corresponds to large bulk viscosity, is considered by adopting the simplest version of extended thermodynamics with only 6 independent fields (ET6); the mass density, the velocity, the temperature and the dynamic <span class="hlt">pressure</span>. Recently, the validity of the theoretical predictions by ET was confirmed by the numerical analysis based on the kinetic theory in [S Kosuge and K Aoki: Phys. Rev. Fluids, Vol. 3, 023401 (2018)]. It was shown that numerical results using the polyatomic version of ellipsoidal statistical model agree with the theoretical predictions by ET for small or moderately large Mach numbers. In the present paper, first, we compare the theoretical predictions by ET6 with the ones by kinetic theory for large Mach number under the same assumptions, that is, the gas is polytropic and the bulk viscosity is proportional to the temperature. Second, the shock <span class="hlt">wave</span> structure for large Mach number in a non-polytropic gas is analyzed with the particular interest in the effect of the temperature dependence of specific heat and the bulk viscosity on the shock <span class="hlt">wave</span> structure. Through the analysis of the case of a rarefied carbon dioxide (CO2) gas, it is shown that these temperature dependences play important roles in the precise analysis of the structure for strong shock <span class="hlt">waves</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhFl...23i6603M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhFl...23i6603M"><span>Experimental observation of standing interfacial <span class="hlt">waves</span> induced by surface <span class="hlt">waves</span> in muddy water</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Maxeiner, Eric; Dalrymple, Robert A.</p> <p>2011-09-01</p> <p>A striking feature has been observed in a laboratory <span class="hlt">wave</span> tank with a thin layer of clear water overlying a layer of mud. A piston-type <span class="hlt">wave</span> <span class="hlt">maker</span> is used to generate long monochromatic surface <span class="hlt">waves</span> in a tank with a layer of kaolinite clay at the bottom. The <span class="hlt">wave</span> action on the mud causes the clay particles to rise from the bottom into the water column, forming a lutocline. As the lutocline approaches the water surface, a set of standing interfacial <span class="hlt">waves</span> form on the lutocline. The interfacial <span class="hlt">wave</span> directions are oriented nearly orthogonal to the surface <span class="hlt">wave</span> direction. The interfacial <span class="hlt">waves</span>, which sometimes cover the entire length and width of the tank, are also temporally subharmonic as the phase of the interfacial <span class="hlt">wave</span> alternates with each passing surface <span class="hlt">wave</span> crest. These interfacial <span class="hlt">waves</span> are the result of a resonant three-<span class="hlt">wave</span> interaction involving the surface <span class="hlt">wave</span> train and the two interfacial <span class="hlt">wave</span> trains. The interfacial <span class="hlt">waves</span> are only present when the lutocline is about 3 cm of the water surface and they can be sufficiently nonlinear as to exhibit superharmonics and a breaking-type of instability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/527914-cloud-point-detection-using-portable-thickness-shear-mode-crystal-resonator','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/527914-cloud-point-detection-using-portable-thickness-shear-mode-crystal-resonator"><span>Cloud-point detection using a <span class="hlt">portable</span> thickness shear mode crystal resonator</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>Mansure, A.J.; Spates, J.J.; Germer, J.W.</p> <p>1997-08-01</p> <p>The Thickness Shear Mode (TSM) crystal resonator monitors the crude oil by propagating a shear <span class="hlt">wave</span> into the oil. The coupling of the shear <span class="hlt">wave</span> and the crystal vibrations is a function of the viscosity of the oil. By driving the crystal with circuitry that incorporates feedback, it is possible to determine the change from Newtonian to non-Newtonian viscosity at the cloud point. A <span class="hlt">portable</span> prototype TSM Cloud Point Detector (CPD) has performed flawlessly during field and lab tests proving the technique is less subjective or operator dependent than the ASTM standard. The TSM CPD, in contrast to standard viscositymore » techniques, makes the measurement in a closed container capable of maintaining up to 100 psi. The closed container minimizes losses of low molecular weight volatiles, allowing samples (25 ml) to be retested with the addition of chemicals. By cycling/thermal soaking the sample, the effects of thermal history can be investigated and eliminated as a source of confusion. The CPD is <span class="hlt">portable</span>, suitable for shipping the field offices for use by personnel without special training or experience in cloud point measurements. As such, it can make cloud point data available without the delays and inconvenience of sending samples to special labs. The crystal resonator technology can be adapted to in-line monitoring of cloud point and deposition detection.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/867193','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/867193"><span>Apparatus and method for enhanced chemical processing in high <span class="hlt">pressure</span> and atmospheric plasmas produced by high frequency electromagnetic <span class="hlt">waves</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Efthimion, Philip C.; Helfritch, Dennis J.</p> <p>1989-11-28</p> <p>An apparatus and method for creating high temperature plasmas for enhanced chemical processing of gaseous fluids, toxic chemicals, and the like, at a wide range of <span class="hlt">pressures</span>, especially at atmospheric and high <span class="hlt">pressures</span> includes an electro-magnetic resonator cavity, preferably a reentrant cavity, and a <span class="hlt">wave</span> guiding structure which connects an electro-magnetic source to the cavity. The cavity includes an intake port and an exhaust port, each having apertures in the conductive walls of the cavity sufficient for the intake of the gaseous fluids and for the discharge of the processed gaseous fluids. The apertures are sufficiently small to prevent the leakage of the electro-magnetic radiation from the cavity. Gaseous fluid flowing from the direction of the electro-magnetic source through the guiding <span class="hlt">wave</span> structure and into the cavity acts on the plasma to push it away from the guiding <span class="hlt">wave</span> structure and the electro-magnetic source. The gaseous fluid flow confines the high temperature plasma inside the cavity and allows complete chemical processing of the gaseous fluids at a wide range of <span class="hlt">pressures</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22947434','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22947434"><span>Head orientation affects the intracranial <span class="hlt">pressure</span> response resulting from shock <span class="hlt">wave</span> loading in the rat.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dal Cengio Leonardi, Alessandra; Keane, Nickolas J; Bir, Cynthia A; Ryan, Anne G; Xu, Liaosa; Vandevord, Pamela J</p> <p>2012-10-11</p> <p>Since an increasing number of returning military personnel are presenting with neurological manifestations of traumatic brain injury (TBI), there has been a great focus on the effects resulting from blast exposure. It is paramount to resolve the physical mechanism by which the critical stress is being inflicted on brain tissue from blast <span class="hlt">wave</span> encounters with the head. This study quantitatively measured the effect of head orientation on intracranial <span class="hlt">pressure</span> (ICP) of rats exposed to a shock <span class="hlt">wave</span>. Furthermore, the study examined how skull maturity affects ICP response of animals exposed to shock <span class="hlt">waves</span> at various orientations. Results showed a significant increase in ICP values in larger rats at any orientation. Furthermore, when side-ICP values were compared to the other orientations, the peak <span class="hlt">pressures</span> were significantly lower suggesting a relation between ICP and orientation of the head due to geometry of the skull and location of sutures. This finding accentuates the importance of skull dynamics in explaining possible injury mechanisms during blast. Also, the rate of <span class="hlt">pressure</span> change was measured and indicated that the rate was significantly higher when the top of the head was facing the shock front. The results confirm that the biomechanical response of the superior rat skull is distinctive compared to other areas of the skull, suggesting a skull flexure mechanism. These results not only present insights into the mechanism of brain injury, but also provide information which can be used for designing more effective protective head gear. Copyright © 2012 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title29-vol7/pdf/CFR-2011-title29-vol7-sec1917-119.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title29-vol7/pdf/CFR-2011-title29-vol7-sec1917-119.pdf"><span>29 CFR 1917.119 - <span class="hlt">Portable</span> ladders.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-07-01</p> <p>... (CONTINUED) MARINE TERMINALS Terminal Facilities § 1917.119 <span class="hlt">Portable</span> ladders. (a) Scope and applicability... Requirements for <span class="hlt">Portable</span> Reinforced Plastic Ladders (d) Standards for job-made <span class="hlt">portable</span> ladders. Job-made...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title10-vol3/pdf/CFR-2012-title10-vol3-sec429-45.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title10-vol3/pdf/CFR-2012-title10-vol3-sec429-45.pdf"><span>10 CFR 429.45 - Automatic commercial ice <span class="hlt">makers</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-01-01</p> <p>... 10 Energy 3 2012-01-01 2012-01-01 false Automatic commercial ice <span class="hlt">makers</span>. 429.45 Section 429.45... PRODUCTS AND COMMERCIAL AND INDUSTRIAL EQUIPMENT Certification § 429.45 Automatic commercial ice <span class="hlt">makers</span>. (a... automatic commercial ice <span class="hlt">makers</span>; and (2) For each basic model of automatic commercial ice <span class="hlt">maker</span> selected for...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title10-vol3/pdf/CFR-2014-title10-vol3-sec429-45.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title10-vol3/pdf/CFR-2014-title10-vol3-sec429-45.pdf"><span>10 CFR 429.45 - Automatic commercial ice <span class="hlt">makers</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-01-01</p> <p>... 10 Energy 3 2014-01-01 2014-01-01 false Automatic commercial ice <span class="hlt">makers</span>. 429.45 Section 429.45... PRODUCTS AND COMMERCIAL AND INDUSTRIAL EQUIPMENT Certification § 429.45 Automatic commercial ice <span class="hlt">makers</span>. (a... automatic commercial ice <span class="hlt">makers</span>; and (2) For each basic model of automatic commercial ice <span class="hlt">maker</span> selected for...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title10-vol3/pdf/CFR-2013-title10-vol3-sec429-45.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title10-vol3/pdf/CFR-2013-title10-vol3-sec429-45.pdf"><span>10 CFR 429.45 - Automatic commercial ice <span class="hlt">makers</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-01-01</p> <p>... 10 Energy 3 2013-01-01 2013-01-01 false Automatic commercial ice <span class="hlt">makers</span>. 429.45 Section 429.45... PRODUCTS AND COMMERCIAL AND INDUSTRIAL EQUIPMENT Certification § 429.45 Automatic commercial ice <span class="hlt">makers</span>. (a... automatic commercial ice <span class="hlt">makers</span>; and (2) For each basic model of automatic commercial ice <span class="hlt">maker</span> selected for...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4011902','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4011902"><span>The 24-hour pulse <span class="hlt">wave</span> velocity, aortic augmentation index, and central blood <span class="hlt">pressure</span> in normotensive volunteers</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kuznetsova, Tatyana Y; Korneva, Viktoria A; Bryantseva, Evgeniya N; Barkan, Vitaliy S; Orlov, Artemy V; Posokhov, Igor N; Rogoza, Anatoly N</p> <p>2014-01-01</p> <p>The purpose of this study was to examine the pulse <span class="hlt">wave</span> velocity, aortic augmentation index corrected for heart rate 75 (AIx@75), and central systolic and diastolic blood <span class="hlt">pressure</span> during 24-hour monitoring in normotensive volunteers. Overall, 467 subjects (206 men and 261 women) were recruited in this study. Participants were excluded from the study if they were less than 19 years of age, had blood test abnormalities, had a body mass index greater than 2 7.5 kg/m2, had impaired glucose tolerance, or had hypotension or hypertension. Ambulatory blood <span class="hlt">pressure</span> monitoring (ABPM) with the BPLab® device was performed in each subject. ABPM waveforms were analyzed using the special automatic Vasotens® algorithm, which allows the calculation of pulse <span class="hlt">wave</span> velocity, AIx@75, central systolic and diastolic blood <span class="hlt">pressure</span> for “24-hour”, “awake”, and “asleep” periods. Circadian rhythms and sex differences in these indexes were identified. Pending further validation in prospective outcome-based studies, our data may be used as preliminary diagnostic values for the BPLab ABPM additional index in adult subjects. PMID:24812515</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1992PhRvB..4614370C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1992PhRvB..4614370C"><span>High-<span class="hlt">pressure</span> ultrasonic study of the commensurate-incommensurate spin-density-<span class="hlt">wave</span> transition in an antiferromagnetic Cr-0.3 at. % Ru alloy single crystal</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cankurtaran, M.; Saunders, G. A.; Wang, Q.; Ford, P. J.; Alberts, H. L.</p> <p>1992-12-01</p> <p>A comprehensive experimental study has been made of the elastic and nonlinear acoustic behavior of a dilute Cr alloy as it undergoes a commensurate (C)-incommensurate (I) spin-density-<span class="hlt">wave</span> transition. Simultaneous measurements of the temperature dependence of ultrasonic <span class="hlt">wave</span> velocity and attenuation of longitudinal and shear 10-MHz ultrasonic <span class="hlt">waves</span> propagated along both the [100] and the [110] direction of Cr-0.3 at. % Ru alloy single crystal have been made in the temperature range 200-300 K. The temperature dependence of ultrasonic attenuation for each mode is characterized by a spikelike peak centered at TCI (=238.6 K) (on cooling) and at TIC (=255.6 K) (on warming). The velocities of both longitudinal and shear ultrasonic <span class="hlt">waves</span> exhibit a large and steep increase at TCI on cooling and a similar drop at TIC on warming with a pronounced hysteresis between TIC and TCI. These observations show that the transition between the commensurate and incommensurate phases is first order. Measurements of the effects of hydrostatic <span class="hlt">pressure</span> (up to 0.15 GPa) on the velocities of ultrasonic <span class="hlt">waves</span>, which were made at several fixed temperatures between 248 and 297 K, show similar features: a steep increase at PCI (increasing <span class="hlt">pressure</span>) and a similar drop at PIC (decreasing <span class="hlt">pressure</span>) with a well-defined hysteresis. Both TCI and TIC increase strongly and approximately linearly with <span class="hlt">pressure</span>, the mean values of dTCI/dP and dTIC/dP being (333+/-3) K/GPa and (277+/-5) K/GPa, respectively. The <span class="hlt">pressure</span> and temperature dependencies of the anomalies in the ultrasonic <span class="hlt">wave</span> velocity have been used to locate both the C-I and I-C boundaries on the magnetic P-T phase diagram. There is a triple point (at about 315 K and 0.22 GPa) where the paramagnetic, commensurate, and incommensurate spin-density-<span class="hlt">wave</span> phases coexist. Results for the complete sets of the elastic stiffness tensor components and their hydrostatic <span class="hlt">pressure</span> derivatives have been used to evaluate the acoustic-mode Gr</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015RScI...86k5113V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015RScI...86k5113V"><span>Peristaltic pump-based low range <span class="hlt">pressure</span> sensor calibration system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vinayakumar, K. B.; Naveen Kumar, G.; Nayak, M. M.; Dinesh, N. S.; Rajanna, K.</p> <p>2015-11-01</p> <p>Peristaltic pumps were normally used to pump liquids in several chemical and biological applications. In the present study, a peristaltic pump was used to <span class="hlt">pressurize</span> the chamber (positive as well negative <span class="hlt">pressures</span>) using atmospheric air. In the present paper, we discuss the development and performance study of an automatic <span class="hlt">pressurization</span> system to calibrate low range (millibar) <span class="hlt">pressure</span> sensors. The system includes a peristaltic pump, calibrated <span class="hlt">pressure</span> sensor (master sensor), <span class="hlt">pressure</span> chamber, and the control electronics. An in-house developed peristaltic pump was used to <span class="hlt">pressurize</span> the chamber. A closed loop control system has been developed to detect and adjust the <span class="hlt">pressure</span> leaks in the chamber. The complete system has been integrated into a <span class="hlt">portable</span> product. The system performance has been studied for a step response and steady state errors. The system is <span class="hlt">portable</span>, free from oil contaminants, and consumes less power compared to existing <span class="hlt">pressure</span> calibration systems. The veracity of the system was verified by calibrating an unknown diaphragm based <span class="hlt">pressure</span> sensor and the results obtained were satisfactory.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3274031','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3274031"><span>Measurement of Blood <span class="hlt">Pressure</span> Using an Arterial Pulsimeter Equipped with a Hall 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>Lee, Sang-Suk; Nam, Dong-Hyun; Hong, You-Sik; Lee, Woo-Beom; Son, Il-Ho; Kim, Keun-Ho; Choi, Jong-Gu</p> <p>2011-01-01</p> <p>To measure precise blood <span class="hlt">pressure</span> (BP) and pulse rate without using a cuff, we have developed an arterial pulsimeter consisting of a small, <span class="hlt">portable</span> apparatus incorporating a Hall device. Regression analysis of the pulse <span class="hlt">wave</span> measured during testing of the arterial pulsimeter was conducted using two equations of the BP algorithm. The estimated values of BP obtained by the cuffless arterial pulsimeter over 5 s were compared with values obtained using electronic or liquid mercury BP meters. The standard deviation between the estimated values and the measured values for systolic and diastolic BP were 8.3 and 4.9, respectively, which are close to the range of values of the BP International Standard. Detailed analysis of the pulse <span class="hlt">wave</span> measured by the cuffless radial artery pulsimeter by detecting changes in the magnetic field can be used to develop a new diagnostic algorithm for BP, which can be applied to new medical apparatus such as the radial artery pulsimeter. PMID:22319381</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ApJ...774...59Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ApJ...774...59Y"><span>Small-scale <span class="hlt">Pressure</span>-balanced Structures Driven by Oblique Slow Mode <span class="hlt">Waves</span> Measured in the Solar Wind</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yao, Shuo; He, J.-S.; Tu, C.-Y.; Wang, L.-H.; Marsch, E.</p> <p>2013-09-01</p> <p>Recently, small-scale <span class="hlt">pressure</span>-balanced structures (PBSs) were identified in the solar wind, but their formation mechanism remains unclear. This work aims to reveal the dependence of the properties of small-scale PBSs on the background magnetic field (B 0) direction and thus to corroborate the in situ mechanism that forms them. We analyze the plasma and magnetic field data obtained by WIND in the quiet solar wind at 1 AU. First, we use a developed moving-average method to obtain B 0(s, t) for every temporal scale (s) at each time moment (t). By wavelet cross-coherence analysis, we obtain the correlation coefficients between the thermal <span class="hlt">pressure</span> P th and the magnetic <span class="hlt">pressure</span> P B, distributing against the temporal scale and the angle θxB between B 0(s, t) and Geocentric Solar Ecliptic coordinates (GSE)-x. We note that the angle coverage of a PBS decreases with shorter temporal scale, but the occurrence of the PBSs is independent of θxB. Suspecting that the isolated small PBSs are formed by compressive <span class="hlt">waves</span> in situ, we continue this study by testing the <span class="hlt">wave</span> modes forming a small-scale PBS with B 0(s, t) quasi-parallel to GSE-x. As a result, we identify that the cross-helicity and the compressibility attain values for a slow mode from theoretical calculations. The <span class="hlt">wave</span> vector is derived from minimum variance analysis. Besides, the proton temperatures obey T < T ∥ derived from the velocity distribution functions, excluding a mirror mode, which is the other candidate for the formation of PBSs in situ. Thus, a small-scale PBS is shown to be driven by oblique, slow-mode <span class="hlt">waves</span> in the solar wind.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140003749','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140003749"><span>Modified ACES <span class="hlt">Portable</span> Life Support Integration, Design, and Testing for Exploration Missions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kelly, Cody</p> <p>2014-01-01</p> <p>NASA's next generation of exploration missions provide a unique challenge to designers of EVA life support equipment, especially in a fiscally-constrained environment. In order to take the next steps of manned space exploration, NASA is currently evaluating the use of the Modified ACES (MACES) suit in conjunction with the Advanced <span class="hlt">Portable</span> Life Support System (PLSS) currently under development. This paper will detail the analysis and integration of the PLSS thermal and ventilation subsystems into the MACES <span class="hlt">pressure</span> garment, design of prototype hardware, and hardware-in-the-loop testing during the spring 2014 timeframe. Prototype hardware was designed with a minimal impact philosophy in order to mitigate design constraints becoming levied on either the advanced PLSS or MACES subsystems. Among challenges faced by engineers were incorporation of life support thermal water systems into the <span class="hlt">pressure</span> garment cavity, operational concept definition between vehicle/<span class="hlt">portable</span> life support system hardware, and structural attachment mechanisms while still enabling maximum EVA efficiency from a crew member's perspective. Analysis was completed in late summer 2013 to 'bound' hardware development, with iterative analysis cycles throughout the hardware development process. The design effort will cumulate in the first ever manned integration of NASA's advanced PLSS system with a <span class="hlt">pressure</span> garment originally intended primarily for use in a contingency survival scenario.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900054827&hterms=function+wave&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dfunction%2Bwave','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900054827&hterms=function+wave&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dfunction%2Bwave"><span>Lower solar chromosphere-corona transition region. II - <span class="hlt">Wave</span> <span class="hlt">pressure</span> effects for a specific form of the heating function</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Woods, D. Tod; Holzer, Thomas E.; Macgregor, Keith B.</p> <p>1990-01-01</p> <p>Lower transition region models with a balance between mechanical heating and radiative losses are expanded to include <span class="hlt">wave</span> <span class="hlt">pressure</span> effects. The models are used to study the simple damping length form of the heating function. The results are compared to the results obtained by Woods et al. (1990) for solutions in the lower transition region. The results suggest that a mixture of fast-mode and slow-mode <span class="hlt">waves</span> may provide the appropriate heating mechanism in the lower transition region, with the decline in effective vertical <span class="hlt">wave</span> speed caused by the refraction and eventual total reflection of the fast-mode <span class="hlt">wave</span> resulting from the decreasing atmospheric density.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22482623-peristaltic-pump-based-low-range-pressure-sensor-calibration-system','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22482623-peristaltic-pump-based-low-range-pressure-sensor-calibration-system"><span>Peristaltic pump-based low range <span class="hlt">pressure</span> sensor calibration 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>Vinayakumar, K. B.; Department of Electronic Systems Engineering, Indian Institute of Science, Bangalore 5600012; Naveen Kumar, G.</p> <p>2015-11-15</p> <p>Peristaltic pumps were normally used to pump liquids in several chemical and biological applications. In the present study, a peristaltic pump was used to <span class="hlt">pressurize</span> the chamber (positive as well negative <span class="hlt">pressures</span>) using atmospheric air. In the present paper, we discuss the development and performance study of an automatic <span class="hlt">pressurization</span> system to calibrate low range (millibar) <span class="hlt">pressure</span> sensors. The system includes a peristaltic pump, calibrated <span class="hlt">pressure</span> sensor (master sensor), <span class="hlt">pressure</span> chamber, and the control electronics. An in-house developed peristaltic pump was used to <span class="hlt">pressurize</span> the chamber. A closed loop control system has been developed to detect and adjust the pressuremore » leaks in the chamber. The complete system has been integrated into a <span class="hlt">portable</span> product. The system performance has been studied for a step response and steady state errors. The system is <span class="hlt">portable</span>, free from oil contaminants, and consumes less power compared to existing <span class="hlt">pressure</span> calibration systems. The veracity of the system was verified by calibrating an unknown diaphragm based <span class="hlt">pressure</span> sensor and the results obtained were satisfactory.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ExFl...59..100C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ExFl...59..100C"><span>Kinematics and dynamics of green water on a fixed platform in a large <span class="hlt">wave</span> basin in focusing <span class="hlt">wave</span> and random <span class="hlt">wave</span> conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chuang, Wei-Liang; Chang, Kuang-An; Mercier, Richard</p> <p>2018-06-01</p> <p>Green water kinematics and dynamics due to <span class="hlt">wave</span> impingements on a simplified geometry, fixed platform were experimentally investigated in a large, deep-water <span class="hlt">wave</span> basin. Both plane focusing <span class="hlt">waves</span> and random <span class="hlt">waves</span> were employed in the generation of green water. The focusing <span class="hlt">wave</span> condition was designed to create two consecutive plunging breaking <span class="hlt">waves</span> with one impinging on the frontal vertical wall of the fixed platform, referred as wall impingement, and the other directly impinging on the deck surface, referred as deck impingement. The random <span class="hlt">wave</span> condition was generated using the JONSWAP spectrum with a significant <span class="hlt">wave</span> height approximately equal to the freeboard. A total of 179 green water events were collected in the random <span class="hlt">wave</span> condition. By examining the green water events in random <span class="hlt">waves</span>, three different flow types are categorized: collapse of overtopping <span class="hlt">wave</span>, fall of bulk water, and breaking <span class="hlt">wave</span> crest. The aerated flow velocity was measured using bubble image velocimetry, while the void fraction was measured using fiber optic reflectometry. For the plane focusing <span class="hlt">wave</span> condition, measurements of impact <span class="hlt">pressure</span> were synchronized with the flow velocity and void fraction measurements. The relationship between the peak <span class="hlt">pressures</span> and the <span class="hlt">pressure</span> rise times is examined. For the high-intensity impact in the deck impingement events, the peak <span class="hlt">pressures</span> are observed to be proportional to the aeration levels. The maximum horizontal velocities in the green water events in random <span class="hlt">waves</span> are well represented by the lognormal distribution. Ritter's solution is shown to quantitatively describe the green water velocity distributions under both the focusing <span class="hlt">wave</span> condition and the random <span class="hlt">wave</span> condition. A prediction equation for green water velocity distribution under random <span class="hlt">waves</span> is proposed.</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/2015EGUGA..1714375A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1714375A"><span>Laboratory modeling of edge <span class="hlt">wave</span> generation over a plane beach by breaking <span class="hlt">waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Abcha, Nizar; Ezersky, Alexander; Pelinovsky, Efim</p> <p>2015-04-01</p> <p>Edge <span class="hlt">waves</span> play an important role in coastal hydrodynamics: in sediment transport, in formation of coastline structure and coastal bottom topography. Investigation of physical mechanisms leading to the edge <span class="hlt">waves</span> generation allows us to determine their effect on the characteristics of spatially periodic patterns like crescent submarine bars and cusps observed in the coastal zone. In the present paper we investigate parametric excitation of edge <span class="hlt">wave</span> with frequency two times less than the frequency of surface <span class="hlt">wave</span> propagating perpendicular to the beach. Such mechanism of edge <span class="hlt">wave</span> generation has been studied previously in a large number of papers using the assumption of non-breaking <span class="hlt">waves</span>. This assumption was used in theoretical calculations and such conditions were created in laboratory experiments. In the natural conditions, the <span class="hlt">wave</span> breaking is typical when edge <span class="hlt">waves</span> are generated at sea beach. We study features of such processes in laboratory experiments. Experiments were performed in the <span class="hlt">wave</span> flume of the Laboratory of Continental and Coast Morphodynamics (M2C), Caen. The flume is equipment with a <span class="hlt">wave</span> <span class="hlt">maker</span> controlled by computer. To model a plane beach, a PVC plate is placed at small angle to the horizontal bottom. Several resistive probes were used to measure characteristics of <span class="hlt">waves</span>: one of them was used to measure free surface displacement near the <span class="hlt">wave</span> <span class="hlt">maker</span> and two probes were glued on the inclined plate. These probes allowed us to measure run-up due to parametrically excited edge <span class="hlt">waves</span>. Run-up height is determined by processing a movie shot by high-speed camera. Sub-harmonic generation of standing edge <span class="hlt">waves</span> is observed for definite control parameters: edge <span class="hlt">waves</span> represent themselves a spatial mode with wavelength equal to double width of the flume; the frequency of edge <span class="hlt">wave</span> is equal to half of surface <span class="hlt">wave</span> frequency. Appearance of sub-harmonic mode instability is studied using probes and movie processing. The dependence of edge <span class="hlt">wave</span> exponential</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25219262','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25219262"><span>[Advances of <span class="hlt">portable</span> electrocardiogram monitor design].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ding, Shenping; Wang, Yinghai; Wu, Weirong; Deng, Lingli; Lu, Jidong</p> <p>2014-06-01</p> <p><span class="hlt">Portable</span> electrocardiogram monitor is an important equipment in the clinical diagnosis of cardiovascular diseases due to its <span class="hlt">portable</span>, real-time features. It has a broad application and development prospects in China. In the present review, previous researches on the <span class="hlt">portable</span> electrocardiogram monitors have been arranged, analyzed and summarized. According to the characteristics of the electrocardiogram (ECG), this paper discusses the ergonomic design of the <span class="hlt">portable</span> electrocardiogram monitor, including hardware and software. The circuit components and software modules were parsed from the ECG features and system functions. Finally, the development trend and reference are provided for the <span class="hlt">portable</span> electrocardiogram monitors and for the subsequent research and product design.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100039412','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100039412"><span><span class="hlt">Portable</span> Dew Point Mass Spectrometry System for Real-Time Gas and Moisture Analysis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Arkin, C.; Gillespie, Stacey; Ratzel, Christopher</p> <p>2010-01-01</p> <p>A <span class="hlt">portable</span> instrument incorporates both mass spectrometry and dew point measurement to provide real-time, quantitative gas measurements of helium, nitrogen, oxygen, argon, and carbon dioxide, along with real-time, quantitative moisture analysis. The <span class="hlt">Portable</span> Dew Point Mass Spectrometry (PDP-MS) system comprises a single quadrupole mass spectrometer and a high vacuum system consisting of a turbopump and a diaphragm-backing pump. A capacitive membrane dew point sensor was placed upstream of the MS, but still within the <span class="hlt">pressure</span>-flow control pneumatic region. <span class="hlt">Pressure</span>-flow control was achieved with an upstream precision metering valve, a capacitance diaphragm gauge, and a downstream mass flow controller. User configurable LabVIEW software was developed to provide real-time concentration data for the MS, dew point monitor, and sample delivery system <span class="hlt">pressure</span> control, <span class="hlt">pressure</span> and flow monitoring, and recording. The system has been designed to include in situ, NIST-traceable calibration. Certain sample tubing retains sufficient water that even if the sample is dry, the sample tube will desorb water to an amount resulting in moisture concentration errors up to 500 ppm for as long as 10 minutes. It was determined that Bev-A-Line IV was the best sample line to use. As a result of this issue, it is prudent to add a high-level humidity sensor to PDP-MS so such events can be prevented in the future.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=SPIRAL+AND+MODEL&pg=7&id=EJ730123','ERIC'); return false;" href="https://eric.ed.gov/?q=SPIRAL+AND+MODEL&pg=7&id=EJ730123"><span>The Loss Spiral of Work <span class="hlt">Pressure</span>, Work-Home Interference and Exhaustion: Reciprocal Relations in a Three-<span class="hlt">Wave</span> Study</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Demerouti, Evangelia; Bakker, Arnold B.; Bulters, Annemieke J.</p> <p>2004-01-01</p> <p>This study tested the "loss spiral" hypothesis of work-home interference (WHI). Accordingly, work <span class="hlt">pressure</span> was expected to lead to WHI and exhaustion, and, vice versa, exhaustion was expected to result in more WHI and work <span class="hlt">pressure</span> over time. Results of SEM-analyses using three <span class="hlt">waves</span> of data obtained from 335 employees of an employment agency…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007APS..DFD.BJ001H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007APS..DFD.BJ001H"><span>A midsummer-night's shock <span class="hlt">wave</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hargather, Michael; Liebner, Thomas; Settles, Gary</p> <p>2007-11-01</p> <p>The aerial pyrotechnic shells used in professional display fireworks explode a bursting charge at altitude in order to disperse the ``stars'' of the display. The shock <span class="hlt">wave</span> from the bursting charge is heard on the ground as a loud report, though it has by then typically decayed to a mere sound <span class="hlt">wave</span>. However, viewers seated near the standard safety borders can still be subjected to weak shock <span class="hlt">waves</span>. These have been visualized using a large, <span class="hlt">portable</span>, retro-reflective ``Edgerton'' shadowgraph technique and a high-speed digital video camera. Images recorded at 10,000 frames per second show essentially-planar shock <span class="hlt">waves</span> from 10- and 15-cm firework shells impinging on viewers during the 2007 Central Pennsylvania July 4th Festival. The shock speed is not measurably above Mach 1, but we nonetheless conclude that, if one can sense a shock-like overpressure, then the <span class="hlt">wave</span> motion is strong enough to be observed by density-sensitive optics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Synthesis&pg=3&id=EJ1158887','ERIC'); return false;" href="https://eric.ed.gov/?q=Synthesis&pg=3&id=EJ1158887"><span>Learning through Making and <span class="hlt">Maker</span> Education</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>Hsu, Yu-Chang; Baldwin, Sally; Ching, Yu-Hui</p> <p>2017-01-01</p> <p>In this paper, we provide an overview of the current efforts in <span class="hlt">maker</span> education, supported by a review of empirical studies. Our synthesis will inform the community about learning outcomes, potential and common issues, challenges, resources, and future research direction regarding <span class="hlt">maker</span> education.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29477564','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29477564"><span>Comparison of laboratory and ambulatory measures of central blood <span class="hlt">pressure</span> and pulse <span class="hlt">wave</span> reflection: hitting the target or missing the mark?</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Burns, Matthew J; Seed, Jeremy D; Incognito, Anthony V; Doherty, Connor J; Notay, Karambir; Millar, Philip J</p> <p>2018-04-01</p> <p>Prior studies demonstrating clinical significance of noninvasive estimates of central blood <span class="hlt">pressure</span> (BP) and pulse <span class="hlt">wave</span> reflection have relied primarily on discrete resting measures. The aim of this study was to compare central BP and pulse <span class="hlt">wave</span> reflection measures sampled during a single resting laboratory visit against those obtained under ambulatory conditions. The secondary aim was to investigate the reproducibility of ambulatory central BP and pulse <span class="hlt">wave</span> reflection measurements. Forty healthy participants (21 males; 24 ± 3 years) completed three measurements of brachial artery pulse <span class="hlt">wave</span> analysis (Oscar 2 with SphygmoCor Inside) in the laboratory followed by 24 hours of ambulatory monitoring. Seventeen participants repeated the 24-hour ambulatory monitoring visit after at least 1 week. Ambulatory measures were divided into daytime (9 AM-9 PM), nighttime (1 AM-6 AM), and 24-hour periods. Compared with laboratory measurements, central systolic BP, augmentation <span class="hlt">pressure</span>, and augmentation index (with and without heart rate normalization) were higher (all P < .01) during daytime and 24-hour periods but lower during the nighttime period (all P < .001). The drop in nighttime brachial systolic BP was larger than central systolic <span class="hlt">pressure</span> (Δ -20 ± 6 vs. -15 ± 6 mm Hg; P < .0001). Repeat ambulatory measurements of central BP and pulse <span class="hlt">wave</span> reflection displayed good-to-excellent intraclass correlation coefficients (r = 0.58-0.86; all P < .01), although measures of pulse <span class="hlt">wave</span> reflection had higher coefficients of variation (14%-41%). The results highlight absolute differences in central BP and pulse <span class="hlt">wave</span> reflection between discrete laboratory and ambulatory conditions. The use of ambulatory measures of central BP and pulse <span class="hlt">wave</span> reflection warrant further investigation for clinical prognostic value. Copyright © 2018 American Heart Association. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title47-vol3/pdf/CFR-2010-title47-vol3-sec51-203.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title47-vol3/pdf/CFR-2010-title47-vol3-sec51-203.pdf"><span>47 CFR 51.203 - Number <span class="hlt">portability</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 47 Telecommunication 3 2010-10-01 2010-10-01 false Number <span class="hlt">portability</span>. 51.203 Section 51.203 Telecommunication FEDERAL COMMUNICATIONS COMMISSION (CONTINUED) COMMON CARRIER SERVICES (CONTINUED) INTERCONNECTION Obligations of All Local Exchange Carriers § 51.203 Number <span class="hlt">portability</span>. The rules governing number <span class="hlt">portability</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title47-vol3/pdf/CFR-2012-title47-vol3-sec51-203.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title47-vol3/pdf/CFR-2012-title47-vol3-sec51-203.pdf"><span>47 CFR 51.203 - Number <span class="hlt">portability</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... 47 Telecommunication 3 2012-10-01 2012-10-01 false Number <span class="hlt">portability</span>. 51.203 Section 51.203 Telecommunication FEDERAL COMMUNICATIONS COMMISSION (CONTINUED) COMMON CARRIER SERVICES (CONTINUED) INTERCONNECTION Obligations of All Local Exchange Carriers § 51.203 Number <span class="hlt">portability</span>. The rules governing number <span class="hlt">portability</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title47-vol3/pdf/CFR-2014-title47-vol3-sec51-203.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title47-vol3/pdf/CFR-2014-title47-vol3-sec51-203.pdf"><span>47 CFR 51.203 - Number <span class="hlt">portability</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-10-01</p> <p>... 47 Telecommunication 3 2014-10-01 2014-10-01 false Number <span class="hlt">portability</span>. 51.203 Section 51.203 Telecommunication FEDERAL COMMUNICATIONS COMMISSION (CONTINUED) COMMON CARRIER SERVICES (CONTINUED) INTERCONNECTION Obligations of All Local Exchange Carriers § 51.203 Number <span class="hlt">portability</span>. The rules governing number <span class="hlt">portability</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title47-vol3/pdf/CFR-2011-title47-vol3-sec51-203.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title47-vol3/pdf/CFR-2011-title47-vol3-sec51-203.pdf"><span>47 CFR 51.203 - Number <span class="hlt">portability</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-10-01</p> <p>... 47 Telecommunication 3 2011-10-01 2011-10-01 false Number <span class="hlt">portability</span>. 51.203 Section 51.203 Telecommunication FEDERAL COMMUNICATIONS COMMISSION (CONTINUED) COMMON CARRIER SERVICES (CONTINUED) INTERCONNECTION Obligations of All Local Exchange Carriers § 51.203 Number <span class="hlt">portability</span>. The rules governing number <span class="hlt">portability</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title47-vol3/pdf/CFR-2013-title47-vol3-sec51-203.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title47-vol3/pdf/CFR-2013-title47-vol3-sec51-203.pdf"><span>47 CFR 51.203 - Number <span class="hlt">portability</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... 47 Telecommunication 3 2013-10-01 2013-10-01 false Number <span class="hlt">portability</span>. 51.203 Section 51.203 Telecommunication FEDERAL COMMUNICATIONS COMMISSION (CONTINUED) COMMON CARRIER SERVICES (CONTINUED) INTERCONNECTION Obligations of All Local Exchange Carriers § 51.203 Number <span class="hlt">portability</span>. The rules governing number <span class="hlt">portability</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/381051','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/381051"><span><span class="hlt">Pressure</span> <span class="hlt">waves</span> in liquid mercury target from pulsed heat loads and the possible way controlling their effects</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>Ni, L.; Skala, K.</p> <p>1996-06-01</p> <p>In ESS project liquid metals are selected as the main target for the pulsed spallation neutron source. Since the very high instantaneous energy is deposited on the heavy molten target in a very short period time, <span class="hlt">pressure</span> <span class="hlt">waves</span> are generated. They travel through the liquid and cause high stress in the container. Also, additional stress should be considered in the wall which is the result of direct heating of the target window. These dynamic processes were simulated with computational codes with the static response being analized first. The total resulting dynamic wall stress has been found to have exceeded themore » design stress for the selected container material. Adding a small amount of gas bubbles in the liquid could be a possible way to reduce the <span class="hlt">pressure</span> <span class="hlt">waves</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title46-vol7/pdf/CFR-2013-title46-vol7-sec182-458.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title46-vol7/pdf/CFR-2013-title46-vol7-sec182-458.pdf"><span>46 CFR 182.458 - <span class="hlt">Portable</span> fuel systems.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... 46 Shipping 7 2013-10-01 2013-10-01 false <span class="hlt">Portable</span> fuel systems. 182.458 Section 182.458 Shipping...) MACHINERY INSTALLATION Specific Machinery Requirements § 182.458 <span class="hlt">Portable</span> fuel systems. (a) <span class="hlt">Portable</span> fuel systems, including <span class="hlt">portable</span> tanks and related fuel lines and accessories, are prohibited except where used...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol7/pdf/CFR-2010-title46-vol7-sec182-458.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol7/pdf/CFR-2010-title46-vol7-sec182-458.pdf"><span>46 CFR 182.458 - <span class="hlt">Portable</span> fuel systems.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 46 Shipping 7 2010-10-01 2010-10-01 false <span class="hlt">Portable</span> fuel systems. 182.458 Section 182.458 Shipping...) MACHINERY INSTALLATION Specific Machinery Requirements § 182.458 <span class="hlt">Portable</span> fuel systems. (a) <span class="hlt">Portable</span> fuel systems, including <span class="hlt">portable</span> tanks and related fuel lines and accessories, are prohibited except where used...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title46-vol7/pdf/CFR-2011-title46-vol7-sec182-458.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title46-vol7/pdf/CFR-2011-title46-vol7-sec182-458.pdf"><span>46 CFR 182.458 - <span class="hlt">Portable</span> fuel systems.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-10-01</p> <p>... 46 Shipping 7 2011-10-01 2011-10-01 false <span class="hlt">Portable</span> fuel systems. 182.458 Section 182.458 Shipping...) MACHINERY INSTALLATION Specific Machinery Requirements § 182.458 <span class="hlt">Portable</span> fuel systems. (a) <span class="hlt">Portable</span> fuel systems, including <span class="hlt">portable</span> tanks and related fuel lines and accessories, are prohibited except where used...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol7/pdf/CFR-2010-title46-vol7-sec169-743.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol7/pdf/CFR-2010-title46-vol7-sec169-743.pdf"><span>46 CFR 169.743 - <span class="hlt">Portable</span> magazine chests.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 46 Shipping 7 2010-10-01 2010-10-01 false <span class="hlt">Portable</span> magazine chests. 169.743 Section 169.743... Vessel Control, Miscellaneous Systems, and Equipment Markings § 169.743 <span class="hlt">Portable</span> magazine chests. <span class="hlt">Portable</span> magazine chests must be marked in letters at least 3 inches high: “<span class="hlt">PORTABLE</span> MAGAZINE CHEST...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title49-vol3/pdf/CFR-2012-title49-vol3-sec180-605.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title49-vol3/pdf/CFR-2012-title49-vol3-sec180-605.pdf"><span>49 CFR 180.605 - Requirements for periodic testing, inspection and repair of <span class="hlt">portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... repair of <span class="hlt">portable</span> tanks. 180.605 Section 180.605 Transportation Other Regulations Relating to... leakage or cracks near areas of stress concentration due to cooling metal shrinkage in welding operations, sharp fillets, reversal of stresses, or otherwise. No field welding may be done except to non-<span class="hlt">pressure</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title49-vol3/pdf/CFR-2014-title49-vol3-sec180-605.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title49-vol3/pdf/CFR-2014-title49-vol3-sec180-605.pdf"><span>49 CFR 180.605 - Requirements for periodic testing, inspection and repair of <span class="hlt">portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-10-01</p> <p>... repair of <span class="hlt">portable</span> tanks. 180.605 Section 180.605 Transportation Other Regulations Relating to... leakage or cracks near areas of stress concentration due to cooling metal shrinkage in welding operations, sharp fillets, reversal of stresses, or otherwise. No field welding may be done except to non-<span class="hlt">pressure</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title49-vol3/pdf/CFR-2011-title49-vol3-sec180-605.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title49-vol3/pdf/CFR-2011-title49-vol3-sec180-605.pdf"><span>49 CFR 180.605 - Requirements for periodic testing, inspection and repair of <span class="hlt">portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-10-01</p> <p>... repair of <span class="hlt">portable</span> tanks. 180.605 Section 180.605 Transportation Other Regulations Relating to... leakage or cracks near areas of stress concentration due to cooling metal shrinkage in welding operations, sharp fillets, reversal of stresses, or otherwise. No field welding may be done except to non-<span class="hlt">pressure</span>...</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_14 --> <div id="page_15" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="281"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title49-vol3/pdf/CFR-2013-title49-vol3-sec180-605.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title49-vol3/pdf/CFR-2013-title49-vol3-sec180-605.pdf"><span>49 CFR 180.605 - Requirements for periodic testing, inspection and repair of <span class="hlt">portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... repair of <span class="hlt">portable</span> tanks. 180.605 Section 180.605 Transportation Other Regulations Relating to... leakage or cracks near areas of stress concentration due to cooling metal shrinkage in welding operations, sharp fillets, reversal of stresses, or otherwise. No field welding may be done except to non-<span class="hlt">pressure</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title48-vol6/pdf/CFR-2010-title48-vol6-sec1837-170.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title48-vol6/pdf/CFR-2010-title48-vol6-sec1837-170.pdf"><span>48 CFR 1837.170 - Pension <span class="hlt">portability</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 48 Federal Acquisition Regulations System 6 2010-10-01 2010-10-01 true Pension <span class="hlt">portability</span>. 1837... ADMINISTRATION SPECIAL CATEGORIES OF CONTRACTING SERVICE CONTRACTING Service Contracts-General 1837.170 Pension <span class="hlt">portability</span>. (a) It is NASA's policy not to require pension <span class="hlt">portability</span> in service contracts. However, pension...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15148018','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15148018"><span><span class="hlt">Portable</span> classroom leads to partnership.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Le Ber, Jeanne Marie; Lombardo, Nancy T; Weber, Alice; Bramble, John</p> <p>2004-01-01</p> <p>Library faculty participation on the School of Medicine Curriculum Steering Committee led to a unique opportunity to partner technology and teaching utilizing the library's <span class="hlt">portable</span> wireless classroom. The pathology lab course master expressed a desire to revise the curriculum using patient cases and direct access to the Web and library resources. Since the pathology lab lacked computers, the library's <span class="hlt">portable</span> wireless classroom provided a solution. Originally developed to provide maximum <span class="hlt">portability</span> and flexibility, the wireless classroom consists of ten laptop computers configured with wireless cards and an access point. While the <span class="hlt">portable</span> wireless classroom led to a partnership with the School of Medicine, there were additional benefits and positive consequences for the library.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title46-vol7/pdf/CFR-2014-title46-vol7-sec195-11-30.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title46-vol7/pdf/CFR-2014-title46-vol7-sec195-11-30.pdf"><span>46 CFR 195.11-30 - <span class="hlt">Portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-10-01</p> <p>... 46 Shipping 7 2014-10-01 2014-10-01 false <span class="hlt">Portable</span> tanks. 195.11-30 Section 195.11-30 Shipping... AND MISCELLANEOUS SYSTEMS AND EQUIPMENT <span class="hlt">Portable</span> Vans and Tanks § 195.11-30 <span class="hlt">Portable</span> tanks. (a) All <span class="hlt">portable</span> tanks, whether hazardous or nonhazardous commodities, shall be loaded and stowed in accordance...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title46-vol7/pdf/CFR-2013-title46-vol7-sec195-11-30.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title46-vol7/pdf/CFR-2013-title46-vol7-sec195-11-30.pdf"><span>46 CFR 195.11-30 - <span class="hlt">Portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... 46 Shipping 7 2013-10-01 2013-10-01 false <span class="hlt">Portable</span> tanks. 195.11-30 Section 195.11-30 Shipping... AND MISCELLANEOUS SYSTEMS AND EQUIPMENT <span class="hlt">Portable</span> Vans and Tanks § 195.11-30 <span class="hlt">Portable</span> tanks. (a) All <span class="hlt">portable</span> tanks, whether hazardous or nonhazardous commodities, shall be loaded and stowed in accordance...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol7/pdf/CFR-2010-title46-vol7-sec195-11-30.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol7/pdf/CFR-2010-title46-vol7-sec195-11-30.pdf"><span>46 CFR 195.11-30 - <span class="hlt">Portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 46 Shipping 7 2010-10-01 2010-10-01 false <span class="hlt">Portable</span> tanks. 195.11-30 Section 195.11-30 Shipping... AND MISCELLANEOUS SYSTEMS AND EQUIPMENT <span class="hlt">Portable</span> Vans and Tanks § 195.11-30 <span class="hlt">Portable</span> tanks. (a) All <span class="hlt">portable</span> tanks, whether hazardous or nonhazardous commodities, shall be loaded and stowed in accordance...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title46-vol7/pdf/CFR-2011-title46-vol7-sec195-11-30.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title46-vol7/pdf/CFR-2011-title46-vol7-sec195-11-30.pdf"><span>46 CFR 195.11-30 - <span class="hlt">Portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-10-01</p> <p>... 46 Shipping 7 2011-10-01 2011-10-01 false <span class="hlt">Portable</span> tanks. 195.11-30 Section 195.11-30 Shipping... AND MISCELLANEOUS SYSTEMS AND EQUIPMENT <span class="hlt">Portable</span> Vans and Tanks § 195.11-30 <span class="hlt">Portable</span> tanks. (a) All <span class="hlt">portable</span> tanks, whether hazardous or nonhazardous commodities, shall be loaded and stowed in accordance...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title46-vol7/pdf/CFR-2012-title46-vol7-sec195-11-30.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title46-vol7/pdf/CFR-2012-title46-vol7-sec195-11-30.pdf"><span>46 CFR 195.11-30 - <span class="hlt">Portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... 46 Shipping 7 2012-10-01 2012-10-01 false <span class="hlt">Portable</span> tanks. 195.11-30 Section 195.11-30 Shipping... AND MISCELLANEOUS SYSTEMS AND EQUIPMENT <span class="hlt">Portable</span> Vans and Tanks § 195.11-30 <span class="hlt">Portable</span> tanks. (a) All <span class="hlt">portable</span> tanks, whether hazardous or nonhazardous commodities, shall be loaded and stowed in accordance...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol4/pdf/CFR-2010-title46-vol4-sec108-651.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol4/pdf/CFR-2010-title46-vol4-sec108-651.pdf"><span>46 CFR 108.651 - <span class="hlt">Portable</span> magazine chests.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 46 Shipping 4 2010-10-01 2010-10-01 false <span class="hlt">Portable</span> magazine chests. 108.651 Section 108.651... AND EQUIPMENT Equipment Markings and Instructions § 108.651 <span class="hlt">Portable</span> magazine chests. Each <span class="hlt">portable</span> magazine chest must be marked: “<span class="hlt">PORTABLE</span> MAGAZINE CHEST—FLAMMABLE—KEEP LIGHTS AND FIRE AWAY” in letters at...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29691642','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29691642"><span>Left atrial <span class="hlt">pressure</span> pattern without a-<span class="hlt">wave</span> in sinus rhythm after cardioversion affects the outcomes after catheter ablation for atrial fibrillation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kishima, Hideyuki; Mine, Takanao; Takahashi, Satoshi; Ashida, Kenki; Ishihara, Masaharu; Masuyama, Tohru</p> <p>2018-04-24</p> <p>The a-<span class="hlt">wave</span> in left atrial <span class="hlt">pressure</span> (LAP) is often not observed after cardioversion (CV). We hypothesized that repeated atrial fibrillation (AF) occurs in patients who do not show a-<span class="hlt">wave</span> pattern after CV. We investigated the impact of "LAP pattern without a-<span class="hlt">wave</span>" on the outcome after catheter ablation (CA) for AF. We studied 100 patients (64 males, age 66 ± 8 years, 42 with non-paroxysmal AF) who underwent CA for AF. Sustained- or induced-AF were terminated with internal CV, and LAP was measured during sinus rhythm (SR) after CV. LAP pattern without a-<span class="hlt">wave</span> was defined as absence of a-<span class="hlt">wave</span> (the "a-<span class="hlt">wave</span>" was defined as a protruding part by 0.2 mmHg or more from the baseline) in LAP <span class="hlt">wave</span> form. AF was terminated with CV in all patients. Recurrent AF was detected in 35/100 (35%) during the follow-up period (13.1 ± 7.8 month). Univariate analysis revealed higher prevalence of LAP pattern without a-<span class="hlt">wave</span> (71 vs. 17%, P < 0.0001), larger left atrial volume, elevated E <span class="hlt">wave</span>, and decreased deceleration time as significant variables. On multivariate analysis, LAP pattern without a-<span class="hlt">wave</span> was only independently associated with recurrent AF (P = 0.0014, OR 9.865, 95% CI 2.327-54.861). Moreover, patients with LAP pattern without a-<span class="hlt">wave</span> had a higher risk of recurrent AF than patients with a-<span class="hlt">wave</span> (25/36 patients, 69 vs. 10/64 patients, 16%, log-rank P < 0.0001). Left atrial <span class="hlt">pressure</span> pattern without a-<span class="hlt">wave</span> in sinus rhythm after cardioversion could predict recurrence after catheter ablation for AF.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004ITEIS.124.2427F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004ITEIS.124.2427F"><span>Thermal Index Evaluation of Local SAR in MRI-Based Head Models of Adult and Children for <span class="hlt">Portable</span> Telephones</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fujiwara, Osamu; Miyamoto, Kayoko; Wang, Jianqing</p> <p></p> <p>Biological hazards due to radio-frequency (RF) <span class="hlt">waves</span> result mainly from the temperature rise in tissue. It should be, therefore, clarified to what extent the RF <span class="hlt">waves</span> of <span class="hlt">portable</span> telephones increase the temperature-rise in human brain that includes the central part governing the body-temperature regulation function. In this paper, we calculated both the specific absorption rate (SAR) and the resultant temperature-rise for 900 MHz and 2 GHz <span class="hlt">portable</span> telephones using the finite-difference time-domain (FDTD) method for three typical use positions, i.e., the vertical position, cheek position and tilt position. As a result, we found that there was an increase for median and 1% value of the cumulative distribution of temperature-rise in children’s brains for any use positions of the <span class="hlt">portable</span> telephones compared to that in the adult’s brain, and also that the increasing trend in children’s brains for temperature-rise is identical to the temperature-rise trend in children’s hypothalamus. In addition, we found that the ten-gram averaged peak SAR among the adult and children heads had the same trend as that of the 0.1% value of the relatively cumulative distribution of temperature-rise, which shows that the ten-gram averaged peak SAR reflects only the localized temperature-rise in the brain surface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title49-vol2/pdf/CFR-2014-title49-vol2-sec174-63.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title49-vol2/pdf/CFR-2014-title49-vol2-sec174-63.pdf"><span>49 CFR 174.63 - <span class="hlt">Portable</span> tanks, IM <span class="hlt">portable</span> tanks, IBCs, Large Packagings, cargo tanks, and multi-unit tank car...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-10-01</p> <p>... 49 Transportation 2 2014-10-01 2014-10-01 false <span class="hlt">Portable</span> tanks, IM <span class="hlt">portable</span> tanks, IBCs, Large Packagings, cargo tanks, and multi-unit tank car tanks. 174.63 Section 174.63 Transportation Other....63 <span class="hlt">Portable</span> tanks, IM <span class="hlt">portable</span> tanks, IBCs, Large Packagings, cargo tanks, and multi-unit tank car...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title49-vol2/pdf/CFR-2010-title49-vol2-sec174-63.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title49-vol2/pdf/CFR-2010-title49-vol2-sec174-63.pdf"><span>49 CFR 174.63 - <span class="hlt">Portable</span> tanks, IM <span class="hlt">portable</span> tanks, IBCs, Large Packagings, cargo tanks, and multi-unit tank car...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 49 Transportation 2 2010-10-01 2010-10-01 false <span class="hlt">Portable</span> tanks, IM <span class="hlt">portable</span> tanks, IBCs, Large Packagings, cargo tanks, and multi-unit tank car tanks. 174.63 Section 174.63 Transportation Other....63 <span class="hlt">Portable</span> tanks, IM <span class="hlt">portable</span> tanks, IBCs, Large Packagings, cargo tanks, and multi-unit tank car...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title49-vol2/pdf/CFR-2011-title49-vol2-sec174-63.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title49-vol2/pdf/CFR-2011-title49-vol2-sec174-63.pdf"><span>49 CFR 174.63 - <span class="hlt">Portable</span> tanks, IM <span class="hlt">portable</span> tanks, IBCs, Large Packagings, cargo tanks, and multi-unit tank car...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-10-01</p> <p>... 49 Transportation 2 2011-10-01 2011-10-01 false <span class="hlt">Portable</span> tanks, IM <span class="hlt">portable</span> tanks, IBCs, Large Packagings, cargo tanks, and multi-unit tank car tanks. 174.63 Section 174.63 Transportation Other....63 <span class="hlt">Portable</span> tanks, IM <span class="hlt">portable</span> tanks, IBCs, Large Packagings, cargo tanks, and multi-unit tank car...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title49-vol2/pdf/CFR-2013-title49-vol2-sec174-63.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title49-vol2/pdf/CFR-2013-title49-vol2-sec174-63.pdf"><span>49 CFR 174.63 - <span class="hlt">Portable</span> tanks, IM <span class="hlt">portable</span> tanks, IBCs, Large Packagings, cargo tanks, and multi-unit tank car...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... 49 Transportation 2 2013-10-01 2013-10-01 false <span class="hlt">Portable</span> tanks, IM <span class="hlt">portable</span> tanks, IBCs, Large Packagings, cargo tanks, and multi-unit tank car tanks. 174.63 Section 174.63 Transportation Other....63 <span class="hlt">Portable</span> tanks, IM <span class="hlt">portable</span> tanks, IBCs, Large Packagings, cargo tanks, and multi-unit tank car...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title49-vol2/pdf/CFR-2012-title49-vol2-sec174-63.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title49-vol2/pdf/CFR-2012-title49-vol2-sec174-63.pdf"><span>49 CFR 174.63 - <span class="hlt">Portable</span> tanks, IM <span class="hlt">portable</span> tanks, IBCs, Large Packagings, cargo tanks, and multi-unit tank car...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... 49 Transportation 2 2012-10-01 2012-10-01 false <span class="hlt">Portable</span> tanks, IM <span class="hlt">portable</span> tanks, IBCs, Large Packagings, cargo tanks, and multi-unit tank car tanks. 174.63 Section 174.63 Transportation Other....63 <span class="hlt">Portable</span> tanks, IM <span class="hlt">portable</span> tanks, IBCs, Large Packagings, cargo tanks, and multi-unit tank car...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4297358','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4297358"><span>Novel <span class="hlt">wave</span> intensity analysis of arterial pulse <span class="hlt">wave</span> propagation accounting for peripheral reflections</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Alastruey, Jordi; Hunt, Anthony A E; Weinberg, Peter D</p> <p>2014-01-01</p> <p>We present a novel analysis of arterial pulse <span class="hlt">wave</span> propagation that combines traditional <span class="hlt">wave</span> intensity analysis with identification of Windkessel <span class="hlt">pressures</span> to account for the effect on the <span class="hlt">pressure</span> waveform of peripheral <span class="hlt">wave</span> reflections. Using haemodynamic data measured in vivo in the rabbit or generated numerically in models of human compliant vessels, we show that traditional <span class="hlt">wave</span> intensity analysis identifies the timing, direction and magnitude of the predominant <span class="hlt">waves</span> that shape aortic <span class="hlt">pressure</span> and flow waveforms in systole, but fails to identify the effect of peripheral reflections. These reflections persist for several cardiac cycles and make up most of the <span class="hlt">pressure</span> waveform, especially in diastole and early systole. Ignoring peripheral reflections leads to an erroneous indication of a reflection-free period in early systole and additional error in the estimates of (i) pulse <span class="hlt">wave</span> velocity at the ascending aorta given by the PU–loop method (9.5% error) and (ii) transit time to a dominant reflection site calculated from the <span class="hlt">wave</span> intensity profile (27% error). These errors decreased to 1.3% and 10%, respectively, when accounting for peripheral reflections. Using our new analysis, we investigate the effect of vessel compliance and peripheral resistance on <span class="hlt">wave</span> intensity, peripheral reflections and reflections originating in previous cardiac cycles. PMID:24132888</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19960009427','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19960009427"><span>Control and reduction of unsteady <span class="hlt">pressure</span> loads in separated shock <span class="hlt">wave</span> turbulent boundary layer interaction</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dolling, David S.; Barter, John W.</p> <p>1995-01-01</p> <p>The focus was on developing means of controlling and reducing unsteady <span class="hlt">pressure</span> loads in separated shock <span class="hlt">wave</span> turbulent boundary layer interactions. Section 1 describes how vortex generators can be used to effectively reduce loads in compression ramp interaction, while Section 2 focuses on the effects of 'boundary-layer separators' on the same interaction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20030004801','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20030004801"><span><span class="hlt">Portable</span> Dental System</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1980-01-01</p> <p><span class="hlt">Portable</span> dental system provides dental care in isolated communities. System includes a patient's chair and a dentist's stool, an X-ray machine and a power unit, all of which fold into compact packages. A large yellow "pumpkin" is a collapsible compressed air tank. <span class="hlt">Portable</span> system has been used successfully in South America in out of the way communities with this back-packable system, and in American nursing homes. This product is no longer manufactured.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-201406180005HQ.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-201406180005HQ.html"><span>White House <span class="hlt">Maker</span> Faire</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2014-06-18</p> <p>The <span class="hlt">Maker</span> Faire trailer is seen outside the rose garden during the first ever White House <span class="hlt">Maker</span> Faire, which brings together students, entrepreneurs, and everyday citizens who are using new tools and techniques to launch new businesses, learn vital skills in science, technology, engineering, and math (STEM), and fuel the renaissance in American manufacturing, at the White House, Wednesday, June 18, 2014 in Washington. The President announced new steps the Administration and its partners are taking to support the ability of more Americans, young and old, to have to access to these tools and techniques and brings their ideas to life. Photo Credit: (NASA/Bill Ingalls)</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_15 --> <div id="page_16" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="301"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/875065','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/875065"><span>Human <span class="hlt">portable</span> preconcentrator system</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Linker, Kevin L.; Bouchier, Francis A.; Hannum, David W.; Rhykerd, Jr., Charles L.</p> <p>2003-01-01</p> <p>A preconcentrator system and apparatus suited to human <span class="hlt">portable</span> use wherein sample potentially containing a target chemical substance is drawn into a chamber and through a pervious screen. The screen is adapted to capture target chemicals and then, upon heating, to release those chemicals into the chamber. Chemicals captured and then released in this fashion are then carried to a <span class="hlt">portable</span> chemical detection device such as a <span class="hlt">portable</span> ion mobility spectrometer. In the preferred embodiment, the means for drawing sample into the chamber comprises a reversible fan which, when operated in reverse direction, creates a backpressure that facilitates evolution of captured target chemicals into the chamber when the screen is heated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015OptEn..54b5111B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015OptEn..54b5111B"><span>Deflectometry using <span class="hlt">portable</span> devices</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Butel, Guillaume P.; Smith, Greg A.; Burge, James H.</p> <p>2015-02-01</p> <p>Deflectometry is a powerful metrology technique that uses off-the-shelf equipment to achieve nanometer-level accuracy surface measurements. However, there is no <span class="hlt">portable</span> device to quickly measure eyeglasses, lenses, or mirrors. We present an entirely <span class="hlt">portable</span> new deflectometry technique that runs on any Android™ smartphone with a front-facing camera. Our technique overcomes some specific issues of <span class="hlt">portable</span> devices like screen nonlinearity and automatic gain control. We demonstrate our application by measuring an amateur telescope mirror and simulating a measurement of the faulty Hubble Space Telescope primary mirror. Our technique can, in less than 1 min, measure surface errors with accuracy up to 50 nm RMS, simply using a smartphone.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title49-vol2/pdf/CFR-2012-title49-vol2-sec172-326.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title49-vol2/pdf/CFR-2012-title49-vol2-sec172-326.pdf"><span>49 CFR 172.326 - <span class="hlt">Portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... 49 Transportation 2 2012-10-01 2012-10-01 false <span class="hlt">Portable</span> tanks. 172.326 Section 172.326... SECURITY PLANS Marking § 172.326 <span class="hlt">Portable</span> tanks. (a) Shipping name. No person may offer for transportation or transport a <span class="hlt">portable</span> tank containing a hazardous material unless it is legibly marked on two...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title49-vol2/pdf/CFR-2013-title49-vol2-sec172-326.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title49-vol2/pdf/CFR-2013-title49-vol2-sec172-326.pdf"><span>49 CFR 172.326 - <span class="hlt">Portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... 49 Transportation 2 2013-10-01 2013-10-01 false <span class="hlt">Portable</span> tanks. 172.326 Section 172.326... SECURITY PLANS Marking § 172.326 <span class="hlt">Portable</span> tanks. (a) Shipping name. No person may offer for transportation or transport a <span class="hlt">portable</span> tank containing a hazardous material unless it is legibly marked on two...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title49-vol2/pdf/CFR-2014-title49-vol2-sec172-326.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title49-vol2/pdf/CFR-2014-title49-vol2-sec172-326.pdf"><span>49 CFR 172.326 - <span class="hlt">Portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-10-01</p> <p>... 49 Transportation 2 2014-10-01 2014-10-01 false <span class="hlt">Portable</span> tanks. 172.326 Section 172.326... SECURITY PLANS Marking § 172.326 <span class="hlt">Portable</span> tanks. (a) Shipping name. No person may offer for transportation or transport a <span class="hlt">portable</span> tank containing a hazardous material unless it is legibly marked on two...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title49-vol2/pdf/CFR-2011-title49-vol2-sec172-326.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title49-vol2/pdf/CFR-2011-title49-vol2-sec172-326.pdf"><span>49 CFR 172.326 - <span class="hlt">Portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-10-01</p> <p>... 49 Transportation 2 2011-10-01 2011-10-01 false <span class="hlt">Portable</span> tanks. 172.326 Section 172.326... SECURITY PLANS Marking § 172.326 <span class="hlt">Portable</span> tanks. (a) Shipping name. No person may offer for transportation or transport a <span class="hlt">portable</span> tank containing a hazardous material unless it is legibly marked on two...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890014040','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890014040"><span>Experimental study of <span class="hlt">pressure</span> and heating rate on a swept cylindrical leading edge resulting from swept shock <span class="hlt">wave</span> interference. 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>Glass, Christopher E.</p> <p>1989-01-01</p> <p>The effects of cylindrical leading edge sweep on surface <span class="hlt">pressure</span> and heat transfer rate for swept shock <span class="hlt">wave</span> interference were investigated. Experimental tests were conducted in the Calspan 48-inch Hypersonic Shock Tunnel at a nominal Mach number of 8, nominal unit Reynolds number of 1.5 x 10 to the 6th power per foot, leading edge and incident shock generator sweep angles of 0, 15, and 30 deg, and incident shock generator angle-of-attack fixed at 12.5 deg. Detailed surface <span class="hlt">pressure</span> and heat transfer rate on the cylindircal leading edge of a swept shock <span class="hlt">wave</span> interference model were measured at the region of the maximum surface <span class="hlt">pressure</span> and heat transfer rate. Results show that <span class="hlt">pressure</span> and heat transfer rate on the cylindrical leading edge of the shock <span class="hlt">wave</span> interference model were reduced as the sweep was increased over the range of tested parameters. Peak surface <span class="hlt">pressure</span> and heat transfer rate on the cylinder were about 10 and 30 times the undisturbed flow stagnation point value, respectively, for the 0 deg sweep test. A comparison of the 15 and 30 deg swept results with the 0 deg swept results showed that peak <span class="hlt">pressure</span> was reduced about 13 percent and 44 percent, respectively, and peak heat transfer rate was reduced about 7 percent and 27 percent, respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22062308-note-portable-light-emitting-diode-based-ruby-fluorescence-spectrometer-high-pressure-calibration','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22062308-note-portable-light-emitting-diode-based-ruby-fluorescence-spectrometer-high-pressure-calibration"><span>Note: A <span class="hlt">portable</span>, light-emitting diode-based ruby fluorescence spectrometer for high-<span class="hlt">pressure</span> calibration</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>Feng Yejun</p> <p>2011-04-15</p> <p>Ruby (Al{sub 2}O{sub 3}, with {approx}0.5 wt. % Cr doping) is one of the most widely used manometers at the giga-Pascal scale. Traditionally, its fluorescence is excited with intense laser sources. Here, I present a simple, robust, and <span class="hlt">portable</span> design that employs light-emitting diodes (LEDs) instead. This LED-based system is safer in comparison with laser-based ones.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..SHK.F9035P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..SHK.F9035P"><span>Numerical Simulation of Laser Ablative Shock <span class="hlt">Waves</span> From Aluminum in Presence of Helium Gas At Different Ambient <span class="hlt">Pressures</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Paturi, Prem Kiran; Durvasula, P. S. L. Kameswari; S, Sai Shiva; Acrhem, University Of Hyderabad Team</p> <p>2017-06-01</p> <p>A two dimensional comparative study of Laser Ablative Shock <span class="hlt">Wave</span> into the Aluminum target in the presence of Helium gas at different ambient <span class="hlt">pressures</span> over a range of 690 - 105 Pa performed using FLASH hydrodynamic codes will be presented. The irradiation of Aluminum target (thickness 2 mm and radius 3 mm) with a 7 ns laser pulse of energy 175 mJ, spot size of 150 µm on the target surface at a wavelength of 532 nm at normal incidence is simulated. Helium gas enclosed in a chamber of height 3 mm and width 3 mm. The electron-ion inverse bremsstrahlung absorption coefficient is considered in the laser energy deposition process. The simulation was performed over a duration of 1 μs. It was observed that an ablative shock is launched into the Helium gas for the <span class="hlt">pressures</span> of 0.5 atm and above. However, for <span class="hlt">pressure</span> less than the 0.5 atm the plasma expanded into the He gas upto 12ns and after which due to <span class="hlt">pressure</span> equilibration with the surroundings and plume splitting shock <span class="hlt">wave</span> is launched in to Al. Authors acknowledge funding from DRDO, India.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/7614499','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/7614499"><span>Reappraisal of quantitative evaluation of pulmonary regurgitation and estimation of pulmonary artery <span class="hlt">pressure</span> by continuous <span class="hlt">wave</span> Doppler echocardiography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lei, M H; Chen, J J; Ko, Y L; Cheng, J J; Kuan, P; Lien, W P</p> <p>1995-01-01</p> <p>This study assessed the usefulness of continuous <span class="hlt">wave</span> Doppler echocardiography and color flow mapping in evaluating pulmonary regurgitation (PR) and estimating pulmonary artery (PA) <span class="hlt">pressure</span>. Forty-three patients were examined, and high quality Doppler spectral recordings of PR were obtained in 32. All patients underwent cardiac catheterization, and simultaneous PA and right ventricular (RV) <span class="hlt">pressures</span> were recorded in 17. Four Doppler regurgitant flow velocity patterns were observed: pandiastolic plateau, biphasic, peak and plateau, and early diastolic triangular types. The peak diastolic and end-diastolic PA-to-RV <span class="hlt">pressure</span> gradients derived from the Doppler flow profiles correlated well with the catheter measurements (r = 0.95 and r = 0.95, respectively). As PA <span class="hlt">pressure</span> increased, the PR flow velocity became higher; a linear relationship between either systolic or mean PA <span class="hlt">pressure</span> and Doppler-derived peak diastolic <span class="hlt">pressure</span> gradient was noted (r = 0.90 and 0.94, respectively). Based on peak diastolic gradients of < 15, 15-30 or > 30 mm Hg, patients could be separated as those with mild, moderate or severe pulmonary hypertension, respectively (p < 0.05). A correlation was also observed between PA diastolic <span class="hlt">pressure</span> and Doppler-derived end-diastolic <span class="hlt">pressure</span> gradient (r = 0.91). Moreover, the Doppler velocity decay slope of PR closely correlated with that derived from the catheter method (r = 0.98). The decay slope tended to be steeper with the increment in regurgitant jet area and length obtained from color flow mapping. In conclusion, continuous <span class="hlt">wave</span> Doppler evaluation of PR is a useful means for noninvasive estimation of PA <span class="hlt">pressure</span>, and the Doppler velocity decay slope seems to reflect the severity of PR.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27959667','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27959667"><span>Bench Evaluation of Four <span class="hlt">Portable</span> Oxygen Concentrators Under Different Conditions Representing Altitudes of 2438, 4200, and 8000 m.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bunel, Vincent; Shoukri, Amr; Choin, Frederic; Roblin, Serge; Smith, Cindy; Similowski, Thomas; Morélot-Panzini, Capucine; Gonzalez, Jesus</p> <p>2016-12-01</p> <p>Bunel, Vincent, Amr Shoukri, Frederic Choin, Serge Roblin, Cindy Smith, Thomas Similowski, Capucine Morélot-Panzini, and Jésus Gonzalez. Bench evaluation of four <span class="hlt">portable</span> oxygen concentrators under different conditions representing altitudes of 2438, 4200, and 8000 m. High Alt Med Biol. 17:370-374, 2016.-Air travel is responsible for a reduction of the partial <span class="hlt">pressure</span> of oxygen (O 2 ) as a result of the decreased barometric <span class="hlt">pressure</span>. This hypobaric hypoxia can be dangerous for passengers with respiratory diseases, requiring initiation or intensification of oxygen therapy during the flight. In-flight oxygen therapy can be provided by <span class="hlt">portable</span> oxygen concentrators, which are less expensive and more practical than oxygen cylinders, but no study has evaluated their capacity to concentrate oxygen under simulated flight conditions. We tested four <span class="hlt">portable</span> oxygen concentrators during a bench test study. The O 2 concentrations (FO 2 ) produced were measured under three different conditions: in room air at sea level, under hypoxia due to a reduction of the partial <span class="hlt">pressure</span> of O 2 (normobaric hypoxia, which can be performed routinely), and under hypoxia due to a reduction of atmospheric <span class="hlt">pressure</span> (hypobaric hypoxia, using a chamber manufactured by Airbus Defence and Space). The FO 2 obtained under conditions of hypobaric hypoxia (chamber) was lower than that measured in room air (0.92 [0.89-0.92] vs. 0.93 [0.92-0.94], p = 0.029), but only one <span class="hlt">portable</span> oxygen concentrator was unable to maintain an FO 2 ≥ 0.90 (0.89 [0.89-0.89]). In contrast, under conditions of normobaric hypoxia (tent) simulating an altitude of 2438 m, none of the apparatuses tested was able to achieve an FO 2 greater than 0.76. (0.75 [0.75-0.76] vs. 0.93 [0.92-0.94], p = 0.029). Almost all <span class="hlt">portable</span> oxygen concentrators were able to generate a sufficient quantity of O 2 at simulated altitudes of 2438 m and can therefore be used in the aircraft cabin. Unfortunately, verification of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol7/pdf/CFR-2010-title46-vol7-sec183-430.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol7/pdf/CFR-2010-title46-vol7-sec183-430.pdf"><span>46 CFR 183.430 - <span class="hlt">Portable</span> lights</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 46 Shipping 7 2010-10-01 2010-10-01 false <span class="hlt">Portable</span> lights 183.430 Section 183.430 Shipping COAST...) ELECTRICAL INSTALLATION Lighting Systems § 183.430 <span class="hlt">Portable</span> lights Each vessel must be equipped with at least two operable <span class="hlt">portable</span> battery lights. One of these lights must be located at the operating station and...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title46-vol7/pdf/CFR-2011-title46-vol7-sec183-430.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title46-vol7/pdf/CFR-2011-title46-vol7-sec183-430.pdf"><span>46 CFR 183.430 - <span class="hlt">Portable</span> lights</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-10-01</p> <p>... 46 Shipping 7 2011-10-01 2011-10-01 false <span class="hlt">Portable</span> lights 183.430 Section 183.430 Shipping COAST...) ELECTRICAL INSTALLATION Lighting Systems § 183.430 <span class="hlt">Portable</span> lights Each vessel must be equipped with at least two operable <span class="hlt">portable</span> battery lights. One of these lights must be located at the operating station and...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title46-vol7/pdf/CFR-2013-title46-vol7-sec183-430.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title46-vol7/pdf/CFR-2013-title46-vol7-sec183-430.pdf"><span>46 CFR 183.430 - <span class="hlt">Portable</span> lights</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... 46 Shipping 7 2013-10-01 2013-10-01 false <span class="hlt">Portable</span> lights 183.430 Section 183.430 Shipping COAST...) ELECTRICAL INSTALLATION Lighting Systems § 183.430 <span class="hlt">Portable</span> lights Each vessel must be equipped with at least two operable <span class="hlt">portable</span> battery lights. One of these lights must be located at the operating station and...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title46-vol7/pdf/CFR-2014-title46-vol7-sec183-430.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title46-vol7/pdf/CFR-2014-title46-vol7-sec183-430.pdf"><span>46 CFR 183.430 - <span class="hlt">Portable</span> lights</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-10-01</p> <p>... 46 Shipping 7 2014-10-01 2014-10-01 false <span class="hlt">Portable</span> lights 183.430 Section 183.430 Shipping COAST...) ELECTRICAL INSTALLATION Lighting Systems § 183.430 <span class="hlt">Portable</span> lights Each vessel must be equipped with at least two operable <span class="hlt">portable</span> battery lights. One of these lights must be located at the operating station and...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title46-vol7/pdf/CFR-2012-title46-vol7-sec183-430.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title46-vol7/pdf/CFR-2012-title46-vol7-sec183-430.pdf"><span>46 CFR 183.430 - <span class="hlt">Portable</span> lights</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... 46 Shipping 7 2012-10-01 2012-10-01 false <span class="hlt">Portable</span> lights 183.430 Section 183.430 Shipping COAST...) ELECTRICAL INSTALLATION Lighting Systems § 183.430 <span class="hlt">Portable</span> lights Each vessel must be equipped with at least two operable <span class="hlt">portable</span> battery lights. One of these lights must be located at the operating station and...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMSH43A..03W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMSH43A..03W"><span>Turbulent Heating and <span class="hlt">Wave</span> <span class="hlt">Pressure</span> in Solar Wind Acceleration Modeling: New Insights to Empirical Forecasting of the Solar Wind</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Woolsey, L. N.; Cranmer, S. R.</p> <p>2013-12-01</p> <p>The study of solar wind acceleration has made several important advances recently due to improvements in modeling techniques. Existing code and simulations test the competing theories for coronal heating, which include reconnection/loop-opening (RLO) models and <span class="hlt">wave</span>/turbulence-driven (WTD) models. In order to compare and contrast the validity of these theories, we need flexible tools that predict the emergent solar wind properties from a wide range of coronal magnetic field structures such as coronal holes, pseudostreamers, and helmet streamers. ZEPHYR (Cranmer et al. 2007) is a one-dimensional magnetohydrodynamics code that includes Alfven <span class="hlt">wave</span> generation and reflection and the resulting turbulent heating to accelerate solar wind in open flux tubes. We present the ZEPHYR output for a wide range of magnetic field geometries to show the effect of the magnetic field profiles on wind properties. We also investigate the competing acceleration mechanisms found in ZEPHYR to determine the relative importance of increased gas <span class="hlt">pressure</span> from turbulent heating and the separate <span class="hlt">pressure</span> source from the Alfven <span class="hlt">waves</span>. To do so, we developed a code that will become publicly available for solar wind prediction. This code, TEMPEST, provides an outflow solution based on only one input: the magnetic field strength as a function of height above the photosphere. It uses correlations found in ZEPHYR between the magnetic field strength at the source surface and the temperature profile of the outflow solution to compute the wind speed profile based on the increased gas <span class="hlt">pressure</span> from turbulent heating. With this initial solution, TEMPEST then adds in the Alfven <span class="hlt">wave</span> <span class="hlt">pressure</span> term to the modified Parker equation and iterates to find a stable solution for the wind speed. This code, therefore, can make predictions of the wind speeds that will be observed at 1 AU based on extrapolations from magnetogram data, providing a useful tool for empirical forecasting of the sol! ar wind.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/ED574761.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/ED574761.pdf"><span>Learning to Program with Game <span class="hlt">Maker</span></span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Johnson, Claire</p> <p>2017-01-01</p> <p>"Game <span class="hlt">Maker</span>" is widely used in UK secondary schools, yet under-researched in that context. This paper presents the findings of a qualitative case study that explores how authoring computer games using "Game <span class="hlt">Maker</span>" can support the learning of basic programming concepts in a mainstream UK secondary setting. The research draws on…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900038569&hterms=marriage&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dmarriage','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900038569&hterms=marriage&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dmarriage"><span>Satellite sound broadcasting system, <span class="hlt">portable</span> reception</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Golshan, Nasser; Vaisnys, Arvydas</p> <p>1990-01-01</p> <p>Studies are underway at JPL in the emerging area of Satellite Sound Broadcast Service (SSBS) for direct reception by low cost <span class="hlt">portable</span>, semi <span class="hlt">portable</span>, mobile and fixed radio receivers. This paper addresses the <span class="hlt">portable</span> reception of digital broadcasting of monophonic audio with source material band limited to 5 KHz (source audio comparable to commercial AM broadcasting). The proposed system provides transmission robustness, uniformity of performance over the coverage area and excellent frequency reuse. Propagation problems associated with indoor <span class="hlt">portable</span> reception are considered in detail and innovative antenna concepts are suggested to mitigate these problems. It is shown that, with the marriage of proper technologies a single medium power satellite can provide substantial direct satellite audio broadcast capability to CONUS in UHF or L Bands, for high quality <span class="hlt">portable</span> indoor reception by low cost radio receivers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol4/pdf/CFR-2010-title46-vol4-sec120-430.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol4/pdf/CFR-2010-title46-vol4-sec120-430.pdf"><span>46 CFR 120.430 - <span class="hlt">Portable</span> lights.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 46 Shipping 4 2010-10-01 2010-10-01 false <span class="hlt">Portable</span> lights. 120.430 Section 120.430 Shipping COAST... Systems § 120.430 <span class="hlt">Portable</span> lights. Each vessel must be equipped with at least two operable <span class="hlt">portable</span> battery lights. One of these lights must be located at the operating station and the other at the access...</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_16 --> <div id="page_17" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="321"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title46-vol4/pdf/CFR-2013-title46-vol4-sec120-430.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title46-vol4/pdf/CFR-2013-title46-vol4-sec120-430.pdf"><span>46 CFR 120.430 - <span class="hlt">Portable</span> lights.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... 46 Shipping 4 2013-10-01 2013-10-01 false <span class="hlt">Portable</span> lights. 120.430 Section 120.430 Shipping COAST... Systems § 120.430 <span class="hlt">Portable</span> lights. Each vessel must be equipped with at least two operable <span class="hlt">portable</span> battery lights. One of these lights must be located at the operating station and the other at the access...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title46-vol4/pdf/CFR-2012-title46-vol4-sec120-430.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title46-vol4/pdf/CFR-2012-title46-vol4-sec120-430.pdf"><span>46 CFR 120.430 - <span class="hlt">Portable</span> lights.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... 46 Shipping 4 2012-10-01 2012-10-01 false <span class="hlt">Portable</span> lights. 120.430 Section 120.430 Shipping COAST... Systems § 120.430 <span class="hlt">Portable</span> lights. Each vessel must be equipped with at least two operable <span class="hlt">portable</span> battery lights. One of these lights must be located at the operating station and the other at the access...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title46-vol4/pdf/CFR-2014-title46-vol4-sec120-430.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title46-vol4/pdf/CFR-2014-title46-vol4-sec120-430.pdf"><span>46 CFR 120.430 - <span class="hlt">Portable</span> lights.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-10-01</p> <p>... 46 Shipping 4 2014-10-01 2014-10-01 false <span class="hlt">Portable</span> lights. 120.430 Section 120.430 Shipping COAST... Systems § 120.430 <span class="hlt">Portable</span> lights. Each vessel must be equipped with at least two operable <span class="hlt">portable</span> battery lights. One of these lights must be located at the operating station and the other at the access...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title46-vol4/pdf/CFR-2011-title46-vol4-sec120-430.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title46-vol4/pdf/CFR-2011-title46-vol4-sec120-430.pdf"><span>46 CFR 120.430 - <span class="hlt">Portable</span> lights.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-10-01</p> <p>... 46 Shipping 4 2011-10-01 2011-10-01 false <span class="hlt">Portable</span> lights. 120.430 Section 120.430 Shipping COAST... Systems § 120.430 <span class="hlt">Portable</span> lights. Each vessel must be equipped with at least two operable <span class="hlt">portable</span> battery lights. One of these lights must be located at the operating station and the other at the access...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ApJ...776...94Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ApJ...776...94Y"><span>Small-scale <span class="hlt">Pressure</span>-balanced Structures Driven by Mirror-mode <span class="hlt">Waves</span> in the Solar Wind</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yao, Shuo; He, J.-S.; Tu, C.-Y.; Wang, L.-H.; Marsch, E.</p> <p>2013-10-01</p> <p>Recently, small-scale <span class="hlt">pressure</span>-balanced structures (PBSs) have been studied with regard to their dependence on the direction of the local mean magnetic field B0 . The present work continues these studies by investigating the compressive <span class="hlt">wave</span> mode forming small PBSs, here for B0 quasi-perpendicular to the x-axis of Geocentric Solar Ecliptic coordinates (GSE-x). All the data used were measured by WIND in the quiet solar wind. From the distribution of PBSs on the plane determined by the temporal scale and angle θxB between the GSE-x and B0 , we notice that at θxB = 115° the PBSs appear at temporal scales ranging from 700 s to 60 s. In the corresponding temporal segment, the correlations between the plasma thermal <span class="hlt">pressure</span> P th and the magnetic <span class="hlt">pressure</span> P B, as well as that between the proton density N p and the magnetic field strength B, are investigated. In addition, we use the proton velocity distribution functions to calculate the proton temperatures T and T ∥. Minimum Variance Analysis is applied to find the magnetic field minimum variance vector BN . We also study the time variation of the cross-helicity σc and the compressibility C p and compare these with values from numerical predictions for the mirror mode. In this way, we finally identify a short segment that has T > T ∥, proton β ~= 1, both pairs of P th-P B and N p-B showing anti-correlation, and σc ≈ 0 with C p > 0. Although the examination of σc and C p is not conclusive, it provides helpful additional information for the <span class="hlt">wave</span> mode identification. Additionally, BN is found to be highly oblique to B0 . Thus, this work suggests that a candidate mechanism for forming small-scale PBSs in the quiet solar wind is due to mirror-mode <span class="hlt">waves</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19660000329','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19660000329"><span>Adapter assembly prevents damage to tubing during high <span class="hlt">pressure</span> tests</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Stinett, L. L.</p> <p>1965-01-01</p> <p><span class="hlt">Portable</span> adapter assembly prevents damage to tubing and injury to personnel when <span class="hlt">pressurizing</span> a system or during high <span class="hlt">pressure</span> tests. The assembly is capable of withstanding high <span class="hlt">pressure</span>. It is securely attached to the tubing stub end and may be removed without brazing, cutting or cleaning the tube.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19024446','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19024446"><span>[Research on a non-invasive pulse <span class="hlt">wave</span> detection and analysis system].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Ting; Yu, Gang</p> <p>2008-10-01</p> <p>A novel non-invasive pulse <span class="hlt">wave</span> detection and analysis system has been developed, including the software and the hardware. Bi-channel signals can be acquired, stored and shown on the screen dynamically at the same time. Pulse <span class="hlt">wave</span> can be reshown and printed after pulse <span class="hlt">wave</span> analysis and pulse <span class="hlt">wave</span> velocity analysis. This system embraces a computer which is designed for fast data saving, analyzing and processing, and a <span class="hlt">portable</span> data sampling machine which is based on a singlechip. Experimental results have shown that the system is stable and easy to use, and the parameters are calculated accurately.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AIPC.1434.1226J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AIPC.1434.1226J"><span>Evaluation of mechanical losses in a linear motor <span class="hlt">pressure</span> <span class="hlt">wave</span> generator</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jacob, Subhash; Rangasamy, Karunanithi; Jonnalagadda, Kranthi Kumar; Chakkala, Damu; Achanur, Mallappa; Govindswamy, Jagadish; Gour, Abhay Singh</p> <p>2012-06-01</p> <p>A moving magnet linear motor compressor or <span class="hlt">pressure</span> <span class="hlt">wave</span> generator (PWG) of 2 cc swept volume with dual opposed piston configuration has been developed to operate miniature pulse tube coolers. Prelimnary experiments yielded only a no-load cold end temperature of 180 K. Auxiliary tests and the interpretation of detailed modeling of a PWG suggest that much of the PV power has been lost in the form of blow-by at piston seals due to large and non-optimum clearance seal gap between piston and cylinder. The results of experimental parameters simulated using Sage provide the optimum seal gap value for maximizing the delivered PV power.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25316410','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25316410"><span>Enhanced acoustic sensing through <span class="hlt">wave</span> compression and <span class="hlt">pressure</span> amplification in anisotropic metamaterials.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Yongyao; Liu, Haijun; Reilly, Michael; Bae, Hyungdae; Yu, Miao</p> <p>2014-10-15</p> <p>Acoustic sensors play an important role in many areas, such as homeland security, navigation, communication, health care and industry. However, the fundamental <span class="hlt">pressure</span> 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 <span class="hlt">wave</span> compression effect that renders direct amplification of <span class="hlt">pressure</span> 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.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=World+AND+Wide+AND+Science&pg=3&id=EJ1172554','ERIC'); return false;" href="https://eric.ed.gov/?q=World+AND+Wide+AND+Science&pg=3&id=EJ1172554"><span>School <span class="hlt">Maker</span> Faires</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>Harlow, Danielle; Hansen, Alexandria</p> <p>2018-01-01</p> <p>The <span class="hlt">Maker</span> Movement (Dougherty 2012) highlights innovation and creativity through "activities focused on designing, building, modifying, and/or repurposing material objects, for playful or useful ends, oriented toward making a 'product' of some sort that can be used, interacted with, or demonstrated" (Martin 2015, p. 31). When engaged in…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhPro..25.1027M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhPro..25.1027M"><span>A Trusted <span class="hlt">Portable</span> Computing Device</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ming-wei, Fang; Jun-jun, Wu; Peng-fei, Yu; Xin-fang, Zhang</p> <p></p> <p>A trusted <span class="hlt">portable</span> computing device and its security mechanism were presented to solve the security issues, such as the attack of virus and Trojan horse, the lost and stolen of storage device, in mobile office. It used smart card to build a trusted <span class="hlt">portable</span> security base, virtualization to create a secure virtual execution environment, two-factor authentication mechanism to identify legitimate users, and dynamic encryption to protect data privacy. The security environment described in this paper is characteristic of <span class="hlt">portability</span>, security and reliability. It can meet the security requirement of mobile office.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/971538','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/971538"><span><span class="hlt">Portable</span> modular detection system</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Brennan, James S [Rodeo, CA; Singh, Anup [Danville, CA; Throckmorton, Daniel J [Tracy, CA; Stamps, James F [Livermore, CA</p> <p>2009-10-13</p> <p>Disclosed herein are <span class="hlt">portable</span> and modular detection devices and systems for detecting electromagnetic radiation, such as fluorescence, from an analyte which comprises at least one optical element removably attached to at least one alignment rail. Also disclosed are modular detection devices and systems having an integrated lock-in amplifier and spatial filter and assay methods using the <span class="hlt">portable</span> and modular detection devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/874525','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/874525"><span><span class="hlt">Portable</span> biochip scanner device</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Perov, Alexander; Sharonov, Alexei; Mirzabekov, Andrei D.</p> <p>2002-01-01</p> <p>A <span class="hlt">portable</span> biochip scanner device used to detect and acquire fluorescence signal data from biological microchips (biochips) is provided. The <span class="hlt">portable</span> biochip scanner device employs a laser for emitting an excitation beam. An optical fiber delivers the laser beam to a <span class="hlt">portable</span> biochip scanner. A lens collimates the laser beam, the collimated laser beam is deflected by a dichroic mirror and focused by an objective lens onto a biochip. The fluorescence light from the biochip is collected and collimated by the objective lens. The fluorescence light is delivered to a photomultiplier tube (PMT) via an emission filter and a focusing lens. The focusing lens focuses the fluorescence light into a pinhole. A signal output of the PMT is processed and displayed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title49-vol3/pdf/CFR-2013-title49-vol3-sec180-603.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title49-vol3/pdf/CFR-2013-title49-vol3-sec180-603.pdf"><span>49 CFR 180.603 - Qualification of <span class="hlt">portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... 49 Transportation 3 2013-10-01 2013-10-01 false Qualification of <span class="hlt">portable</span> tanks. 180.603 Section... MAINTENANCE OF PACKAGINGS Qualification and Maintenance of <span class="hlt">Portable</span> Tanks § 180.603 Qualification of <span class="hlt">portable</span> tanks. (a) Each <span class="hlt">portable</span> tank used for the transportation of hazardous materials must be an authorized...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/8040951','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/8040951"><span>Toe <span class="hlt">pressure</span> determination by audiophotoplethysmography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fronek, A; Blazek, V; Curran, B</p> <p>1994-08-01</p> <p>The purpose of this study was to evaluate the performance of audiophotoplethysmography as a modality to measure toe <span class="hlt">pressure</span> without the requirement of a recorder. A <span class="hlt">portable</span> photoplethysmograph with an audio output was used to determine toe <span class="hlt">pressures</span>, and the results were compared with those obtained by a commercial photoplethysmograph with a recorder. Thirty-one measurements in control subjects and 62 measurements in patients with arterial occlusive disease were performed. The average toe <span class="hlt">pressure</span> recorded with oscillography with standard photoplethysmography was 103.5 mm Hg +/- 14.7 SD and 95.9 mm Hg +/- 13.4 SD with audio-photoplethysmography. In the patient group the <span class="hlt">pressure</span> recorded with a commercial photoplethysmograph was 65.3 mm Hg +/- 34.9 SD compared with 61.6 mm Hg +/- 34.8 SD obtained with audio-photoplethysmography. The difference in both groups was insignificant, and the correlation between both methods was very good. A <span class="hlt">portable</span> hand-held photoplethysmograph equipped with an audio output was used to measure toe <span class="hlt">pressure</span> in control subjects and in patients with arterial occlusive disease. The results have been compared with the oscillometric method by a standard commercial photoplethysmograph connected to a recorder. The correlation was very good in the control and patient groups, and the difference between both methods was below the level of statistical significance. The fact that no recorder is needed may help in introducing toe <span class="hlt">pressure</span> measurement into everyday office diagnostic practice.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24030680','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24030680"><span><span class="hlt">Portable</span> nucleic acid thermocyclers.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Almassian, David R; Cockrell, Lisa M; Nelson, William M</p> <p>2013-11-21</p> <p>A nucleic acid thermal cycler is considered to be <span class="hlt">portable</span> if it is under ten pounds, easily carried by one individual, and battery powered. Nucleic acid amplification includes both polymerase chain reaction (e.g. PCR, RT-PCR) and isothermal amplification (e.g. RPA, HDA, LAMP, NASBA, RCA, ICAN, SMART, SDA). There are valuable applications for <span class="hlt">portable</span> nucleic acid thermocyclers in fields that include clinical diagnostics, biothreat detection, and veterinary testing. A system that is <span class="hlt">portable</span> allows for the distributed detection of targets at the point of care and a reduction of the time from sample to answer. The designer of a <span class="hlt">portable</span> nucleic acid thermocycler must carefully consider both thermal control and the detection of amplification. In addition to thermal control and detection, the designer may consider the integration of a sample preparation subsystem with the nucleic acid thermocycler. There are a variety of technologies that can achieve accurate thermal control and the detection of nucleic acid amplification. Important evaluation criteria for each technology include maturity, power requirements, cost, sensitivity, speed, and manufacturability. Ultimately the needs of a particular market will lead to user requirements that drive the decision between available technologies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10077E..0AS','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10077E..0AS"><span>Blood pulse <span class="hlt">wave</span> velocity and <span class="hlt">pressure</span> sensing via fiber based and free space based optical sensors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sirkis, Talia; Beiderman, Yevgeny; Agdarov, Sergey; Beiderman, Yafim; Zalevsky, Zeev</p> <p>2017-02-01</p> <p>Continuous noninvasive measurement of vital bio-signs, such as cardiopulmonary parameters, is an important tool in evaluation of the patient's physiological condition and health monitoring. On the demand of new enabling technologies, some works have been done in continuous monitoring of blood <span class="hlt">pressure</span> and pulse <span class="hlt">wave</span> velocity. In this paper, we introduce two techniques for non-contact sensing of vital bio signs. In the first approach the optical sensor is based on single mode in-fibers Mach-Zehnder interferometer (MZI) to detect heartbeat, respiration and pulse <span class="hlt">wave</span> velocity (PWV). The introduced interferometer is based on a new implanted scheme. It replaces the conventional MZI realized by inserting of discontinuities in the fiber to break the total internal reflection and scatter/collect light. The proposed fiber sensor was successfully incorporated into shirt to produce smart clothing. The measurements obtained from the smart clothing could be obtained in comfortable manner and there is no need to have an initial calibration or a direct contact between the sensor and the skin of the tested individual. In the second concept we show a remote noncontact blood pulse <span class="hlt">wave</span> velocity and <span class="hlt">pressure</span> measurement based on tracking the temporal changes of reflected secondary speckle patterns produced in human skin when illuminated by a laser beams. In both concept experimental validation of the proposed schemes is shown and analyzed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol1/pdf/CFR-2010-title46-vol1-sec2-75-25.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol1/pdf/CFR-2010-title46-vol1-sec2-75-25.pdf"><span>46 CFR 2.75-25 - <span class="hlt">Portable</span> fire extinguishers.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 46 Shipping 1 2010-10-01 2010-10-01 false <span class="hlt">Portable</span> fire extinguishers. 2.75-25 Section 2.75-25... Personnel § 2.75-25 <span class="hlt">Portable</span> fire extinguishers. (a) The <span class="hlt">portable</span> fire extinguishers listed and labeled as..., inclusive. (b) The procedures for manufacturers to follow and the requirements governing <span class="hlt">portable</span> fire...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title47-vol5/pdf/CFR-2010-title47-vol5-sec80-1189.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title47-vol5/pdf/CFR-2010-title47-vol5-sec80-1189.pdf"><span>47 CFR 80.1189 - <span class="hlt">Portable</span> ship earth stations.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 47 Telecommunication 5 2010-10-01 2010-10-01 false <span class="hlt">Portable</span> ship earth stations. 80.1189 Section....1189 <span class="hlt">Portable</span> ship earth stations. (a) <span class="hlt">Portable</span> ship earth stations are authorized to operate on board more than one ship. <span class="hlt">Portable</span> ship earth stations are also authorized to be operated on board fixed...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title47-vol5/pdf/CFR-2011-title47-vol5-sec80-1189.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title47-vol5/pdf/CFR-2011-title47-vol5-sec80-1189.pdf"><span>47 CFR 80.1189 - <span class="hlt">Portable</span> ship earth stations.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-10-01</p> <p>... 47 Telecommunication 5 2011-10-01 2011-10-01 false <span class="hlt">Portable</span> ship earth stations. 80.1189 Section....1189 <span class="hlt">Portable</span> ship earth stations. (a) <span class="hlt">Portable</span> ship earth stations are authorized to operate on board more than one ship. <span class="hlt">Portable</span> ship earth stations are also authorized to be operated on board fixed...</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_17 --> <div id="page_18" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="341"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title47-vol5/pdf/CFR-2014-title47-vol5-sec80-1189.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title47-vol5/pdf/CFR-2014-title47-vol5-sec80-1189.pdf"><span>47 CFR 80.1189 - <span class="hlt">Portable</span> ship earth stations.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-10-01</p> <p>... 47 Telecommunication 5 2014-10-01 2014-10-01 false <span class="hlt">Portable</span> ship earth stations. 80.1189 Section....1189 <span class="hlt">Portable</span> ship earth stations. (a) <span class="hlt">Portable</span> ship earth stations are authorized to operate on board more than one ship. <span class="hlt">Portable</span> ship earth stations are also authorized to be operated on board fixed...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title47-vol5/pdf/CFR-2013-title47-vol5-sec80-1189.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title47-vol5/pdf/CFR-2013-title47-vol5-sec80-1189.pdf"><span>47 CFR 80.1189 - <span class="hlt">Portable</span> ship earth stations.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... 47 Telecommunication 5 2013-10-01 2013-10-01 false <span class="hlt">Portable</span> ship earth stations. 80.1189 Section....1189 <span class="hlt">Portable</span> ship earth stations. (a) <span class="hlt">Portable</span> ship earth stations are authorized to operate on board more than one ship. <span class="hlt">Portable</span> ship earth stations are also authorized to be operated on board fixed...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title47-vol5/pdf/CFR-2012-title47-vol5-sec80-1189.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title47-vol5/pdf/CFR-2012-title47-vol5-sec80-1189.pdf"><span>47 CFR 80.1189 - <span class="hlt">Portable</span> ship earth stations.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... 47 Telecommunication 5 2012-10-01 2012-10-01 false <span class="hlt">Portable</span> ship earth stations. 80.1189 Section....1189 <span class="hlt">Portable</span> ship earth stations. (a) <span class="hlt">Portable</span> ship earth stations are authorized to operate on board more than one ship. <span class="hlt">Portable</span> ship earth stations are also authorized to be operated on board fixed...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title21-vol8/pdf/CFR-2011-title21-vol8-sec868-5655.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title21-vol8/pdf/CFR-2011-title21-vol8-sec868-5655.pdf"><span>21 CFR 868.5655 - <span class="hlt">Portable</span> liquid oxygen unit.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-04-01</p> <p>... 21 Food and Drugs 8 2011-04-01 2011-04-01 false <span class="hlt">Portable</span> liquid oxygen unit. 868.5655 Section 868...) MEDICAL DEVICES ANESTHESIOLOGY DEVICES Therapeutic Devices § 868.5655 <span class="hlt">Portable</span> liquid oxygen unit. (a) Identification. A <span class="hlt">portable</span> liquid oxygen unit is a <span class="hlt">portable</span>, thermally insulated container of liquid oxygen that...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title21-vol8/pdf/CFR-2010-title21-vol8-sec868-5655.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title21-vol8/pdf/CFR-2010-title21-vol8-sec868-5655.pdf"><span>21 CFR 868.5655 - <span class="hlt">Portable</span> liquid oxygen unit.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-04-01</p> <p>... 21 Food and Drugs 8 2010-04-01 2010-04-01 false <span class="hlt">Portable</span> liquid oxygen unit. 868.5655 Section 868...) MEDICAL DEVICES ANESTHESIOLOGY DEVICES Therapeutic Devices § 868.5655 <span class="hlt">Portable</span> liquid oxygen unit. (a) Identification. A <span class="hlt">portable</span> liquid oxygen unit is a <span class="hlt">portable</span>, thermally insulated container of liquid oxygen that...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title21-vol8/pdf/CFR-2013-title21-vol8-sec868-5655.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title21-vol8/pdf/CFR-2013-title21-vol8-sec868-5655.pdf"><span>21 CFR 868.5655 - <span class="hlt">Portable</span> liquid oxygen unit.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-04-01</p> <p>... 21 Food and Drugs 8 2013-04-01 2013-04-01 false <span class="hlt">Portable</span> liquid oxygen unit. 868.5655 Section 868...) MEDICAL DEVICES ANESTHESIOLOGY DEVICES Therapeutic Devices § 868.5655 <span class="hlt">Portable</span> liquid oxygen unit. (a) Identification. A <span class="hlt">portable</span> liquid oxygen unit is a <span class="hlt">portable</span>, thermally insulated container of liquid oxygen that...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title21-vol8/pdf/CFR-2012-title21-vol8-sec868-5655.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title21-vol8/pdf/CFR-2012-title21-vol8-sec868-5655.pdf"><span>21 CFR 868.5655 - <span class="hlt">Portable</span> liquid oxygen unit.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-04-01</p> <p>... 21 Food and Drugs 8 2012-04-01 2012-04-01 false <span class="hlt">Portable</span> liquid oxygen unit. 868.5655 Section 868...) MEDICAL DEVICES ANESTHESIOLOGY DEVICES Therapeutic Devices § 868.5655 <span class="hlt">Portable</span> liquid oxygen unit. (a) Identification. A <span class="hlt">portable</span> liquid oxygen unit is a <span class="hlt">portable</span>, thermally insulated container of liquid oxygen that...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title21-vol8/pdf/CFR-2014-title21-vol8-sec868-5655.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title21-vol8/pdf/CFR-2014-title21-vol8-sec868-5655.pdf"><span>21 CFR 868.5655 - <span class="hlt">Portable</span> liquid oxygen unit.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-04-01</p> <p>... 21 Food and Drugs 8 2014-04-01 2014-04-01 false <span class="hlt">Portable</span> liquid oxygen unit. 868.5655 Section 868...) MEDICAL DEVICES ANESTHESIOLOGY DEVICES Therapeutic Devices § 868.5655 <span class="hlt">Portable</span> liquid oxygen unit. (a) Identification. A <span class="hlt">portable</span> liquid oxygen unit is a <span class="hlt">portable</span>, thermally insulated container of liquid oxygen that...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1875c0020M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1875c0020M"><span>Development of a heavy duty <span class="hlt">portable</span> variable power supply (HPVPS)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Musa, Ahmad Zulfadli Bin; Lung, Chong Man; Abidin, Wan'Amirah Basyarah Binti Zainol</p> <p>2017-08-01</p> <p>This paper covers the innovation of a Heavy Duty <span class="hlt">Portable</span> Variable Power Supply (HPVPS) in Jabatan Kejuruteraan Elektrik (JKE), Politeknik Mukah, Sarawak (PMU). This project consists of variable power supply which can vary the output from 1.2 V to 11.6V, AC pure <span class="hlt">wave</span> inverter to convert DC to AC for the operation of low power home appliances and also used Li-on rechargeable batteries to store the electrical energy and additional feature that can be used to jump-start the batteries of the car. The main objective of this project is to make the user can operate the electronic devices anywhere whenever if no electricity while doing their lab activities. Most of the regulated power supply in JKE lab aged 9-10 years old and need periodical maintenance and need cost and also the unit can be used is not enough to support the whole class during lab activities. As a result, the P&P process will be facing the major problem in order to make the lab activities running smoothly. By development of the <span class="hlt">portable</span> variable power supply, the P&P process is more efficient and very helpful.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4817968','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4817968"><span>Appropriateness for Total Joint Replacement: Perspectives of Decision-<span class="hlt">Makers</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Clavel, Nathalie; De coster, Carolyn; Pomey, Marie-Pascale; Sanmartin, Claudia; Bohm, Éric; Dunbar, Michael J.; Frank, CY; Hawker, Gillian; Noseworthy, Tom</p> <p>2016-01-01</p> <p>Background: Improving access to total joint replacement (TJR) has been a priority. Without robust mechanisms to ensure appropriateness, these procedures may be overused, incurring substantial costs. In that context, decision-<span class="hlt">makers</span> are particularly concerned with the appropriateness of TJR. Objective: While our previous research focused on the appropriateness of TJR from clinical and patient perspectives, this study is aimed at understanding decision-<span class="hlt">makers</span>' perspectives. Methods: Using a semi-structured guide, we interviewed a convenience sample of decision-<span class="hlt">makers</span> in four Canadian provinces (Alberta, Manitoba, Nova Scotia and Quebec) between February and March 2013. For the purposes of this study, a decision-<span class="hlt">maker</span> was defined as a manager, institutional leader or policy <span class="hlt">maker</span>. Results: Fifteen interviews were conducted with decision-<span class="hlt">makers</span> at ministry (n = 3), regional (n = 6) and institutional levels (n = 8). Decision-<span class="hlt">makers</span> see themselves as having a key role in the appropriateness discourse, that of optimizing resource allocation and efficient delivery of services for TJR, to improve population outcomes. Conclusion: The decision-<span class="hlt">makers</span>' view of appropriateness recognizes the importance of the clinical view, but it offers a very different input into the appropriateness discourse, more closely aligned with appropriateness of setting, which refers to cost-effectiveness considerations. PMID:27027795</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1918713Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1918713Z"><span>Cracked rocks with positive and negative Poisson's ratio: real-crack properties extracted from <span class="hlt">pressure</span> dependence of elastic-<span class="hlt">wave</span> velocities</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zaitsev, Vladimir Y.; Radostin, Andrey V.; Dyskin, Arcady V.; Pasternak, Elena</p> <p>2017-04-01</p> <p>We report results of analysis of literature data on P- and S-<span class="hlt">wave</span> velocities of rocks subjected to variable hydrostatic <span class="hlt">pressure</span>. Out of about 90 examined samples, in more than 40% of the samples the reconstructed Poisson's ratios are negative for lowest confining <span class="hlt">pressure</span> with gradual transition to the conventional positive values at higher <span class="hlt">pressure</span>. The portion of rocks exhibiting negative Poisson's ratio appeared to be unexpectedly high. To understand the mechanism of negative Poisson's ratio, <span class="hlt">pressure</span> dependences of P- and S-<span class="hlt">wave</span> velocities were analyzed using the effective medium model in which the reduction in the elastic moduli due to cracks is described in terms of compliances with respect to shear and normal loading that are imparted to the rock by the presence of cracks. This is in contrast to widely used descriptions of effective cracked medium based on a specific crack model (e.g., penny-shape crack) in which the ratio between normal and shear compliances of such a crack is strictly predetermined. The analysis of <span class="hlt">pressure</span>-dependences of the elastic <span class="hlt">wave</span> velocities makes it possible to reveal the ratio between pure normal and shear compliances (called q-ratio below) for real defects and quantify their integral content in the rock. The examination performed demonstrates that a significant portion (over 50%) of cracks exhibit q-ratio several times higher than that assumed for the conventional penny-shape cracks. This leads to faster reduction of the Poisson's ratio with increasing the crack concentration. Samples with negative Poisson's ratio are characterized by elevated q-ratio and simultaneously crack concentration. Our results clearly indicate that the traditional crack model is not adequate for a significant portion of rocks and that the interaction between the opposite crack faces leading to domination of the normal compliance and reduced shear displacement discontinuity can play an important role in the mechanical behavior of rocks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994nasa.reptR....P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994nasa.reptR....P"><span>Method for cancelling expansion <span class="hlt">waves</span> in a <span class="hlt">wave</span> rotor</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Paxson, Daniel E.</p> <p>1994-03-01</p> <p>A <span class="hlt">wave</span> rotor system includes a <span class="hlt">wave</span> rotor coupled to first and second end plates. Special ports are provided, one in each of the first and second end plates, to cancel expansion <span class="hlt">waves</span> generated by the release of working fluid from the <span class="hlt">wave</span> rotor. One of the expansion <span class="hlt">waves</span> is reflected in the <span class="hlt">wave</span> rotor from a reflecting portion, and provided to the special port in the second end plate. Fluid present at the special port in the second end plate has a stagnation <span class="hlt">pressure</span> and mass flow which is substantially the same as that of the cells of the <span class="hlt">wave</span> rotor communicating with such special port. This allows for cancellation of the expansion <span class="hlt">wave</span> generated by the release of working fluid from the <span class="hlt">wave</span> rotor. The special port in the second end plate has a first end corresponding substantially to the head of the expansion <span class="hlt">wave</span>, and a second end corresponding substantially to the tail of the expansion <span class="hlt">wave</span>. Also, the special port is configured to continually change along the circumference of the second end plate to affect expansion <span class="hlt">wave</span> cancellation. An expansion <span class="hlt">wave</span> generated by a second release of working fluid from the <span class="hlt">wave</span> rotor is cancelled in a similar manner to that described above using a special port in the first end plate. Preferably the cycle of operation of the <span class="hlt">wave</span> rotor system is designed so that the stagnation <span class="hlt">pressure</span> and mass flow of the fluid present at the special ports is the same so that the special ports may be connected by a common duct.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015Icar..250..368B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015Icar..250..368B"><span>Winds, <span class="hlt">waves</span> and shorelines from ancient martian seas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Banfield, Don; Donelan, Mark; Cavaleri, Luigi</p> <p>2015-04-01</p> <p>We consider under what environmental conditions water <span class="hlt">waves</span> (and thus eventually shorelines) should be expected to be produced on hypothetical ancient martian seas and lakes. For winds and atmospheric <span class="hlt">pressures</span> that are too small, no <span class="hlt">waves</span> should be expected, and thus no shorelines. If the winds and atmospheric <span class="hlt">pressure</span> are above some threshold, then <span class="hlt">waves</span> can be formed, and shorelines are possible. We establish these criteria separating conditions under which <span class="hlt">waves</span> will or will not form on an ancient martian open body of water. We consider not only atmospheric <span class="hlt">pressure</span> and wind, but also temperature and salinity, but find these latter effects to be secondary. The normal criterion for the onset of water <span class="hlt">waves</span> under terrestrial conditions is extended to recognize the greater atmospheric viscous boundary layer depth for low atmospheric <span class="hlt">pressures</span>. We used terrestrial <span class="hlt">wave</span> models to predict the <span class="hlt">wave</span> environment expected for reasonable ranges of atmospheric <span class="hlt">pressure</span> and wind for end-member cases of ocean salinity. These models were modified only to reflect the different fluids considered at Mars, the different martian surface gravity, and the varying atmospheric <span class="hlt">pressure</span>, wind and fetch. The models were favorably validated against one another, and also against experiments conducted in a <span class="hlt">wave</span> tank in a <span class="hlt">pressure</span> controlled wind tunnel (NASA Ames MARSWIT). We conclude that if <span class="hlt">wave</span>-cut shorelines can be confirmed on Mars, this can constrain the range of possible atmospheric <span class="hlt">pressures</span> and wind speeds that could have existed when the open water was present on Mars.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/956999','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/956999"><span><span class="hlt">Portable</span> apparatus for separating sample and detecting target analytes</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Renzi, Ronald F.; Wally, Karl; Crocker, Robert W.; Stamps, James F.; Griffiths; Stewart K. ,; Fruetel, Julia A.; Horn, Brent A.; Shokair, Isaac R.; Yee, Daniel D.; VanderNoot, Victoria A.; Wiedenman, Boyd J.; West, Jason A. A.; Ferko, Scott M.</p> <p>2008-11-18</p> <p><span class="hlt">Portable</span> devices and methods for determining the presence of a target analyte using a <span class="hlt">portable</span> device are provided. The <span class="hlt">portable</span> device is preferably hand-held. A sample is injected to the <span class="hlt">portable</span> device. A microfluidic separation is performed within the <span class="hlt">portable</span> device and at least one separated component detected by a detection module within the <span class="hlt">portable</span> device, in embodiments of the invention. A target analyte is identified, based on the separated component, and the presence of the target analyte is indicated on an output interface of the <span class="hlt">portable</span> device, in accordance with embodiments of the invention.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.9546Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.9546Z"><span>Unusual properties of high-compliance porosity extracted from measurements of <span class="hlt">pressure</span>-dependent <span class="hlt">wave</span> velocities in rocks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zaitsev, Vladimir Y.; Radostin, Andrey V.; Pasternak, Elena; Dyskin, Arcady</p> <p>2016-04-01</p> <p>Conventionally the interpretation of <span class="hlt">wave</span> velocities and their variations under load is conducted assuming that closable cracks have simple planar shapes, like the popular model of penny-shape cracks. For such cracks, the proportion between complementary variations in different elastic parameters of rocks (such as S- and P-<span class="hlt">wave</span> velocities) is strictly pre-determined, in particular, it is independent of the crack aspect ratio and rather weakly dependent on the Poisson's ratio of the intact rock. Real rocks, however, contain multitude of cracks of different geometry. Faces of such cracks can exhibit complex modes of interaction when closed by external load, which may result in very different ratios between normal- and shear compliances of such defects. In order to describe the reduction of different elastic moduli, we propose a model in which the compliances of crack-like defects are explicitly decoupled and are not predetermined, so that the ratio q between total normal- and shear- compliances imparted to the rock mass (as well as individual values of these compliances) can be estimated from experimental data on reduction of different elastic moduli (e.g., <span class="hlt">pressure</span> dependences of P- and S-<span class="hlt">wave</span> velocities). Physically, the so-extracted ratio q can be interpreted as intrinsic property of individual crack-like defects similar to each other, or as a characteristic of proportion between concentrations of pure normal cracks with very large q and pure shear cracks with q→0. The latter case can correspond, e.g., to saturated cracks in which weakly-compressible liquid prevents crack closing under normal loading. It can be shown that for conventional dry planar cracks, the compliance ratio is q ˜2. The developed model applied to the data on <span class="hlt">wave</span>-velocity variations with external <span class="hlt">pressure</span> indicates that elastic properties of the real crack-like defects in rocks can differ considerably from the usually assumed ones. Comparison with experimental data on variations P- and S-<span class="hlt">wave</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title10-vol3/pdf/CFR-2014-title10-vol3-sec431-132.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title10-vol3/pdf/CFR-2014-title10-vol3-sec431-132.pdf"><span>10 CFR 431.132 - Definitions concerning automatic commercial ice <span class="hlt">makers</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-01-01</p> <p>... 10 Energy 3 2014-01-01 2014-01-01 false Definitions concerning automatic commercial ice <span class="hlt">makers</span>... CERTAIN COMMERCIAL AND INDUSTRIAL EQUIPMENT Automatic Commercial Ice <span class="hlt">Makers</span> § 431.132 Definitions concerning automatic commercial ice <span class="hlt">makers</span>. Automatic commercial ice <span class="hlt">maker</span> means a factory-made assembly (not...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title10-vol3/pdf/CFR-2012-title10-vol3-sec431-132.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title10-vol3/pdf/CFR-2012-title10-vol3-sec431-132.pdf"><span>10 CFR 431.132 - Definitions concerning automatic commercial ice <span class="hlt">makers</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-01-01</p> <p>... 10 Energy 3 2012-01-01 2012-01-01 false Definitions concerning automatic commercial ice <span class="hlt">makers</span>... CERTAIN COMMERCIAL AND INDUSTRIAL EQUIPMENT Automatic Commercial Ice <span class="hlt">Makers</span> § 431.132 Definitions concerning automatic commercial ice <span class="hlt">makers</span>. Automatic commercial ice <span class="hlt">maker</span> means a factory-made assembly (not...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title10-vol3/pdf/CFR-2010-title10-vol3-sec431-132.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title10-vol3/pdf/CFR-2010-title10-vol3-sec431-132.pdf"><span>10 CFR 431.132 - Definitions concerning automatic commercial ice <span class="hlt">makers</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-01-01</p> <p>... 10 Energy 3 2010-01-01 2010-01-01 false Definitions concerning automatic commercial ice <span class="hlt">makers</span>... CERTAIN COMMERCIAL AND INDUSTRIAL EQUIPMENT Automatic Commercial Ice <span class="hlt">Makers</span> § 431.132 Definitions concerning automatic commercial ice <span class="hlt">makers</span>. Automatic commercial ice <span class="hlt">maker</span> means a factory-made assembly (not...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title10-vol3/pdf/CFR-2011-title10-vol3-sec431-132.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title10-vol3/pdf/CFR-2011-title10-vol3-sec431-132.pdf"><span>10 CFR 431.132 - Definitions concerning automatic commercial ice <span class="hlt">makers</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-01-01</p> <p>... 10 Energy 3 2011-01-01 2011-01-01 false Definitions concerning automatic commercial ice <span class="hlt">makers</span>... CERTAIN COMMERCIAL AND INDUSTRIAL EQUIPMENT Automatic Commercial Ice <span class="hlt">Makers</span> § 431.132 Definitions concerning automatic commercial ice <span class="hlt">makers</span>. Automatic commercial ice <span class="hlt">maker</span> means a factory-made assembly (not...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title10-vol3/pdf/CFR-2013-title10-vol3-sec431-132.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title10-vol3/pdf/CFR-2013-title10-vol3-sec431-132.pdf"><span>10 CFR 431.132 - Definitions concerning automatic commercial ice <span class="hlt">makers</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-01-01</p> <p>... 10 Energy 3 2013-01-01 2013-01-01 false Definitions concerning automatic commercial ice <span class="hlt">makers</span>... CERTAIN COMMERCIAL AND INDUSTRIAL EQUIPMENT Automatic Commercial Ice <span class="hlt">Makers</span> § 431.132 Definitions concerning automatic commercial ice <span class="hlt">makers</span>. Automatic commercial ice <span class="hlt">maker</span> means a factory-made assembly (not...</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_18 --> <div id="page_19" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="361"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol3/pdf/CFR-2010-title46-vol3-sec78-47-70.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol3/pdf/CFR-2010-title46-vol3-sec78-47-70.pdf"><span>46 CFR 78.47-70 - <span class="hlt">Portable</span> magazine chests.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 46 Shipping 3 2010-10-01 2010-10-01 false <span class="hlt">Portable</span> magazine chests. 78.47-70 Section 78.47-70... Fire and Emergency Equipment, Etc. § 78.47-70 <span class="hlt">Portable</span> magazine chests. (a) <span class="hlt">Portable</span> magazine chest shall be marked in letters of at least 3 inches high “<span class="hlt">PORTABLE</span> MAGAZINE CHEST—FLAMMABLE—KEEP LIGHTS AND...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol4/pdf/CFR-2010-title46-vol4-sec97-37-47.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol4/pdf/CFR-2010-title46-vol4-sec97-37-47.pdf"><span>46 CFR 97.37-47 - <span class="hlt">Portable</span> magazine chests.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 46 Shipping 4 2010-10-01 2010-10-01 false <span class="hlt">Portable</span> magazine chests. 97.37-47 Section 97.37-47... OPERATIONS Markings for Fire and Emergency Equipment, Etc. § 97.37-47 <span class="hlt">Portable</span> magazine chests. (a) <span class="hlt">Portable</span> magazine chests shall be marked in letters at least 3 inches high: “<span class="hlt">PORTABLE</span> MAGAZINE CHEST—FLAMMABLE—KEEP...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol7/pdf/CFR-2010-title46-vol7-sec196-37-47.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol7/pdf/CFR-2010-title46-vol7-sec196-37-47.pdf"><span>46 CFR 196.37-47 - <span class="hlt">Portable</span> magazine chests.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 46 Shipping 7 2010-10-01 2010-10-01 false <span class="hlt">Portable</span> magazine chests. 196.37-47 Section 196.37-47... Markings for Fire and Emergency Equipment, etc. § 196.37-47 <span class="hlt">Portable</span> magazine chests. (a) <span class="hlt">Portable</span> magazine chests shall be marked in letters at least 3 inches high: <span class="hlt">PORTABLE</span> MAGAZINE CHEST — FLAMMABLE — KEEP...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1174439','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1174439"><span>Human <span class="hlt">portable</span> preconcentrator system</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Linker, Kevin L.; Brusseau, Charles A.; Hannum, David W.; Puissant, James G.; Varley, Nathan R.</p> <p>2003-08-12</p> <p>A preconcentrator system and apparatus suited to human <span class="hlt">portable</span> use wherein sample potentially containing a target chemical substance is drawn into a chamber and through a pervious screen. The screen is adapted to capture target chemicals and then, upon heating, to release those chemicals into the chamber. Chemicals captured and then released in this fashion are then carried to a <span class="hlt">portable</span> chemical detection device such as a <span class="hlt">portable</span> ion mobility spectrometer. In the preferred embodiment, the means for drawing sample into the chamber comprises a reversible fan which, when operated in reverse direction, creates a backpressure that facilitates evolution of captured target chemicals into the chamber when the screen is heated. The screen can be positioned directly in front of the detector prior to heating to improve detection capability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120016989','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120016989"><span>A Field <span class="hlt">Portable</span> Hyperspectral Goniometer for Coastal Characterization</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bachmann, Charles M.; Gray, Deric; Abelev, Andrei; Philpot, William; Fusina, Robert A.; Musser, Joseph A.; Vermillion, Michael; Doctor, Katarina; White, Maurice; Georgiev, Georgi</p> <p>2012-01-01</p> <p>During an airborne multi-sensor remote sensing experiment at the Virginia Coast Reserve (VCR) Long Term Ecological Research (LTER) site in June 2011 (VCR '11), first measurements were taken with the new NRL Goniometer for Outdoor <span class="hlt">Portable</span> Hyperspectral Earth Reflectance (GOPHER). GOPHER measures the angular distribution of hyperspectral reflectance. GOPHER was constructed for NRL by Spectra Vista Corporation (SVC) and the University of Lethbridge through a capital equipment purchase in 2010. The GOPHER spectrometer is an SVC HR -1024, which measures hyperspectral reflectance over the range from 350 -2500 nm, the visible, near infrared, and short-<span class="hlt">wave</span> infrared. During measurements, the spectrometer travels along a zenith quarter -arc track that can rotate in azimuth, allowing for measurement of the bi-directional reflectance distribution function (BRDF) over the whole hemisphere. The zenith arc has a radius of approximately 2m, and the spectrometer scan pattern can be programmed on the fly during calibration and validation efforts. The spectrometer and zenith arc assembly can be raised and lowered along a mast to allow for measurement of uneven terrain or vegetation canopies of moderate height. Hydraulics on the chassis allow for leveling of the instrument in the field. At just over 400 lbs, GOPHER is a field <span class="hlt">portable</span> instrument and can be transformed into a compact trailer assembly for movement over long distances in the field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1016022','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1016022"><span><span class="hlt">Portable</span> convertible blast effects shield</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Pastrnak, John W.; Hollaway, Rocky; Henning, Carl D.; Deteresa, Steve; Grundler, Walter; Hagler,; Lisle B.; Kokko, Edwin; Switzer, Vernon A</p> <p>2010-10-26</p> <p>A rapidly deployable <span class="hlt">portable</span> convertible blast effects shield/ballistic shield includes a set two or more telescoping cylindrical rings operably connected to each other to convert between a telescopically-collapsed configuration for storage and transport, and a telescopically-extended upright configuration forming an expanded inner volume. In a first embodiment, the upright configuration provides blast effects shielding, such as against blast <span class="hlt">pressures</span>, shrapnel, and/or fire balls. And in a second embodiment, the upright configuration provides ballistic shielding, such as against incoming weapons fire, shrapnel, etc. Each ring has a high-strength material construction, such as a composite fiber and matrix material, capable of substantially inhibiting blast effects and impinging projectiles from passing through the shield. And the set of rings are releasably securable to each other in the telescopically-extended upright configuration, such as by click locks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/909409','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/909409"><span><span class="hlt">Portable</span> convertible blast effects shield</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Pastrnak, John W [Livermore, CA; Hollaway, Rocky [Modesto, CA; Henning, Carl D [Livermore, CA; Deteresa, Steve [Livermore, CA; Grundler, Walter [Hayward, CA; Hagler, Lisle B [Berkeley, CA; Kokko, Edwin [Dublin, CA; Switzer, Vernon A [Livermore, CA</p> <p>2007-05-22</p> <p>A rapidly deployable <span class="hlt">portable</span> convertible blast effects shield/ballistic shield includes a set two or more telescoping cylindrical rings operably connected to each other to convert between a telescopically-collapsed configuration for storage and transport, and a telescopically-extended upright configuration forming an expanded inner volume. In a first embodiment, the upright configuration provides blast effects shielding, such as against blast <span class="hlt">pressures</span>, shrapnel, and/or fire balls. And in a second embodiment, the upright configuration provides ballistic shielding, such as against incoming weapons fire, shrapnel, etc. Each ring has a high-strength material construction, such as a composite fiber and matrix material, capable of substantially inhibiting blast effects and impinging projectiles from passing through the shield. And the set of rings are releasably securable to each other in the telescopically-extended upright configuration, such as by click locks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/2005/1211/','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/2005/1211/"><span><span class="hlt">Wave</span> data processing toolbox manual</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Sullivan, Charlene M.; Warner, John C.; Martini, Marinna A.; Lightsom, Frances S.; Voulgaris, George; Work, Paul</p> <p>2006-01-01</p> <p>Researchers routinely deploy oceanographic equipment in estuaries, coastal nearshore environments, and shelf settings. These deployments usually include tripod-mounted instruments to measure a suite of physical parameters such as currents, <span class="hlt">waves</span>, and <span class="hlt">pressure</span>. Instruments such as the RD Instruments Acoustic Doppler Current Profiler (ADCP(tm)), the Sontek Argonaut, and the Nortek Aquadopp(tm) Profiler (AP) can measure these parameters. The data from these instruments must be processed using proprietary software unique to each instrument to convert measurements to real physical values. These processed files are then available for dissemination and scientific evaluation. For example, the proprietary processing program used to process data from the RD Instruments ADCP for <span class="hlt">wave</span> information is called <span class="hlt">Waves</span>Mon. Depending on the length of the deployment, <span class="hlt">Waves</span>Mon will typically produce thousands of processed data files. These files are difficult to archive and further analysis of the data becomes cumbersome. More imperative is that these files alone do not include sufficient information pertinent to that deployment (metadata), which could hinder future scientific interpretation. This open-file report describes a toolbox developed to compile, archive, and disseminate the processed <span class="hlt">wave</span> measurement data from an RD Instruments ADCP, a Sontek Argonaut, or a Nortek AP. This toolbox will be referred to as the <span class="hlt">Wave</span> Data Processing Toolbox. The <span class="hlt">Wave</span> Data Processing Toolbox congregates the processed files output from the proprietary software into two NetCDF files: one file contains the statistics of the burst data and the other file contains the raw burst data (additional details described below). One important advantage of this toolbox is that it converts the data into NetCDF format. Data in NetCDF format is easy to disseminate, is <span class="hlt">portable</span> to any computer platform, and is viewable with public-domain freely-available software. Another important advantage is that a metadata</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110015963','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110015963"><span><span class="hlt">Portable</span> Multigas Monitors for International Space Station</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mudgett, Paul D.; Pilgrim, Jeffrey S.; Ruff, Gary A.</p> <p>2011-01-01</p> <p>The Environmental Health System (EHS) on International Space Station (ISS) includes <span class="hlt">portable</span> instruments to measure various cabin gases that acutely impact crew health. These hand-held devices measure oxygen, carbon dioxide, carbon monoxide, hydrogen chloride and hydrogen cyanide. The oxygen and carbon dioxide units also serve to back up key functions of the Major Constituent Analyzers. Wherever possible, commercial off-the-shelf (COTS) devices are employed by EHS to save development and sustaining costs. COTS hardware designed for general terrestrial applications however has limitations such as no <span class="hlt">pressure</span> compensation, limited life of the active sensor, calibration drift, battery issues, unpredictable vendor support and obsolescence. The EHS fleet (inflight and ground inventory) of instruments is both aging and dwindling in number. With the retirement of the US Space Shuttle, maintenance of on-orbit equipment becomes all the more difficult. A project is underway to search for gas monitoring technology that is highly reliable and stable for years. Tunable Diode Laser Spectroscopy (TDLS) seems to be the front-runner technology, but generally is not yet commercially available in <span class="hlt">portable</span> form. NASA has fostered the development of TDLS through the Small Business Innovative Research (SBIR) program. A number of gases of interest to the aerospace and submarine communities can be addressed by TDLS including the list mentioned above plus hydrogen fluoride, ammonia and water (humidity). There are several different forms of TDLS including photoacoustic and direct absorption spectroscopy using various multipass cell geometries. This paper describes the history of <span class="hlt">portable</span> gas monitoring on NASA spacecraft and provides a status of the development of TDLS based instruments. Planned TDLS flight experiments on ISS could lead both to operational use on ISS and important roles in future Exploration spacecraft and habitats.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900011479','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900011479"><span>Experimental feasibility of investigating acoustic <span class="hlt">waves</span> in Couette flow with entropy and <span class="hlt">pressure</span> gradients</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Parrott, Tony L.; Zorumski, William E.; Rawls, John W., Jr.</p> <p>1990-01-01</p> <p>The feasibility is discussed for an experimental program for studying the behavior of acoustic <span class="hlt">wave</span> propagation in the presence of strong gradients of <span class="hlt">pressure</span>, 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 <span class="hlt">pressure</span> 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 <span class="hlt">pressure</span> 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.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title21-vol8/pdf/CFR-2013-title21-vol8-sec868-6250.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title21-vol8/pdf/CFR-2013-title21-vol8-sec868-6250.pdf"><span>21 CFR 868.6250 - <span class="hlt">Portable</span> air compressor.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-04-01</p> <p>... 21 Food and Drugs 8 2013-04-01 2013-04-01 false <span class="hlt">Portable</span> air compressor. 868.6250 Section 868.6250...) MEDICAL DEVICES ANESTHESIOLOGY DEVICES Miscellaneous § 868.6250 <span class="hlt">Portable</span> air compressor. (a) Identification. A <span class="hlt">portable</span> air compressor is a device intended to provide compressed air for medical purposes, e...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title21-vol8/pdf/CFR-2010-title21-vol8-sec868-6250.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title21-vol8/pdf/CFR-2010-title21-vol8-sec868-6250.pdf"><span>21 CFR 868.6250 - <span class="hlt">Portable</span> air compressor.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-04-01</p> <p>... 21 Food and Drugs 8 2010-04-01 2010-04-01 false <span class="hlt">Portable</span> air compressor. 868.6250 Section 868.6250...) MEDICAL DEVICES ANESTHESIOLOGY DEVICES Miscellaneous § 868.6250 <span class="hlt">Portable</span> air compressor. (a) Identification. A <span class="hlt">portable</span> air compressor is a device intended to provide compressed air for medical purposes, e...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title21-vol8/pdf/CFR-2011-title21-vol8-sec868-6250.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title21-vol8/pdf/CFR-2011-title21-vol8-sec868-6250.pdf"><span>21 CFR 868.6250 - <span class="hlt">Portable</span> air compressor.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-04-01</p> <p>... 21 Food and Drugs 8 2011-04-01 2011-04-01 false <span class="hlt">Portable</span> air compressor. 868.6250 Section 868.6250...) MEDICAL DEVICES ANESTHESIOLOGY DEVICES Miscellaneous § 868.6250 <span class="hlt">Portable</span> air compressor. (a) Identification. A <span class="hlt">portable</span> air compressor is a device intended to provide compressed air for medical purposes, e...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title29-vol7/pdf/CFR-2013-title29-vol7-sec1915-132.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title29-vol7/pdf/CFR-2013-title29-vol7-sec1915-132.pdf"><span>29 CFR 1915.132 - <span class="hlt">Portable</span> electric tools.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-07-01</p> <p>... 29 Labor 7 2013-07-01 2013-07-01 false <span class="hlt">Portable</span> electric tools. 1915.132 Section 1915.132 Labor... § 1915.132 <span class="hlt">Portable</span> electric tools. The provisions of this section shall apply to ship repairing... frames of <span class="hlt">portable</span> electric tools and appliances, except double insulated tools approved by Underwriters...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title29-vol7/pdf/CFR-2012-title29-vol7-sec1915-132.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title29-vol7/pdf/CFR-2012-title29-vol7-sec1915-132.pdf"><span>29 CFR 1915.132 - <span class="hlt">Portable</span> electric tools.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-07-01</p> <p>... 29 Labor 7 2012-07-01 2012-07-01 false <span class="hlt">Portable</span> electric tools. 1915.132 Section 1915.132 Labor... § 1915.132 <span class="hlt">Portable</span> electric tools. The provisions of this section shall apply to ship repairing... frames of <span class="hlt">portable</span> electric tools and appliances, except double insulated tools approved by Underwriters...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title29-vol7/pdf/CFR-2014-title29-vol7-sec1915-132.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title29-vol7/pdf/CFR-2014-title29-vol7-sec1915-132.pdf"><span>29 CFR 1915.132 - <span class="hlt">Portable</span> electric tools.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-07-01</p> <p>... 29 Labor 7 2014-07-01 2014-07-01 false <span class="hlt">Portable</span> electric tools. 1915.132 Section 1915.132 Labor... § 1915.132 <span class="hlt">Portable</span> electric tools. The provisions of this section shall apply to ship repairing... frames of <span class="hlt">portable</span> electric tools and appliances, except double insulated tools approved by Underwriters...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title29-vol7/pdf/CFR-2011-title29-vol7-sec1915-132.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title29-vol7/pdf/CFR-2011-title29-vol7-sec1915-132.pdf"><span>29 CFR 1915.132 - <span class="hlt">Portable</span> electric tools.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-07-01</p> <p>... 29 Labor 7 2011-07-01 2011-07-01 false <span class="hlt">Portable</span> electric tools. 1915.132 Section 1915.132 Labor... § 1915.132 <span class="hlt">Portable</span> electric tools. The provisions of this section shall apply to ship repairing... frames of <span class="hlt">portable</span> electric tools and appliances, except double insulated tools approved by Underwriters...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title29-vol7/pdf/CFR-2010-title29-vol7-sec1915-132.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title29-vol7/pdf/CFR-2010-title29-vol7-sec1915-132.pdf"><span>29 CFR 1915.132 - <span class="hlt">Portable</span> electric tools.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-07-01</p> <p>... 29 Labor 7 2010-07-01 2010-07-01 false <span class="hlt">Portable</span> electric tools. 1915.132 Section 1915.132 Labor... § 1915.132 <span class="hlt">Portable</span> electric tools. The provisions of this section shall apply to ship repairing... frames of <span class="hlt">portable</span> electric tools and appliances, except double insulated tools approved by Underwriters...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title21-vol8/pdf/CFR-2011-title21-vol8-sec868-5440.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title21-vol8/pdf/CFR-2011-title21-vol8-sec868-5440.pdf"><span>21 CFR 868.5440 - <span class="hlt">Portable</span> oxygen generator.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-04-01</p> <p>... 21 Food and Drugs 8 2011-04-01 2011-04-01 false <span class="hlt">Portable</span> oxygen generator. 868.5440 Section 868...) MEDICAL DEVICES ANESTHESIOLOGY DEVICES Therapeutic Devices § 868.5440 <span class="hlt">Portable</span> oxygen generator. (a) Identification. A <span class="hlt">portable</span> oxygen generator is a device that is intended to release oxygen for respiratory...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title21-vol8/pdf/CFR-2013-title21-vol8-sec868-5440.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title21-vol8/pdf/CFR-2013-title21-vol8-sec868-5440.pdf"><span>21 CFR 868.5440 - <span class="hlt">Portable</span> oxygen generator.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-04-01</p> <p>... 21 Food and Drugs 8 2013-04-01 2013-04-01 false <span class="hlt">Portable</span> oxygen generator. 868.5440 Section 868...) MEDICAL DEVICES ANESTHESIOLOGY DEVICES Therapeutic Devices § 868.5440 <span class="hlt">Portable</span> oxygen generator. (a) Identification. A <span class="hlt">portable</span> oxygen generator is a device that is intended to release oxygen for respiratory...</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.gpo.gov/fdsys/pkg/CFR-2012-title21-vol8/pdf/CFR-2012-title21-vol8-sec868-5440.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title21-vol8/pdf/CFR-2012-title21-vol8-sec868-5440.pdf"><span>21 CFR 868.5440 - <span class="hlt">Portable</span> oxygen generator.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-04-01</p> <p>... 21 Food and Drugs 8 2012-04-01 2012-04-01 false <span class="hlt">Portable</span> oxygen generator. 868.5440 Section 868...) MEDICAL DEVICES ANESTHESIOLOGY DEVICES Therapeutic Devices § 868.5440 <span class="hlt">Portable</span> oxygen generator. (a) Identification. A <span class="hlt">portable</span> oxygen generator is a device that is intended to release oxygen for respiratory...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title21-vol8/pdf/CFR-2014-title21-vol8-sec868-5440.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title21-vol8/pdf/CFR-2014-title21-vol8-sec868-5440.pdf"><span>21 CFR 868.5440 - <span class="hlt">Portable</span> oxygen generator.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-04-01</p> <p>... 21 Food and Drugs 8 2014-04-01 2014-04-01 false <span class="hlt">Portable</span> oxygen generator. 868.5440 Section 868...) MEDICAL DEVICES ANESTHESIOLOGY DEVICES Therapeutic Devices § 868.5440 <span class="hlt">Portable</span> oxygen generator. (a) Identification. A <span class="hlt">portable</span> oxygen generator is a device that is intended to release oxygen for respiratory...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title21-vol8/pdf/CFR-2010-title21-vol8-sec868-5440.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title21-vol8/pdf/CFR-2010-title21-vol8-sec868-5440.pdf"><span>21 CFR 868.5440 - <span class="hlt">Portable</span> oxygen generator.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-04-01</p> <p>... 21 Food and Drugs 8 2010-04-01 2010-04-01 false <span class="hlt">Portable</span> oxygen generator. 868.5440 Section 868...) MEDICAL DEVICES ANESTHESIOLOGY DEVICES Therapeutic Devices § 868.5440 <span class="hlt">Portable</span> oxygen generator. (a) Identification. A <span class="hlt">portable</span> oxygen generator is a device that is intended to release oxygen for respiratory...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoJI.211.1494O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoJI.211.1494O"><span>Spectral element modelling of seismic <span class="hlt">wave</span> propagation in visco-elastoplastic media including excess-pore <span class="hlt">pressure</span> development</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Oral, Elif; Gélis, Céline; Bonilla, Luis Fabián; Delavaud, Elise</p> <p>2017-12-01</p> <p>Numerical modelling of seismic <span class="hlt">wave</span> propagation, considering soil nonlinearity, has become a major topic in seismic hazard studies when strong shaking is involved under particular soil conditions. Indeed, when strong ground motion propagates in saturated soils, pore <span class="hlt">pressure</span> is another important parameter to take into account when successive phases of contractive and dilatant soil behaviour are expected. Here, we model 1-D seismic <span class="hlt">wave</span> propagation in linear and nonlinear media using the spectral element numerical method. The study uses a three-component (3C) nonlinear rheology and includes pore-<span class="hlt">pressure</span> excess. The 1-D-3C model is used to study the 1987 Superstition Hills earthquake (ML 6.6), which was recorded at the Wildlife Refuge Liquefaction Array, USA. The data of this event present strong soil nonlinearity involving pore-<span class="hlt">pressure</span> effects. The ground motion is numerically modelled for different assumptions on soil rheology and input motion (1C versus 3C), using the recorded borehole signals as input motion. The computed acceleration-time histories show low-frequency amplification and strong high-frequency damping due to the development of pore <span class="hlt">pressure</span> in one of the soil layers. Furthermore, the soil is found to be more nonlinear and more dilatant under triaxial loading compared to the classical 1C analysis, and significant differences in surface displacements are observed between the 1C and 3C approaches. This study contributes to identify and understand the dominant phenomena occurring in superficial layers, depending on local soil properties and input motions, conditions relevant for site-specific studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title46-vol4/pdf/CFR-2012-title46-vol4-sec98-30-6.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title46-vol4/pdf/CFR-2012-title46-vol4-sec98-30-6.pdf"><span>46 CFR 98.30-6 - Lifting a <span class="hlt">portable</span> tank.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... 46 Shipping 4 2012-10-01 2012-10-01 false Lifting a <span class="hlt">portable</span> tank. 98.30-6 Section 98.30-6... CONSTRUCTION, ARRANGEMENT, AND OTHER PROVISIONS FOR CERTAIN DANGEROUS CARGOES IN BULK <span class="hlt">Portable</span> Tanks § 98.30-6 Lifting a <span class="hlt">portable</span> tank. No person may lift a <span class="hlt">portable</span> tank with another <span class="hlt">portable</span> tank. [CGD 73-172, 39 FR...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21360978','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21360978"><span>[Experimental research on the electromagnetic radiation immunity of a kind of <span class="hlt">portable</span> monitor].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yuan, Jun; Xiao, Dongping; Jian, Xin</p> <p>2010-11-01</p> <p>The paper is focused on a kind of <span class="hlt">portable</span> monitor that is widely used in military hospitals. In order to study the electromagnetic radiation immunity of the monitor, the experiments of electromagnetic radiation caused by radio frequency continuous <span class="hlt">wave</span> in reverberation chamber and by ultra wide band (UWB) electromagnetic pulse have been done. The study results show that UWB electromagnetic pulse interferes observably the operating state of the monitor. It should be paid high attention to take protective measures. The monitor tested has some electromagnetic immunity ability for radio frequency continuous <span class="hlt">wave</span> radiation. The frequent abnormal phenomena are baseline drift and waveform distortion. The electromagnetic sensitivity of the monitor is related to the frequency of interference source. The monitor tested is most sensitive to the frequency of 390 MHz.</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 acoustic <span class="hlt">waves</span> 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 acoustic <span class="hlt">waves</span> 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 acoustic <span class="hlt">waves</span> 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 acoustic <span class="hlt">waves</span> in the regions with large kR0 (k is the <span class="hlt">wave</span> number and R0 is the equilibrium bubble radius). Stability of the oscillating bubbles under acoustic 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('https://www.gpo.gov/fdsys/pkg/CFR-2010-title14-vol3/pdf/CFR-2010-title14-vol3-sec125-204.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title14-vol3/pdf/CFR-2010-title14-vol3-sec125-204.pdf"><span>14 CFR 125.204 - <span class="hlt">Portable</span> electronic devices.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-01-01</p> <p>... 14 Aeronautics and Space 3 2010-01-01 2010-01-01 false <span class="hlt">Portable</span> electronic devices. 125.204... Equipment Requirements § 125.204 <span class="hlt">Portable</span> electronic devices. (a) Except as provided in paragraph (b) of... operation of, any <span class="hlt">portable</span> electronic device on any U.S.-registered civil aircraft operating under this part...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title14-vol3/pdf/CFR-2011-title14-vol3-sec125-204.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title14-vol3/pdf/CFR-2011-title14-vol3-sec125-204.pdf"><span>14 CFR 125.204 - <span class="hlt">Portable</span> electronic devices.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-01-01</p> <p>... 14 Aeronautics and Space 3 2011-01-01 2011-01-01 false <span class="hlt">Portable</span> electronic devices. 125.204... Equipment Requirements § 125.204 <span class="hlt">Portable</span> electronic devices. (a) Except as provided in paragraph (b) of... operation of, any <span class="hlt">portable</span> electronic device on any U.S.-registered civil aircraft operating under this part...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title14-vol3/pdf/CFR-2013-title14-vol3-sec125-204.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title14-vol3/pdf/CFR-2013-title14-vol3-sec125-204.pdf"><span>14 CFR 125.204 - <span class="hlt">Portable</span> electronic devices.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-01-01</p> <p>... 14 Aeronautics and Space 3 2013-01-01 2013-01-01 false <span class="hlt">Portable</span> electronic devices. 125.204... Equipment Requirements § 125.204 <span class="hlt">Portable</span> electronic devices. (a) Except as provided in paragraph (b) of... operation of, any <span class="hlt">portable</span> electronic device on any U.S.-registered civil aircraft operating under this part...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title14-vol3/pdf/CFR-2014-title14-vol3-sec125-204.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title14-vol3/pdf/CFR-2014-title14-vol3-sec125-204.pdf"><span>14 CFR 125.204 - <span class="hlt">Portable</span> electronic devices.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-01-01</p> <p>... 14 Aeronautics and Space 3 2014-01-01 2014-01-01 false <span class="hlt">Portable</span> electronic devices. 125.204... Equipment Requirements § 125.204 <span class="hlt">Portable</span> electronic devices. (a) Except as provided in paragraph (b) of... operation of, any <span class="hlt">portable</span> electronic device on any U.S.-registered civil aircraft operating under this part...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title14-vol3/pdf/CFR-2012-title14-vol3-sec125-204.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title14-vol3/pdf/CFR-2012-title14-vol3-sec125-204.pdf"><span>14 CFR 125.204 - <span class="hlt">Portable</span> electronic devices.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-01-01</p> <p>... 14 Aeronautics and Space 3 2012-01-01 2012-01-01 false <span class="hlt">Portable</span> electronic devices. 125.204... Equipment Requirements § 125.204 <span class="hlt">Portable</span> electronic devices. (a) Except as provided in paragraph (b) of... operation of, any <span class="hlt">portable</span> electronic device on any U.S.-registered civil aircraft operating under this part...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title30-vol1/pdf/CFR-2010-title30-vol1-sec47-44.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title30-vol1/pdf/CFR-2010-title30-vol1-sec47-44.pdf"><span>30 CFR 47.44 - Temporary, <span class="hlt">portable</span> containers.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-07-01</p> <p>... 30 Mineral Resources 1 2010-07-01 2010-07-01 false Temporary, <span class="hlt">portable</span> containers. 47.44 Section... TRAINING HAZARD COMMUNICATION (HazCom) Container Labels and Other Forms of Warning § 47.44 Temporary, <span class="hlt">portable</span> containers. (a) The operator does not have to label a temporary, <span class="hlt">portable</span> container if he or she...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title48-vol6/pdf/CFR-2010-title48-vol6-sec1852-237-71.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title48-vol6/pdf/CFR-2010-title48-vol6-sec1852-237-71.pdf"><span>48 CFR 1852.237-71 - Pension <span class="hlt">portability</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 48 Federal Acquisition Regulations System 6 2010-10-01 2010-10-01 true Pension <span class="hlt">portability</span>. 1852... 1852.237-71 Pension <span class="hlt">portability</span>. As prescribed at 1837.110-70(b), insert the following clause: Pension <span class="hlt">Portability</span> (JAN 1997) (a) In order for pension costs attributable to employees assigned to this contract to...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910000103&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=19910000103&hterms=sensors+pressure&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dsensors%2Bpressure"><span>Calculation Of Pneumatic Attenuation In <span class="hlt">Pressure</span> Sensors</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.</p> <p>1991-01-01</p> <p>Errors caused by attenuation of air-<span class="hlt">pressure</span> <span class="hlt">waves</span> in narrow tubes calculated by method based on fundamental equations of flow. Changes in ambient <span class="hlt">pressure</span> transmitted along narrow tube to sensor. Attenuation of high-frequency components of <span class="hlt">pressure</span> <span class="hlt">wave</span> calculated from <span class="hlt">wave</span> equation derived from Navier-Stokes equations of viscous flow in tube. Developed to understand and compensate for frictional attenuation in narrow tubes used to connect aircraft <span class="hlt">pressure</span> sensors with <span class="hlt">pressure</span> taps on affected surfaces.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950038025&hterms=wave&qs=N%3D0%26Ntk%3DTitle%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dthe%2B5%2Bwave','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950038025&hterms=wave&qs=N%3D0%26Ntk%3DTitle%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dthe%2B5%2Bwave"><span>Compressional ULF <span class="hlt">waves</span> in the outer magnetosphere. 2: A case study of Pc 5 type <span class="hlt">wave</span> activity</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zhu, Xiaoming; Kivelson, Margaret G.</p> <p>1994-01-01</p> <p>In previously published work (Zhu and Kivelson, 1991) the spatial distribution of compressional magnetic pulsations of period 2 - 20 min in the outer magnetosphere was described. In this companion paper, we study some specific compressional events within our data set, seeking to determine the structure of the <span class="hlt">waves</span> and identifying the <span class="hlt">wave</span> generation mechanism. We use both the magnetic field and three-dimensional plasma data observed by the International Sun-Earth Explorer (ISEE) 1 and/or 2 spacecraft to characterize eight compressional ultra low frequency (ULF) <span class="hlt">wave</span> events with frequencies below 8 mHz in the outer magnetosphere. High time resolution plasma data for the event of July 24, 1978, made possible a detailed analysis of the <span class="hlt">waves</span>. <span class="hlt">Wave</span> properties specific to the event of July 24, 1978, can be summarized as follows: (1) Partial plasma <span class="hlt">pressures</span> in the different energy ranges responded to the magnetic field <span class="hlt">pressure</span> differently. In the low-energy range they oscillated in phase with the magnetic <span class="hlt">pressure</span>, while oscillations in higher-energy ranges were out-of-phase; (2) Perpendicular wavelengths for the event were determined to be 60,000 and 30,000 km in the radial and azimuthal directions, respectively. <span class="hlt">Wave</span> properties common to all events can be summarized as follows: (1) Compressional Pc 5 <span class="hlt">wave</span> activity is correlated with Beta, the ratio of the plasma <span class="hlt">pressure</span> to the magnetic <span class="hlt">pressure</span>; the absolute magnitude of the plasma <span class="hlt">pressure</span> plays a minor role for the <span class="hlt">wave</span> activity; (2) The magnetic equator is a node of the compressional perturbation of the magnetic field; (3) The criterion for the mirror mode instability is often satisfied near the equator in the outer magnetosphere when the compressional <span class="hlt">waves</span> are present. We believe these <span class="hlt">waves</span> are generated by internal magnetohydrodynamic (MHD) instabilities.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMNH51C1902L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMNH51C1902L"><span>3D Numerical Simulation of the <span class="hlt">Wave</span> and Current Loads on a Truss Foundation of the Offshore Wind Turbine During the Extreme Typhoon Event</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lin, C. W.; Wu, T. R.; Chuang, M. H.; Tsai, Y. L.</p> <p>2015-12-01</p> <p>The wind in Taiwan Strait is strong and stable which offers an opportunity to build offshore wind farms. However, frequently visited typhoons and strong ocean current require more attentions on the <span class="hlt">wave</span> force and local scour around the foundation of the turbine piles. In this paper, we introduce an in-house, multi-phase CFD model, Splash3D, for solving the flow field with breaking <span class="hlt">wave</span>, strong turbulent, and scour phenomena. Splash3D solves Navier-Stokes Equation with Large-Eddy Simulation (LES) for the fluid domain, and uses volume of fluid (VOF) with piecewise linear interface reconstruction (PLIC) method to describe the break free-surface. The <span class="hlt">waves</span> were generated inside the computational domain by internal <span class="hlt">wave</span> <span class="hlt">maker</span> with a mass-source function. This function is designed to adequately simulate the <span class="hlt">wave</span> condition under observed extreme events based on JONSWAP spectrum and dispersion relationship. Dirichlet velocity boundary condition is assigned at the upper stream boundary to induce the ocean current. At the downstream face, the sponge-layer method combined with <span class="hlt">pressure</span> Dirichlet boundary condition is specified for dissipating <span class="hlt">waves</span> and conducting current out of the domain. Numerical <span class="hlt">pressure</span> gauges are uniformly set on the structure surface to obtain the force distribution on the structure. As for the local scour around the foundation, we developed Discontinuous Bi-viscous Model (DBM) for the development of the scour hole. Model validations were presented as well. The force distribution under observed irregular <span class="hlt">wave</span> condition was extracted by the irregular-surface force extraction (ISFE) method, which provides a fast and elegant way to integrate the force acting on the surface of irregular structure. From the Simulation results, we found that the total force is mainly induced by the impinging <span class="hlt">waves</span>, and the force from the ocean current is about 2 order of magnitude smaller than the <span class="hlt">wave</span> force. We also found the dynamic <span class="hlt">pressure</span>, <span class="hlt">wave</span> height, and the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19236433','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19236433"><span>Influence of arterial <span class="hlt">wave</span> reflection on carotid blood <span class="hlt">pressure</span> and intima-media thickness in older endurance trained men and women with pre-hypertension.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Heffernan, Kevin S; Jae, Sae Young; Tomayko, Emily; Ishaque, Muhammad R; Fernhall, Bo; Wilund, Kenneth R</p> <p>2009-05-01</p> <p>Increased carotid intima-media thickness (IMT) with aging is a significant predictor of mortality. Older endurance trained (ET) individuals have lower carotid artery stiffness but similar carotid IMT when compared to sedentary (SED) age-matched peers. The purpose of this study was to examine the contribution of arterial <span class="hlt">wave</span> reflections to carotid hemodynamics and IMT in older ET and SED with pre-hypertension. Subjects consisted of endurance-trained master athletes and age-matched sedentary controls (mean age 67 years). Carotid artery Beta-stiffness index and IMT was assessed with ultrasonography. Carotid <span class="hlt">pressure</span> and augmented <span class="hlt">pressure</span> from <span class="hlt">wave</span> reflections (obtained from pulse contour analysis) was measured with applanation tonometry. Carotid systolic blood <span class="hlt">pressure</span> (SBP) and IMT were not different between groups (P>0.05). Carotid stiffness was significantly lower in ET versus SED (7.3 +/- 0.8 versus 9.9 +/- 0.6, P<0.05). Augmented <span class="hlt">pressure</span> was significantly greater in ET versus SED (17.7 +/- 1.6 versus 13.3 +/- 1.5 mmHg, P<0.05). When adjusting for differences in resting heart rate, there were no group differences in augmented <span class="hlt">pressure</span>. In conclusion, older ET persons with pre-hypertension have reduced carotid artery stiffness, but similar carotid SBP and carotid IMT when compared to SED. The lack of change in carotid SBP and IMT in older ET may be related to the inability of chronic exercise training to reduce bradycardia-related augmented <span class="hlt">pressure</span> from <span class="hlt">wave</span> reflections with aging.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/868610','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/868610"><span>Refrigeration system having standing <span class="hlt">wave</span> compressor</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Lucas, Timothy S.</p> <p>1992-01-01</p> <p>A compression-evaporation refrigeration system, wherein gaseous compression of the refrigerant is provided by a standing <span class="hlt">wave</span> compressor. The standing <span class="hlt">wave</span> compressor is modified so as to provide a separate subcooling system for the refrigerant, so that efficiency losses due to flashing are reduced. Subcooling occurs when heat exchange is provided between the refrigerant and a heat pumping surface, which is exposed to the standing acoustic <span class="hlt">wave</span> within the standing <span class="hlt">wave</span> compressor. A variable capacity and variable discharge <span class="hlt">pressure</span> for the standing <span class="hlt">wave</span> compressor is provided. A control circuit simultaneously varies the capacity and discharge <span class="hlt">pressure</span> in response to changing operating conditions, thereby maintaining the minimum discharge <span class="hlt">pressure</span> needed for condensation to occur at any time. Thus, the power consumption of the standing <span class="hlt">wave</span> compressor is reduced and system efficiency is improved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFMNG43A1203W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFMNG43A1203W"><span>Alfven Simple <span class="hlt">Waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Webb, G. M.; Zank, G. P.; Burrows, R.</p> <p>2009-12-01</p> <p>Multi-dimensional Alfvén simple <span class="hlt">waves</span> in magnetohydrodynamics (MHD) are investigated using Boillat's formalism. For simple <span class="hlt">wave</span> solutions, all physical variables (the gas density, <span class="hlt">pressure</span>, fluid velocity, entropy, and magnetic field induction in the MHD case) depend on a single phase function ǎrphi which is a function of the space and time variables. The simple <span class="hlt">wave</span> ansatz requires that the <span class="hlt">wave</span> normal and the normal speed of the <span class="hlt">wave</span> front depend only on the phase function ǎrphi. This leads to an implicit equation for the phase function, and a generalisation of the concept of a plane <span class="hlt">wave</span>. We obtain examples of Alfvén simple <span class="hlt">waves</span>, based on the right eigenvector solutions for the Alfvén mode. The Alfvén mode solutions have six integrals, namely that the entropy, density, magnetic <span class="hlt">pressure</span> and the group velocity (the sum of the Alfvén and fluid velocity) are constant throughout the <span class="hlt">wave</span>. The eigen-equations require that the rate of change of the magnetic induction B with ǎrphi throughout the <span class="hlt">wave</span> is perpendicular to both the <span class="hlt">wave</span> normal n and B. Methods to construct simple <span class="hlt">wave</span> solutions based on specifying either a solution ansatz for n(ǎrphi) or B(ǎrphi) are developed.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_20 --> <div id="page_21" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="401"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.loc.gov/pictures/collection/hh/item/hi0052.photos.058591p/','SCIGOV-HHH'); return false;" href="https://www.loc.gov/pictures/collection/hh/item/hi0052.photos.058591p/"><span>11. RW Meyer Sugar Mill: 18761889. Locomotive=type, firetube, <span class="hlt">portable</span> boiler, ...</span></a></p> <p><a target="_blank" href="http://www.loc.gov/pictures/collection/hh/">Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey</a></p> <p></p> <p></p> <p>11. RW Meyer Sugar Mill: 1876-1889. Locomotive=type, fire-tube, <span class="hlt">portable</span> boiler, model No. 1, Manufactured by Ames Iron Works, Oswego, New York, 1879. 120 lbs./sq. in. working <span class="hlt">pressure</span>, 66 sq. ft. heating surface in tubes. View: the boiler provided steam for steam engine which in turn powered the centrifugals. View shows front fire box, end of boiler. Below fire-box,used for removing ashes, is a door. Circular openings at the rear of the fire-box are where fire-tubes connected with furnace. Column to right of fire-box carried <span class="hlt">pressure</span> and water level gauges. Fluted chimney-type structure is steam-port, safety valve, and whistle. Weights originally sat on the arm extending from the top of the port and controlled the boiler <span class="hlt">pressure</span>. - R. W. Meyer Sugar Mill, State Route 47, Kualapuu, Maui County, HI</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title29-vol5/pdf/CFR-2013-title29-vol5-sec1910-25.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title29-vol5/pdf/CFR-2013-title29-vol5-sec1910-25.pdf"><span>29 CFR 1910.25 - <span class="hlt">Portable</span> wood ladders.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-07-01</p> <p>... 29 Labor 5 2013-07-01 2013-07-01 false <span class="hlt">Portable</span> wood ladders. 1910.25 Section 1910.25 Labor... OCCUPATIONAL SAFETY AND HEALTH STANDARDS Walking-Working Surfaces § 1910.25 <span class="hlt">Portable</span> wood ladders. (a... for the construction, care, and use of the common types of <span class="hlt">portable</span> wood ladders, in order to insure...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title29-vol5/pdf/CFR-2014-title29-vol5-sec1910-25.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title29-vol5/pdf/CFR-2014-title29-vol5-sec1910-25.pdf"><span>29 CFR 1910.25 - <span class="hlt">Portable</span> wood ladders.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-07-01</p> <p>... 29 Labor 5 2014-07-01 2014-07-01 false <span class="hlt">Portable</span> wood ladders. 1910.25 Section 1910.25 Labor... OCCUPATIONAL SAFETY AND HEALTH STANDARDS Walking-Working Surfaces § 1910.25 <span class="hlt">Portable</span> wood ladders. (a... for the construction, care, and use of the common types of <span class="hlt">portable</span> wood ladders, in order to insure...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title14-vol3/pdf/CFR-2014-title14-vol3-sec135-144.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title14-vol3/pdf/CFR-2014-title14-vol3-sec135-144.pdf"><span>14 CFR 135.144 - <span class="hlt">Portable</span> electronic devices.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-01-01</p> <p>... 14 Aeronautics and Space 3 2014-01-01 2014-01-01 false <span class="hlt">Portable</span> electronic devices. 135.144... Equipment § 135.144 <span class="hlt">Portable</span> electronic devices. (a) Except as provided in paragraph (b) of this section, no... <span class="hlt">portable</span> electronic device on any of the following U.S.-registered civil aircraft operating under this part...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title14-vol3/pdf/CFR-2010-title14-vol3-sec135-144.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title14-vol3/pdf/CFR-2010-title14-vol3-sec135-144.pdf"><span>14 CFR 135.144 - <span class="hlt">Portable</span> electronic devices.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-01-01</p> <p>... 14 Aeronautics and Space 3 2010-01-01 2010-01-01 false <span class="hlt">Portable</span> electronic devices. 135.144... Equipment § 135.144 <span class="hlt">Portable</span> electronic devices. (a) Except as provided in paragraph (b) of this section, no... <span class="hlt">portable</span> electronic device on any of the following U.S.-registered civil aircraft operating under this part...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title14-vol3/pdf/CFR-2011-title14-vol3-sec135-144.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title14-vol3/pdf/CFR-2011-title14-vol3-sec135-144.pdf"><span>14 CFR 135.144 - <span class="hlt">Portable</span> electronic devices.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-01-01</p> <p>... 14 Aeronautics and Space 3 2011-01-01 2011-01-01 false <span class="hlt">Portable</span> electronic devices. 135.144... Equipment § 135.144 <span class="hlt">Portable</span> electronic devices. (a) Except as provided in paragraph (b) of this section, no... <span class="hlt">portable</span> electronic device on any of the following U.S.-registered civil aircraft operating under this part...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title14-vol3/pdf/CFR-2012-title14-vol3-sec135-144.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title14-vol3/pdf/CFR-2012-title14-vol3-sec135-144.pdf"><span>14 CFR 135.144 - <span class="hlt">Portable</span> electronic devices.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-01-01</p> <p>... 14 Aeronautics and Space 3 2012-01-01 2012-01-01 false <span class="hlt">Portable</span> electronic devices. 135.144... Equipment § 135.144 <span class="hlt">Portable</span> electronic devices. (a) Except as provided in paragraph (b) of this section, no... <span class="hlt">portable</span> electronic device on any of the following U.S.-registered civil aircraft operating under this part...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title14-vol3/pdf/CFR-2013-title14-vol3-sec135-144.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title14-vol3/pdf/CFR-2013-title14-vol3-sec135-144.pdf"><span>14 CFR 135.144 - <span class="hlt">Portable</span> electronic devices.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-01-01</p> <p>... 14 Aeronautics and Space 3 2013-01-01 2013-01-01 false <span class="hlt">Portable</span> electronic devices. 135.144... Equipment § 135.144 <span class="hlt">Portable</span> electronic devices. (a) Except as provided in paragraph (b) of this section, no... <span class="hlt">portable</span> electronic device on any of the following U.S.-registered civil aircraft operating under this part...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title33-vol2/pdf/CFR-2012-title33-vol2-sec127-203.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title33-vol2/pdf/CFR-2012-title33-vol2-sec127-203.pdf"><span>33 CFR 127.203 - <span class="hlt">Portable</span> gas detectors.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-07-01</p> <p>... 33 Navigation and Navigable Waters 2 2012-07-01 2012-07-01 false <span class="hlt">Portable</span> gas detectors. 127.203... Waterfront Facilities Handling Liquefied Natural Gas Equipment § 127.203 <span class="hlt">Portable</span> gas detectors. The marine transfer area for LNG must have at least two <span class="hlt">portable</span> gas detectors capable of measuring 0-100% of the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title33-vol2/pdf/CFR-2011-title33-vol2-sec127-203.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title33-vol2/pdf/CFR-2011-title33-vol2-sec127-203.pdf"><span>33 CFR 127.203 - <span class="hlt">Portable</span> gas detectors.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-07-01</p> <p>... 33 Navigation and Navigable Waters 2 2011-07-01 2011-07-01 false <span class="hlt">Portable</span> gas detectors. 127.203... Waterfront Facilities Handling Liquefied Natural Gas Equipment § 127.203 <span class="hlt">Portable</span> gas detectors. The marine transfer area for LNG must have at least two <span class="hlt">portable</span> gas detectors capable of measuring 0-100% of the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title33-vol2/pdf/CFR-2014-title33-vol2-sec127-203.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title33-vol2/pdf/CFR-2014-title33-vol2-sec127-203.pdf"><span>33 CFR 127.203 - <span class="hlt">Portable</span> gas detectors.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-07-01</p> <p>... 33 Navigation and Navigable Waters 2 2014-07-01 2014-07-01 false <span class="hlt">Portable</span> gas detectors. 127.203... Waterfront Facilities Handling Liquefied Natural Gas Equipment § 127.203 <span class="hlt">Portable</span> gas detectors. The marine transfer area for LNG must have at least two <span class="hlt">portable</span> gas detectors capable of measuring 0-100% of the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title33-vol2/pdf/CFR-2013-title33-vol2-sec127-203.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title33-vol2/pdf/CFR-2013-title33-vol2-sec127-203.pdf"><span>33 CFR 127.203 - <span class="hlt">Portable</span> gas detectors.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-07-01</p> <p>... 33 Navigation and Navigable Waters 2 2013-07-01 2013-07-01 false <span class="hlt">Portable</span> gas detectors. 127.203... Waterfront Facilities Handling Liquefied Natural Gas Equipment § 127.203 <span class="hlt">Portable</span> gas detectors. The marine transfer area for LNG must have at least two <span class="hlt">portable</span> gas detectors capable of measuring 0-100% of the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title33-vol2/pdf/CFR-2010-title33-vol2-sec127-203.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title33-vol2/pdf/CFR-2010-title33-vol2-sec127-203.pdf"><span>33 CFR 127.203 - <span class="hlt">Portable</span> gas detectors.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-07-01</p> <p>... 33 Navigation and Navigable Waters 2 2010-07-01 2010-07-01 false <span class="hlt">Portable</span> gas detectors. 127.203... Waterfront Facilities Handling Liquefied Natural Gas Equipment § 127.203 <span class="hlt">Portable</span> gas detectors. The marine transfer area for LNG must have at least two <span class="hlt">portable</span> gas detectors capable of measuring 0-100% of the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JPlPh..78...71W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JPlPh..78...71W"><span>Double Alfvén <span class="hlt">waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Webb, G. M.; Hu, Q.; Dasgupta, B.; Zank, G. P.</p> <p>2012-02-01</p> <p>Double Alfvén <span class="hlt">wave</span> solutions of the magnetohydrodynamic equations in which the physical variables (the gas density ρ, fluid velocity u, gas <span class="hlt">pressure</span> p, and magnetic field induction B) depend only on two independent <span class="hlt">wave</span> phases ϕ1(x,t) and ϕ2(x,t) are obtained. The integrals for the double Alfvén <span class="hlt">wave</span> are the same as for simple <span class="hlt">waves</span>, namely, the gas <span class="hlt">pressure</span>, magnetic <span class="hlt">pressure</span>, and group velocity of the <span class="hlt">wave</span> are constant. Compatibility conditions on the evolution of the magnetic field B due to changes in ϕ1 and ϕ2, as well as constraints due to Gauss's law ∇ · B = 0 are discussed. The magnetic field lines and hodographs of B in which the tip of the magnetic field B moves on the sphere |B| = B = const. are used to delineate the physical characteristics of the <span class="hlt">wave</span>. Hamilton's equations for the simple Alfvén <span class="hlt">wave</span> with <span class="hlt">wave</span> normal n(ϕ), and with magnetic induction B(ϕ) in which ϕ is the <span class="hlt">wave</span> phase, are obtained by using the Frenet-Serret equations for curves x=X(ϕ) in differential geometry. The use of differential geometry of 2D surfaces in a 3D Euclidean space to describe double Alfvén <span class="hlt">waves</span> is briefly discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080031178','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080031178"><span>Unified Application Vapor Screen Flow Visualization and <span class="hlt">Pressure</span> Sensitive Paint Measurement Techniques to Vortex- and Shock <span class="hlt">Wave</span>-Dominated Flow Fields</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Erickson, Gary E.</p> <p>2008-01-01</p> <p>Laser vapor screen (LVS) flow visualization and <span class="hlt">pressure</span> sensitive paint (PSP) techniques were applied in a unified approach to wind tunnel testing of slender wing and missile configurations dominated by vortex flows and shock <span class="hlt">waves</span> at subsonic, transonic, and supersonic speeds. The off-surface cross-flow patterns using the LVS technique were combined with global PSP surface static <span class="hlt">pressure</span> mappings to characterize the leading-edge vortices and shock <span class="hlt">waves</span> that coexist and interact at high angles of attack (alpha). The synthesis of LVS and PSP techniques was also effective in identifying the significant effects of passive surface porosity and the presence of vertical tail surfaces on the flow topologies. An overview is given of LVS and PSP applications in selected experiments on small-scale models of generic slender wing and missile configurations in the NASA Langley Research Center (NASA LaRC) Unitary Plan Wind Tunnel (UPWT) and 8-Foot Transonic <span class="hlt">Pressure</span> Tunnel (8-Foot TPT).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27765845','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27765845"><span>The reservoir-<span class="hlt">wave</span> approach to characterize pulmonary vascular-right ventricular interactions in humans.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ghimire, Anukul; Andersen, Mads J; Burrowes, Lindsay M; Bouwmeester, J Christopher; Grant, Andrew D; Belenkie, Israel; Fine, Nowell M; Borlaug, Barry A; Tyberg, John V</p> <p>2016-12-01</p> <p>Using the reservoir-<span class="hlt">wave</span> approach (RWA) we previously characterized pulmonary vasculature mechanics in a normal canine model. We found reflected backward-traveling <span class="hlt">waves</span> that decrease <span class="hlt">pressure</span> and increase flow in the proximal pulmonary artery (PA). These <span class="hlt">waves</span> decrease right ventricular (RV) afterload and facilitate RV ejection. With pathological alterations to the pulmonary vasculature, these <span class="hlt">waves</span> may change and impact RV performance. Our objective in this study was to characterize PA <span class="hlt">wave</span> reflection and the alterations in RV performance in cardiac patients, using the RWA. PA <span class="hlt">pressure</span>, Doppler-flow velocity, and pulmonary arterial wedge <span class="hlt">pressure</span> were measured in 11 patients with exertional dyspnea. The RWA was employed to analyze PA <span class="hlt">pressure</span> and flow; <span class="hlt">wave</span> intensity analysis characterized PA <span class="hlt">waves</span>. <span class="hlt">Wave</span>-related <span class="hlt">pressure</span> was partitioned into two components: <span class="hlt">pressures</span> due to forward-traveling and to backward-traveling <span class="hlt">waves</span>. RV performance was assessed by examining the work done in raising reservoir <span class="hlt">pressure</span> and that associated with the <span class="hlt">wave</span> components of systolic PA <span class="hlt">pressure</span>. <span class="hlt">Wave</span>-related work, the mostly nonrecoverable energy expended by the RV to eject blood, tended to vary directly with mean PA <span class="hlt">pressure</span>. Where PA <span class="hlt">pressures</span> were lower, there were <span class="hlt">pressure</span>-decreasing/flow-increasing backward <span class="hlt">waves</span> that aided RV ejection. Where PA <span class="hlt">pressures</span> were higher, there were <span class="hlt">pressure</span>-increasing/flow-decreasing backward <span class="hlt">waves</span> that impeded RV ejection. <span class="hlt">Pressure</span>-increasing/flow-decreasing backward <span class="hlt">waves</span> were responsible for systolic notches in the Doppler flow velocity profiles in patients with the highest PA <span class="hlt">pressure</span>. Pulmonary hypertension is characterized by reflected <span class="hlt">waves</span> that impede RV ejection and an increase in <span class="hlt">wave</span>-related work. The RWA may facilitate the development of therapeutic strategies. Copyright © 2016 the American Physiological Society.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title29-vol7/pdf/CFR-2010-title29-vol7-sec1917-119.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title29-vol7/pdf/CFR-2010-title29-vol7-sec1917-119.pdf"><span>29 CFR 1917.119 - <span class="hlt">Portable</span> ladders.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-07-01</p> <p>... Requirements for <span class="hlt">Portable</span> Reinforced Plastic Ladders (d) Standards for job-made <span class="hlt">portable</span> ladders. Job-made... usage. (1) Ladders made by fastening rungs or devices across a single rail are prohibited. (2) Ladders...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvE..97d3101C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvE..97d3101C"><span>Generation of intermittent gravitocapillary <span class="hlt">waves</span> via parametric forcing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Castillo, Gustavo; Falcón, Claudio</p> <p>2018-04-01</p> <p>We report on the generation of an intermittent <span class="hlt">wave</span> field driven by a horizontally moving <span class="hlt">wave</span> <span class="hlt">maker</span> interacting with Faraday <span class="hlt">waves</span>. The spectrum of the local gravitocapillary surface <span class="hlt">wave</span> fluctuations displays a power law in frequency for a wide range of forcing parameters. We compute the probability density function of the local surface height increments, which show that they change strongly across time scales. The structure functions of these increments are shown to display power laws as a function of the time lag, with exponents that are nonlinear functions of the order of the structure function. We argue that the origin of this scale-invariant intermittent spectrum is the Faraday <span class="hlt">wave</span> pattern breakup due to its advection by the propagating gravity <span class="hlt">waves</span>. Finally, some interpretations are proposed to explain the appearance of this intermittent spectrum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800000224&hterms=Tidal+waves&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DTidal%2Bwaves','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800000224&hterms=Tidal+waves&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DTidal%2Bwaves"><span>Oceanic-<span class="hlt">wave</span>-measurement system</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Holmes, J. F.; Miles, R. T.</p> <p>1980-01-01</p> <p>Barometer mounted on bouy senses <span class="hlt">wave</span> heights. As <span class="hlt">wave</span> motion raises and lowers barometer, <span class="hlt">pressure</span> differential is proportional to <span class="hlt">wave</span> height. Monitoring circuit samples barometer output every half cycle of <span class="hlt">wave</span> motion and adds magnitudes of adjacent positive and negative peaks. Resulting output signals, proportional to <span class="hlt">wave</span> height, are transmitted to central monitoring station.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27387562','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27387562"><span><span class="hlt">Maker</span> Cultures and the Prospects for Technological Action.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nascimento, Susana; Pólvora, Alexandre</p> <p>2018-06-01</p> <p>Supported by easier and cheaper access to tools and expanding communities, <span class="hlt">maker</span> cultures are pointing towards the ideas of (almost) everyone designing, creating, producing and distributing renewed, new and improved products, machines, things or artefacts. A careful analysis of the assumptions and challenges of <span class="hlt">maker</span> cultures emphasizes the relevance of what may be called technological action, that is, active and critical interventions regarding the purposes and applications of technologies within ordinary lives, thus countering the deterministic trends of current directions of technology. In such transformative potential, we will explore a set of elements what is and could be technological action through snapshots of <span class="hlt">maker</span> cultures based on the empirical research conducted in three particular contexts: the Fab Lab Network, <span class="hlt">Maker</span> Media core outputs and initiatives such as <span class="hlt">Maker</span> Faires, and the Open Source Hardware Association (OSHWA). Elements such as control and empowerment through material engagement, openness and sharing, and social, cultural, political and ethical values of the common good in topics such as diversity, sustainability and transparency, are critically analysed.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_21 --> <div id="page_22" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="421"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA433111','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA433111"><span><span class="hlt">Portable</span> Chemical Sterilizer (PCS) for Surgical Instruments</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2004-12-01</p> <p><span class="hlt">PORTABLE</span> CHEMICAL STERILIZER (PCS) FOR SURGICAL INSTRUMENTS CJ Doona*, FE Feeherry, MA Curtin‡, K Kustin‡, S Kandlikar‡ U.S. Army-Soldier...denotes Contractors) Biomedical Technologies ABSTRACT A novel device called the <span class="hlt">Portable</span> Chemical Sterilizer (PCS) has been developed for the...rapid, safe, <span class="hlt">portable</span>, power-free, and convenient sterilization of objects or surfaces contaminated with pathogenic microorganisms that cause</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19670000332','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19670000332"><span>Hand-held instrument should relieve hematoma <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>Raggio, L. J.; Robertson, T. L.</p> <p>1967-01-01</p> <p><span class="hlt">Portable</span> instrument relieves hematomas beneath fingernails and toenails without surgery. This device simplifies the operative procedure with an instant variable heating tip, adjustable depth settings and interchangeable tip sizes for cauterizing small areas and relieving <span class="hlt">pressurized</span> clots.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/345016','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/345016"><span>Acceptance test report for <span class="hlt">portable</span> exhauster POR-007/Skid E</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>Kriskovich, J.R.</p> <p>1998-07-24</p> <p>This document describes Acceptance Testing performed on <span class="hlt">Portable</span> Exhauster POR-007/Skid E. It includes measurements of bearing vibration levels, <span class="hlt">pressure</span> decay testing, programmable logic controller interlocks, high vacuum, flow and <span class="hlt">pressure</span> control functional testing. The purpose of Acceptance testing documented by this report was to demonstrate compliance of the exhausters with the performance criteria established within HNF-0490, Rev. 1 following a repair and upgrade effort at Hanford. In addition, data obtained during this testing is required for the resolution of outstanding Non-conformance Reports (NCR), and finally, to demonstrate the functionality of the associated software for the <span class="hlt">pressure</span> control and high vacuummore » exhauster operating modes provided for by W-320. Additional testing not required by the ATP was also performed to assist in the disposition and close out of receiving inspection report and for application design information (system curve). Results of this testing are also captured within this document.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25282441','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25282441"><span>Sensitization of a stray-field NMR to vibrations: a potential for MR elastometry with a <span class="hlt">portable</span> NMR sensor.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mastikhin, Igor; Barnhill, Marie</p> <p>2014-11-01</p> <p>An NMR signal from a sample in a constant stray field of a <span class="hlt">portable</span> NMR sensor is sensitized to vibrations. The CPMG sequence is synchronized to vibrations so that the constant gradient becomes an "effective" square-<span class="hlt">wave</span> gradient, leading to the vibration-induced phase accumulation. The integrating nature of the spot measurement, combined with the phase distribution due to a non-uniform gradient and/or a <span class="hlt">wave</span> field, leads to a destructive interference, the drop in the signal intensity and changes in the echo train shape. Vibrations with amplitudes as small as 140 nm were reliably detected with the permanent gradient of 12.4 T/m. The signal intensity depends on the phase offset between the vibrations and the pulse sequence. This approach opens the way for performing elastometry and micro-rheology measurements with <span class="hlt">portable</span> NMR devices beyond the walls of a laboratory. Even without synchronization, if a vibration frequency is comparable to 1/2TE of the CPMG sequence, the signal can be severely affected, making it important for potential industrial applications of stray-field NMR. Copyright © 2014 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title49-vol2/pdf/CFR-2010-title49-vol2-sec172-326.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title49-vol2/pdf/CFR-2010-title49-vol2-sec172-326.pdf"><span>49 CFR 172.326 - <span class="hlt">Portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... petroleum gas (LPG) that is unodorized as authorized in § 173.315(b)(1) unless it is legibly marked NON... the <span class="hlt">portable</span> tank are not visible. (d) NON-ODORIZED marking on <span class="hlt">portable</span> tanks containing LPG. After...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1016497','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1016497"><span><span class="hlt">Portable</span> convertible blast effects shield</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Pastrnak, John W [Livermore, CA; Hollaway, Rocky [Modesto, CA; Henning, Carl D [Livermore, CA; Deteresa, Steve [Livermore, CA; Grundler, Walter [Hayward, CA; Hagler, Lisle B [Berkeley, CA; Kokko, Edwin [Dublin, CA; Switzer, Vernon A [Livermore, CA</p> <p>2011-03-15</p> <p>A rapidly deployable <span class="hlt">portable</span> convertible blast effects shield/ballistic shield includes a set two or more frusto-conically-tapered telescoping rings operably connected to each other to convert between a telescopically-collapsed configuration for storage and transport, and a telescopically-extended upright configuration forming an expanded inner volume. In a first embodiment, the upright configuration provides blast effects shielding, such as against blast <span class="hlt">pressures</span>, shrapnel, and/or fire balls. And in a second embodiment, the upright configuration provides ballistic shielding, such as against incoming weapons fire, shrapnel, etc. Each ring has a high-strength material construction, such as a composite fiber and matrix material, capable of substantially inhibiting blast effects and impinging projectiles from passing through the shield. And the set of rings are releasably securable to each other in the telescopically-extended upright configuration by the friction fit of adjacent pairs of frusto-conically-tapered rings to each other.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ResPh...8..292K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ResPh...8..292K"><span>Solitary traveling <span class="hlt">wave</span> solutions of <span class="hlt">pressure</span> equation of bubbly liquids with examination for viscosity and heat transfer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Khater, Mostafa M. A.; Seadawy, Aly R.; Lu, Dianchen</p> <p>2018-03-01</p> <p>In this research, we investigate one of the most popular model in nature and also industrial which is the <span class="hlt">pressure</span> equation of bubbly liquids with examination for viscosity and heat transfer which has many application in nature and engineering. Understanding the physical meaning of exact and solitary traveling <span class="hlt">wave</span> solutions for this equation gives the researchers in this field a great clear vision of the <span class="hlt">pressure</span> <span class="hlt">waves</span> in a mixture liquid and gas bubbles taking into consideration the viscosity of liquid and the heat transfer and also dynamics of contrast agents in the blood flow at ultrasonic researches. To achieve our goal, we apply three different methods which are extended tanh-function method, extended simple equation method and a new auxiliary equation method on this equation. We obtained exact and solitary traveling <span class="hlt">wave</span> solutions and we also discuss the similarity and difference between these three method and make a comparison between results that we obtained with another results that obtained with the different researchers using different methods. All of these results and discussion explained the fact that our new auxiliary equation method is considered to be the most general, powerful and the most result-oriented. These kinds of solutions and discussion allow for the understanding of the phenomenon and its intrinsic properties as well as the ease of way of application and its applicability to other phenomena.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/6712368','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/6712368"><span>Observations of tornadoes and wall clouds with a <span class="hlt">portable</span> FM-CW Doppler radar: 1989--1990 results</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>Bluestein, H.B.; Unruh, W.P.</p> <p>1990-01-01</p> <p>The purpose of this paper is to report on our progress using a <span class="hlt">portable</span>, 1 W,FM (frequency modulated)-CW (continuous <span class="hlt">wave</span>) Doppler radar developed at the Los Alamos National Laboratory (LANL), to make measurements of the wind field in tornadoes and wall clouds along with simultaneous visual documentation. Results using a CW version of the radar in 1987--1988 are given in Bluestein and Unruh (1989). 18 refs., 2 figs., 1 tab.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27997379','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27997379"><span>The impact of intraocular <span class="hlt">pressure</span> on elastic <span class="hlt">wave</span> velocity estimates in the crystalline lens.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Park, Suhyun; Yoon, Heechul; Larin, Kirill V; Emelianov, Stanislav Y; Aglyamov, Salavat R</p> <p>2016-12-20</p> <p>Intraocular <span class="hlt">pressure</span> (IOP) is believed to influence the mechanical properties of ocular tissues including cornea and sclera. The elastic properties of the crystalline lens have been mainly investigated with regard to presbyopia, the age-related loss of accommodation power of the eye. However, the relationship between the elastic properties of the lens and IOP remains to be established. The objective of this study is to measure the elastic <span class="hlt">wave</span> velocity, which represents the mechanical properties of tissue, in the crystalline lens ex vivo in response to changes in IOP. The elastic <span class="hlt">wave</span> velocities in the cornea and lens from seven enucleated bovine globe samples were estimated using ultrasound shear <span class="hlt">wave</span> elasticity imaging. To generate and then image the elastic <span class="hlt">wave</span> propagation, an ultrasound imaging system was used to transmit a 600 µs pushing pulse at 4.5 MHz center frequency and to acquire ultrasound tracking frames at 6 kHz frame rate. The pushing beams were separately applied to the cornea and lens. IOP in the eyeballs was varied from 5 to 50 mmHg. The results indicate that while the elastic <span class="hlt">wave</span> velocity in the cornea increased from 0.96  ±  0.30 m s -1 to 6.27  ±  0.75 m s -1 as IOP was elevated from 5 to 50 mmHg, there were insignificant changes in the elastic <span class="hlt">wave</span> velocity in the crystalline lens with the minimum and the maximum speeds of 1.44  ±  0.27 m s -1 and 2.03  ±  0.46 m s -1 , respectively. This study shows that ultrasound shear <span class="hlt">wave</span> elasticity imaging can be used to assess the biomechanical properties of the crystalline lens noninvasively. Also, it was observed that the dependency of the crystalline lens stiffness on the IOP was significantly lower in comparison with that of cornea.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/345017','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/345017"><span>Acceptance test report for <span class="hlt">portable</span> exhauster POR-008/Skid F</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>Kriskovich, J.R.</p> <p>1998-07-24</p> <p><span class="hlt">Portable</span> Exhauster POR-008 was procured via HNF-0490, Specification for a <span class="hlt">Portable</span> Exhausted System for Waste Tank Ventilation. Prior to taking ownership, acceptance testing was performed at the vendors. However at the conclusion of testing a number of issues remained that required resolution before the exhausters could be used by Project W-320. The purpose of acceptance testing documented by this report was to demonstrate compliance of the exhausters with the performance criteria established within HNF-O49O, Rev. 1 following a repair and upgrade effort at Hanford. In addition, data obtained during this testing is required for the resolution of outstanding Non-conformance Reportsmore » (NCR), and finally, to demonstrate the functionality of the associated software for the <span class="hlt">pressure</span> control and high vacuum exhauster operating modes provided for by W-320. Additional testing not required by the ATP was also performed to assist in the disposition and close out of receiving inspection report and for application design information (system curve). Results of this testing are also captured within this document.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3907428','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3907428"><span>Fast Acceleration of 2D <span class="hlt">Wave</span> Propagation Simulations Using Modern Computational Accelerators</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Wang, Wei; Xu, Lifan; Cavazos, John; Huang, Howie H.; Kay, Matthew</p> <p>2014-01-01</p> <p>Recent developments in modern computational accelerators like Graphics Processing Units (GPUs) and coprocessors provide great opportunities for making scientific applications run faster than ever before. However, efficient parallelization of scientific code using new programming tools like CUDA requires a high level of expertise that is not available to many scientists. This, plus the fact that parallelized code is usually not <span class="hlt">portable</span> to different architectures, creates major challenges for exploiting the full capabilities of modern computational accelerators. In this work, we sought to overcome these challenges by studying how to achieve both automated parallelization using OpenACC and enhanced <span class="hlt">portability</span> using OpenCL. We applied our parallelization schemes using GPUs as well as Intel Many Integrated Core (MIC) coprocessor to reduce the run time of <span class="hlt">wave</span> propagation simulations. We used a well-established 2D cardiac action potential model as a specific case-study. To the best of our knowledge, we are the first to study auto-parallelization of 2D cardiac <span class="hlt">wave</span> propagation simulations using OpenACC. Our results identify several approaches that provide substantial speedups. The OpenACC-generated GPU code achieved more than speedup above the sequential implementation and required the addition of only a few OpenACC pragmas to the code. An OpenCL implementation provided speedups on GPUs of at least faster than the sequential implementation and faster than a parallelized OpenMP implementation. An implementation of OpenMP on Intel MIC coprocessor provided speedups of with only a few code changes to the sequential implementation. We highlight that OpenACC provides an automatic, efficient, and <span class="hlt">portable</span> approach to achieve parallelization of 2D cardiac <span class="hlt">wave</span> simulations on GPUs. Our approach of using OpenACC, OpenCL, and OpenMP to parallelize this particular model on modern computational accelerators should be applicable to other computational models of <span class="hlt">wave</span> propagation in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28081502','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28081502"><span>Quantitative determinations using <span class="hlt">portable</span> Raman spectroscopy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Navin, Chelliah V; Tondepu, Chaitanya; Toth, Roxana; Lawson, Latevi S; Rodriguez, Jason D</p> <p>2017-03-20</p> <p>A <span class="hlt">portable</span> Raman spectrometer was used to develop chemometric models to determine percent (%) drug release and potency for 500mg ciprofloxacin HCl tablets. Parallel dissolution and chromatographic experiments were conducted alongside Raman experiments to assess and compare the performance and capabilities of <span class="hlt">portable</span> Raman instruments in determining critical drug attributes. All batches tested passed the 30min dissolution specification and the Raman model for drug release was able to essentially reproduce the dissolution profiles obtained by ultraviolet spectroscopy at 276nm for all five batches of the 500mg ciprofloxacin tablets. The five batches of 500mg ciprofloxacin tablets also passed the potency (assay) specification and the % label claim for the entire set of tablets run were nearly identical, 99.4±5.1 for the <span class="hlt">portable</span> Raman method and 99.2±1.2 for the chromatographic method. The results indicate that <span class="hlt">portable</span> Raman spectrometers can be used to perform quantitative analysis of critical product attributes of finished drug products. The findings of this study indicate that <span class="hlt">portable</span> Raman may have applications in the areas of process analytical technology and rapid pharmaceutical surveillance. Published by Elsevier B.V.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title30-vol1/pdf/CFR-2010-title30-vol1-sec18-35.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title30-vol1/pdf/CFR-2010-title30-vol1-sec18-35.pdf"><span>30 CFR 18.35 - <span class="hlt">Portable</span> (trailing) cables and cords.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-07-01</p> <p>... 30 Mineral Resources 1 2010-07-01 2010-07-01 false <span class="hlt">Portable</span> (trailing) cables and cords. 18.35... and Design Requirements § 18.35 <span class="hlt">Portable</span> (trailing) cables and cords. (a) <span class="hlt">Portable</span> cables and cords... a <span class="hlt">portable</span> (trailing) cable shall not exceed 500 feet. Where the method of mining requires the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820012622','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820012622"><span>Precise time dissemination via <span class="hlt">portable</span> atomic clocks</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Putkovich, K.</p> <p>1982-01-01</p> <p>The most precise operational method of time dissemination over long distances presently available to the Precise Time and Time Interval (PTTI) community of users is by means of <span class="hlt">portable</span> atomic clocks. The Global Positioning System (GPS), the latest system showing promise of replacing <span class="hlt">portable</span> clocks for global PTTI dissemination, was evaluated. Although GPS has the technical capability of providing superior world-wide dissemination, the question of present cost and future accessibility may require a continued reliance on <span class="hlt">portable</span> clocks for a number of years. For these reasons a study of <span class="hlt">portable</span> clock operations as they are carried out today was made. The <span class="hlt">portable</span> clock system that was utilized by the U.S. Naval Observatory (NAVOBSY) in the global synchronization of clocks over the past 17 years is described and the concepts on which it is based are explained. Some of its capabilities and limitations are also discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19720006654','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19720006654"><span>Diffraction of a plane <span class="hlt">wave</span> by a three-dimensional corner</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ting, L.; Kung, F.</p> <p>1971-01-01</p> <p>By the superposition of the conical solution for the diffraction of a plane pulse by a three dimensional corner, the solution for a general incident plane <span class="hlt">wave</span> is constructed. A numerical program is presented for the computation of the <span class="hlt">pressure</span> distribution on the surface due to an incident plane <span class="hlt">wave</span> of any <span class="hlt">wave</span> form and at any incident angle. Numerical examples are presented to show the <span class="hlt">pressure</span> signature at several points on the surface due to incident <span class="hlt">wave</span> with a front shock <span class="hlt">wave</span>, two shock <span class="hlt">waves</span> in succession, or a compression <span class="hlt">wave</span> with same peak <span class="hlt">pressure</span>. The examples show that when the distance of a point on the surface from the edges or the vertex is comparable to the distance for the front <span class="hlt">pressure</span> raise to reach the maximum, the peak <span class="hlt">pressure</span> at that point can be much less than that given by a regular reflection, because the diffracted <span class="hlt">wave</span> front arrives at that point prior to the arrival of the peak incident <span class="hlt">wave</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26377510','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26377510"><span>Analysis of Measured and Simulated Supraglottal Acoustic <span class="hlt">Waves</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fraile, Rubén; Evdokimova, Vera V; Evgrafova, Karina V; Godino-Llorente, Juan I; Skrelin, Pavel A</p> <p>2016-09-01</p> <p>To date, although much attention has been paid to the estimation and modeling of the voice source (ie, the glottal airflow volume velocity), the measurement and characterization of the supraglottal <span class="hlt">pressure</span> <span class="hlt">wave</span> have been much less studied. Some previous results have unveiled that the supraglottal <span class="hlt">pressure</span> <span class="hlt">wave</span> has some spectral resonances similar to those of the voice <span class="hlt">pressure</span> <span class="hlt">wave</span>. This makes the supraglottal <span class="hlt">wave</span> partially intelligible. Although the explanation for such effect seems to be clearly related to the reflected <span class="hlt">pressure</span> <span class="hlt">wave</span> traveling upstream along the vocal tract, the influence that nonlinear source-filter interaction has on it is not as clear. This article provides an insight into this issue by comparing the acoustic analyses of measured and simulated supraglottal and voice <span class="hlt">waves</span>. Simulations have been performed using a high-dimensional discrete vocal fold model. Results of such comparative analysis indicate that spectral resonances in the supraglottal <span class="hlt">wave</span> are mainly caused by the regressive <span class="hlt">pressure</span> <span class="hlt">wave</span> that travels upstream along the vocal tract and not by source-tract interaction. On the contrary and according to simulation results, source-tract interaction has a role in the loss of intelligibility that happens in the supraglottal <span class="hlt">wave</span> with respect to the voice <span class="hlt">wave</span>. This loss of intelligibility mainly corresponds to spectral differences for frequencies above 1500 Hz. Copyright © 2016 The Voice Foundation. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title49-vol3/pdf/CFR-2011-title49-vol3-sec178-277.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title49-vol3/pdf/CFR-2011-title49-vol3-sec178-277.pdf"><span>49 CFR 178.277 - Requirements for the design, construction, inspection and testing of <span class="hlt">portable</span> tanks intended for...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-10-01</p> <p>... design <span class="hlt">pressure</span> in the ASME Code, Section VIII (IBR, see § 171.7 of this subchapter). Holding time is the... 49 Transportation 3 2011-10-01 2011-10-01 false Requirements for the design, construction... FOR PACKAGINGS Specifications for <span class="hlt">Portable</span> Tanks § 178.277 Requirements for the design, construction...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title49-vol3/pdf/CFR-2012-title49-vol3-sec178-277.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title49-vol3/pdf/CFR-2012-title49-vol3-sec178-277.pdf"><span>49 CFR 178.277 - Requirements for the design, construction, inspection and testing of <span class="hlt">portable</span> tanks intended for...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... design <span class="hlt">pressure</span> in the ASME Code, Section VIII (IBR, see § 171.7 of this subchapter). Holding time is the... 49 Transportation 3 2012-10-01 2012-10-01 false Requirements for the design, construction... FOR PACKAGINGS Specifications for <span class="hlt">Portable</span> Tanks § 178.277 Requirements for the design, construction...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title49-vol3/pdf/CFR-2014-title49-vol3-sec178-277.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title49-vol3/pdf/CFR-2014-title49-vol3-sec178-277.pdf"><span>49 CFR 178.277 - Requirements for the design, construction, inspection and testing of <span class="hlt">portable</span> tanks intended for...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-10-01</p> <p>... design <span class="hlt">pressure</span> in the ASME Code, Section VIII (IBR, see § 171.7 of this subchapter). Holding time is the... 49 Transportation 3 2014-10-01 2014-10-01 false Requirements for the design, construction... FOR PACKAGINGS Specifications for <span class="hlt">Portable</span> Tanks § 178.277 Requirements for the design, construction...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title49-vol2/pdf/CFR-2010-title49-vol2-sec178-277.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title49-vol2/pdf/CFR-2010-title49-vol2-sec178-277.pdf"><span>49 CFR 178.277 - Requirements for the design, construction, inspection and testing of <span class="hlt">portable</span> tanks intended for...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... design <span class="hlt">pressure</span> in the ASME Code, Section VIII (IBR, see § 171.7 of this subchapter). Holding time is the... 49 Transportation 2 2010-10-01 2010-10-01 false Requirements for the design, construction... FOR PACKAGINGS Specifications for <span class="hlt">Portable</span> Tanks § 178.277 Requirements for the design, construction...</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.gpo.gov/fdsys/pkg/CFR-2013-title49-vol3/pdf/CFR-2013-title49-vol3-sec178-277.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title49-vol3/pdf/CFR-2013-title49-vol3-sec178-277.pdf"><span>49 CFR 178.277 - Requirements for the design, construction, inspection and testing of <span class="hlt">portable</span> tanks intended for...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... design <span class="hlt">pressure</span> in the ASME Code, Section VIII (IBR, see § 171.7 of this subchapter). Holding time is the... 49 Transportation 3 2013-10-01 2013-10-01 false Requirements for the design, construction... FOR PACKAGINGS Specifications for <span class="hlt">Portable</span> Tanks § 178.277 Requirements for the design, construction...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFMOS53D..08M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFMOS53D..08M"><span>Laboratory study of spectral <span class="hlt">waves</span> over a muddy bottom</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Maxeiner, E.; Dalrymple, R. A.</p> <p>2010-12-01</p> <p>The attenuation of water <span class="hlt">waves</span> propagating over a muddy ocean floor has been studied extensively both analytically and experimentally over the past 30 years. Possible mechanisms for this include surface <span class="hlt">wave</span> interactions with the bottom, surface <span class="hlt">wave</span> interactions with <span class="hlt">waves</span> formed at the water/mud interface (lutocline) and shear instability at the water/mud interface. Typically these studies have focused on monochromatic <span class="hlt">waves</span>. Observations of <span class="hlt">wave</span> attenuation in the field, however, are subject to a spectrum of <span class="hlt">wave</span> frequencies and sizes. A few field studies (Sheremet and Stone, 2003; Elgar and Raubenheimer, 2008) have explored the possible effects that a wide spectrum of <span class="hlt">wave</span> frequencies may have on <span class="hlt">wave</span> damping mechanisms. In this study, the <span class="hlt">wave</span> attenuation exhibited by a sea spectrum over a muddy bottom is studied experimentally in a laboratory for the first time. Using an 18 m-long <span class="hlt">wave</span> tank at the Coastal Engineering Laboratory at Johns Hopkins University, a piston-style <span class="hlt">wave</span> <span class="hlt">maker</span> is used to create both monochromatic and spectral <span class="hlt">waves</span>. A 10 m-long section of the tank floor incorporates a recessed layer of kaolinite clay which subsequently mixes with the overlying water in the presence of <span class="hlt">waves</span>. Testing consists of three phases. First, a series of monochromatic <span class="hlt">wave</span> trains are produced over a range of <span class="hlt">wave</span> frequencies and in a range of water depths to assess the damping behavior with respect to a variety of parameters such as <span class="hlt">wave</span> frequency, <span class="hlt">wave</span> height and water depth. Damping is assessed by comparing <span class="hlt">wave</span> height at various longitudinal locations in the tank. Second, “<span class="hlt">wave</span> beats” are created by superimposing <span class="hlt">waves</span> of two frequencies to create a longer envelope. Third, the <span class="hlt">wave</span> <span class="hlt">maker</span> is used to generate a representative random sea condition, based on the Pierson-Moskowitz sea spectrum. For this type of testing, damping is assessed by measuring <span class="hlt">wave</span> energy flux over a period of time at various longitudinal locations in the tank. Spectral analysis is also</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1993nasa.reptQR...P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1993nasa.reptQR...P"><span>System and method for cancelling expansion <span class="hlt">waves</span> in a <span class="hlt">wave</span> rotor</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Paxson, Daniel E.</p> <p>1993-12-01</p> <p>A <span class="hlt">wave</span> rotor system that is comprised of a <span class="hlt">wave</span> rotor coupled to first and second plates is described. Special ports are provided, one in each of the first and second end plates, to cancel expansion <span class="hlt">waves</span> generated by the release of working fluid from the <span class="hlt">wave</span> rotor. One of the expansion <span class="hlt">waves</span> is reflected in the <span class="hlt">wave</span> rotor from a reflecting portion and provided to the special port in the second end plate. Fluid present at the special port in the second end plate has a stagnation <span class="hlt">pressure</span> and mass flow which is the same as that of the cells of the <span class="hlt">wave</span> rotor communicating with such special port. This allows for cancellation of the expansion <span class="hlt">wave</span> generated by the release of working fluid from the <span class="hlt">wave</span> rotor. The special port in the second end plate has a first end corresponding to the head of the expansion <span class="hlt">wave</span> and a second end corresponding to the tail of the expansion <span class="hlt">wave</span>. Also, the special port is configured to continually change along the circumference of the second end plate to affect expansion <span class="hlt">wave</span> cancellation. An expansion <span class="hlt">wave</span> generated by a second release of working fluid from the <span class="hlt">wave</span> rotor is cancelled in a similar manner to that described above using a special port in the first end plate. The cycle of operation of the <span class="hlt">wave</span> rotor system is designed so that the stagnation <span class="hlt">pressure</span> and mass flow of the fluid present at the special ports is the same so that the special ports may be connected by a common duct.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012APS..DFDR24001D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012APS..DFDR24001D"><span>Planar Reflection of Detonations <span class="hlt">Waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Damazo, Jason; Shepherd, Joseph</p> <p>2012-11-01</p> <p>An experimental study examining normally reflected gaseous detonation <span class="hlt">waves</span> is undertaken so that the physics of reflected detonations may be understood. Focused schlieren visualization is used to describe the boundary layer development behind the incident detonation <span class="hlt">wave</span> and the nature of the reflected shock <span class="hlt">wave</span>. Reflected shock <span class="hlt">wave</span> bifurcation-which has received extensive study as it pertains to shock tube performance-is predicted by classical bifurcation theory, but is not observed in the present study for undiluted hydrogen-oxygen and ethylene-oxygen detonation <span class="hlt">waves</span>. <span class="hlt">Pressure</span> and thermocouple gauges are installed in the floor of the detonation tube so as to examine both the wall <span class="hlt">pressure</span> and heat flux. From the <span class="hlt">pressure</span> results, we observe an inconsistency between the measured reflected shock speed and the measured reflected shock strength with one dimensional flow predictions confirming earlier experiments performed in our laboratory. This research is sponsored by the DHS through the University of Rhode Island, Center of Excellence for Explosives Detection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100008839','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100008839"><span>Unified Application of Vapor Screen Flow Visualization and <span class="hlt">Pressure</span> Sensitive Paint Measurement Techniques to Vortex- and Shock <span class="hlt">Wave</span>-Dominated Flow Fields</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Erickson, Gary E.</p> <p>2010-01-01</p> <p>Laser vapor screen (LVS) flow visualization and <span class="hlt">pressure</span> sensitive paint (PSP) techniques were applied in a unified approach to wind tunnel testing of slender wing and missile configurations dominated by vortex flows and shock <span class="hlt">waves</span> at subsonic, transonic, and supersonic speeds. The off-surface cross-flow patterns using the LVS technique were combined with global PSP surface static <span class="hlt">pressure</span> mappings to characterize the leading-edge vortices and shock <span class="hlt">waves</span> that coexist and interact at high angles of attack. The synthesis of LVS and PSP techniques was also effective in identifying the significant effects of passive surface porosity and the presence of vertical tail surfaces on the flow topologies. An overview is given of LVS and PSP applications in selected experiments on small-scale models of generic slender wing and missile configurations in the NASA Langley Research Center (NASA LaRC) Unitary Plan Wind Tunnel (UPWT) and 8-Foot Transonic <span class="hlt">Pressure</span> Tunnel (8-Foot TPT).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28102355','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28102355"><span>Determining arterial <span class="hlt">wave</span> transit time from a single aortic <span class="hlt">pressure</span> pulse in rats: vascular impulse response analysis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chang, Ru-Wen; Chang, Chun-Yi; Lai, Liang-Chuan; Wu, Ming-Shiou; Young, Tai-Horng; Chen, Yih-Sharng; Wang, Chih-Hsien; Chang, Kuo-Chu</p> <p>2017-01-19</p> <p>Arterial <span class="hlt">wave</span> transit time (τ w ) in the lower body circulation is an effective biomarker of cardiovascular risk that substantially affects systolic workload imposed on the heart. This study evaluated a method for determining τ w from the vascular impulse response on the basis of the measured aortic <span class="hlt">pressure</span> and an assumed triangular flow (Q tri ). The base of the unknown Q tri was constructed with a duration set equal to ejection time. The timing of the peak triangle was derived using a fourth-order derivative of the <span class="hlt">pressure</span> waveform. Values of τ w s obtained using Q tri were compared with those obtained from the measure aortic flow <span class="hlt">wave</span> (Q m ). Healthy rats (n = 27), rats with chronic kidney disease (CKD; n = 22), and rats with type 1 (n = 22) or type 2 (n = 11) diabetes were analyzed. The cardiovascular conditions in the CKD rats and both diabetic groups were characterized by a decrease in τ w s. The following significant relation was observed (P < 0.0001): τ w triQ  = -1.5709 + 1.0604 × τ w mQ (r 2  = 0.9641). Our finding indicates that aortic impulse response can be an effective method for the estimation of arterial τ w by using a single <span class="hlt">pressure</span> recording together with the assumed Q tri .</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16110713','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16110713"><span>Cost-effectiveness of <span class="hlt">pressure</span>-relieving devices for the prevention and treatment of <span class="hlt">pressure</span> ulcers.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fleurence, Rachael L</p> <p>2005-01-01</p> <p>The cost-effectiveness of alternating <span class="hlt">pressure</span>-relieving devices, mattress replacements, and mattress overlays compared with a standard hospital (high-specification foam mattress) for the prevention and treatment of <span class="hlt">pressure</span> ulcers in hospital patients in the United Kingdom was investigated. A decision-analytic model was constructed to evaluate different strategies to prevent or treat <span class="hlt">pressure</span> ulcers. Three scenarios were evaluated: the prevention of <span class="hlt">pressure</span> ulcers, the treatment of superficial ulcers, and the treatment of severe ulcers. Epidemiological and effectiveness data were obtained from the clinical literature. Expert opinion using a rating scale technique was used to obtain quality of life data. Costs of the devices were obtained from manufacturers, whereas costs of treatment were obtained from the literature. Uncertainty was explored through probabilistic sensitivity analysis. Using 30,000 pounds sterling/QALY (quality-adjusted life year) as the decision-<span class="hlt">maker</span>'s cut off point (the current UK standard), in scenario 1 (prevention), the cost-effective strategy was the mattress overlay at 1, 4, and 12 weeks. In scenarios 2 and 3, the cost-effective strategy was the mattress replacement at 1, 4, and 12 weeks. Standard care was a dominated intervention in all scenarios for values of the decision-<span class="hlt">maker</span>'s ceiling ratio ranging from 5,000 pounds sterling to 100,000 pounds sterling/QALY. However, the probabilistic sensitivity analysis results reflected the high uncertainty surrounding the choice of devices. Current information suggests that alternating <span class="hlt">pressure</span> mattress overlays may be cost-effective for the prevention of <span class="hlt">pressure</span> ulcers, whereas alternating <span class="hlt">pressure</span> mattress replacements appears to be cost-effective for the treatment of superficial and severe <span class="hlt">pressure</span> ulcers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21084239','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21084239"><span>Heat <span class="hlt">waves</span> in the United States: mortality risk during heat <span class="hlt">waves</span> and effect modification by heat <span class="hlt">wave</span> characteristics in 43 U.S. communities.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Anderson, G Brooke; Bell, Michelle L</p> <p>2011-02-01</p> <p>Devastating health effects from recent heat <span class="hlt">waves</span>, and projected increases in frequency, duration, and severity of heat <span class="hlt">waves</span> from climate change, highlight the importance of understanding health consequences of heat <span class="hlt">waves</span>. We analyzed mortality risk for heat <span class="hlt">waves</span> in 43 U.S. cities (1987-2005) and investigated how effects relate to heat <span class="hlt">waves</span>' intensity, duration, or timing in season. Heat <span class="hlt">waves</span> were defined as ≥ 2 days with temperature ≥ 95th percentile for the community for 1 May through 30 September. Heat <span class="hlt">waves</span> were characterized by their intensity, duration, and timing in season. Within each community, we estimated mortality risk during each heat <span class="hlt">wave</span> compared with non-heat <span class="hlt">wave</span> days, controlling for potential confounders. We combined individual heat <span class="hlt">wave</span> effect estimates using Bayesian hierarchical modeling to generate overall effects at the community, regional, and national levels. We estimated how heat <span class="hlt">wave</span> mortality effects were modified by heat <span class="hlt">wave</span> characteristics (intensity, duration, timing in season). Nationally, mortality increased 3.74% [95% posterior interval (PI), 2.29-5.22%] during heat <span class="hlt">waves</span> compared with non-heat <span class="hlt">wave</span> days. Heat <span class="hlt">wave</span> mortality risk increased 2.49% for every 1°F increase in heat <span class="hlt">wave</span> intensity and 0.38% for every 1-day increase in heat <span class="hlt">wave</span> duration. Mortality increased 5.04% (95% PI, 3.06-7.06%) during the first heat <span class="hlt">wave</span> of the summer versus 2.65% (95% PI, 1.14-4.18%) during later heat <span class="hlt">waves</span>, compared with non-heat <span class="hlt">wave</span> days. Heat <span class="hlt">wave</span> mortality impacts and effect modification by heat <span class="hlt">wave</span> characteristics were more pronounced in the Northeast and Midwest compared with the South. We found higher mortality risk from heat <span class="hlt">waves</span> that were more intense or longer, or those occurring earlier in summer. These findings have implications for decision <span class="hlt">makers</span> and researchers estimating health effects from climate change.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title47-vol4/pdf/CFR-2014-title47-vol4-sec73-1530.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title47-vol4/pdf/CFR-2014-title47-vol4-sec73-1530.pdf"><span>47 CFR 73.1530 - <span class="hlt">Portable</span> test stations [Definition].</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-10-01</p> <p>... 47 Telecommunication 4 2014-10-01 2014-10-01 false <span class="hlt">Portable</span> test stations [Definition]. 73.1530 Section 73.1530 Telecommunication FEDERAL COMMUNICATIONS COMMISSION (CONTINUED) BROADCAST RADIO SERVICES RADIO BROADCAST SERVICES Rules Applicable to All Broadcast Stations § 73.1530 <span class="hlt">Portable</span> test stations [Definition]. A <span class="hlt">portable</span> test station is one...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title47-vol4/pdf/CFR-2012-title47-vol4-sec73-1530.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title47-vol4/pdf/CFR-2012-title47-vol4-sec73-1530.pdf"><span>47 CFR 73.1530 - <span class="hlt">Portable</span> test stations [Definition].</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... 47 Telecommunication 4 2012-10-01 2012-10-01 false <span class="hlt">Portable</span> test stations [Definition]. 73.1530 Section 73.1530 Telecommunication FEDERAL COMMUNICATIONS COMMISSION (CONTINUED) BROADCAST RADIO SERVICES RADIO BROADCAST SERVICES Rules Applicable to All Broadcast Stations § 73.1530 <span class="hlt">Portable</span> test stations [Definition]. A <span class="hlt">portable</span> test station is one...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12309376','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12309376"><span>The message is the message-<span class="hlt">maker</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chalkley, A B</p> <p>1977-03-01</p> <p>For those engaged in family planning or other demographic work of an active kind, serious errors can be made and much money and skill wasted unless there is a clear idea of available means of communication. Literacy and media-diffusion figures offer vague parameters, especially in Asia, and the role of spoken communication -- considered key in "illiterate" societies -- is even more difficult to assess. For mass media, the starting point is "diffusion rates" representing numbers of TV sets owned or newspapers sold per 1000 population and so on -- measures of quantity. This article surveys the population growth rates, urban-rural distribution, educational levels, literacy rates, numbers of newspapers bought, radios and TVs owned (per 1000 population) for 12 Asian countries, and discusses their meaning in terms of media use. Chief among the points made are that print media still have an enormous role to play in the developing countries -- newspaper diffusion rates are quite high, even in countries with low urban population (especially India). The quality of electronic media (too often considered the natural "<span class="hlt">wave</span> of the future" everywhere) varies but is generally not high. Where they are fully developed their role is vital -- but it might be noted that it is the message <span class="hlt">makers</span> themselves who are most vital. Choosing the right medium and the proper message for it is essential.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5087469','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5087469"><span>Design and Implementation of an Electronic Front-End Based on Square <span class="hlt">Wave</span> Excitation for Ultrasonic Torsional Guided <span class="hlt">Wave</span> Viscosity 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>Rabani, Amir</p> <p>2016-01-01</p> <p>The market for process instruments generally requires low cost devices that are robust, small in size, <span class="hlt">portable</span>, and usable in-plant. Ultrasonic torsional guided <span class="hlt">wave</span> sensors have received much attention by researchers for measurement of viscosity and/or density of fluids in recent years. The supporting electronic systems for these sensors providing many different settings of sine-<span class="hlt">wave</span> signals are bulky and expensive. In contrast, a system based on bursts of square <span class="hlt">waves</span> instead of sine <span class="hlt">waves</span> would have a considerable advantage in that respect and could be built using simple integrated circuits at a cost that is orders of magnitude lower than for a windowed sine <span class="hlt">wave</span> device. This paper explores the possibility of using square <span class="hlt">wave</span> bursts as the driving signal source for the ultrasonic torsional guided <span class="hlt">wave</span> viscosity sensor. A simple design of a compact and fully automatic analogue square <span class="hlt">wave</span> front-end for the sensor is also proposed. The successful operation of the system is demonstrated by using the sensor for measuring the viscosity in a representative fluid. This work provides the basis for design and manufacture of low cost compact standalone ultrasonic guided <span class="hlt">wave</span> sensors and enlightens the possibility of using coded excitation techniques utilising square <span class="hlt">wave</span> sequences in such applications. PMID:27754324</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27754324','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27754324"><span>Design and Implementation of an Electronic Front-End Based on Square <span class="hlt">Wave</span> Excitation for Ultrasonic Torsional Guided <span class="hlt">Wave</span> Viscosity Sensor.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rabani, Amir</p> <p>2016-10-12</p> <p>The market for process instruments generally requires low cost devices that are robust, small in size, <span class="hlt">portable</span>, and usable in-plant. Ultrasonic torsional guided <span class="hlt">wave</span> sensors have received much attention by researchers for measurement of viscosity and/or density of fluids in recent years. The supporting electronic systems for these sensors providing many different settings of sine-<span class="hlt">wave</span> signals are bulky and expensive. In contrast, a system based on bursts of square <span class="hlt">waves</span> instead of sine <span class="hlt">waves</span> would have a considerable advantage in that respect and could be built using simple integrated circuits at a cost that is orders of magnitude lower than for a windowed sine <span class="hlt">wave</span> device. This paper explores the possibility of using square <span class="hlt">wave</span> bursts as the driving signal source for the ultrasonic torsional guided <span class="hlt">wave</span> viscosity sensor. A simple design of a compact and fully automatic analogue square <span class="hlt">wave</span> front-end for the sensor is also proposed. The successful operation of the system is demonstrated by using the sensor for measuring the viscosity in a representative fluid. This work provides the basis for design and manufacture of low cost compact standalone ultrasonic guided <span class="hlt">wave</span> sensors and enlightens the possibility of using coded excitation techniques utilising square <span class="hlt">wave</span> sequences in such applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1409586-pressure-induced-electronic-topological-transitions-charge-density-wave-material-se','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1409586-pressure-induced-electronic-topological-transitions-charge-density-wave-material-se"><span><span class="hlt">Pressure</span>-induced electronic topological transitions in the charge-density-<span class="hlt">wave</span> material In 4 Se 3</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Zhang, Yuhang; Song, Liyan; Shao, Xuecheng</p> <p>2017-08-01</p> <p>High-<span class="hlt">pressure</span> in situ angle dispersive X-ray diffraction (ADXRD) measurements were performed on the charge-density-<span class="hlt">wave</span> (CDW) material In4Se3 up to 48.8 GPa. <span class="hlt">Pressure</span>-induced structural changes were observed at 7.0 and 34.2 GPa, respectively. Using the CALYPSO methodology, the first high-<span class="hlt">pressure</span> phase was solved as an exotic Pca21 structure. The compressional behaviors of the initial Pnnm and the Pca21 phases were all determined. Combined with first-principle calculations, we find that, unexpectedly, the Pnnm phase probably experiences twice electronic topological transitions (ETTs), from the initial possible CDW state to a semimetallic state at about 2.3 GPa and then back to a possible CDWmore » state at around 3.5 GPa, which was uncovered for the first time in CDW systems. In the both possible CDW states, <span class="hlt">pressure</span> provokes a decrease of band-gap. The observation of a bulk metallic state was ascribed to structural transition to the Pca21 phase. Besides, based on electronic band structure calculations, the thermoelectric property of the Pnnm phase under compression was discussed. Our results show that <span class="hlt">pressure</span> play a dramatic role in tuning In4Se3's structure and transport properties.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ApPhA.112..129A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ApPhA.112..129A"><span>Effects of <span class="hlt">pressure</span> characteristics on transfection efficiency in laser-induced stress <span class="hlt">wave</span>-mediated gene delivery</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ando, Takahiro; Sato, Shunichi; Ashida, Hiroshi; Obara, Minoru</p> <p>2013-07-01</p> <p>Laser-induced stress <span class="hlt">waves</span> (LISWs) generated by irradiating a light-absorbing medium with a pulsed laser can transiently increase the permeability of cell membranes for gene delivery. In this study, we investigated the effects of <span class="hlt">pressure</span> characteristics of LISWs upon gene transfection efficiency using lasers with different pulse durations: a 6-ns pulsed Nd:YAG laser and 20-ns and 200-µs pulsed ruby lasers. LISWs were generated by irradiating a black rubber disk, on which a transparent plastic sheet was adhered for confinement of the laser-produced plasma. Rat dorsal skin was injected with plasmid DNA coding for luciferase, to which LISWs were applied. With nanosecond laser pulses, transfection efficiency increased linearly with increasing positive peak <span class="hlt">pressure</span> in the range of 35 to 145 MPa, the corresponding impulse ranging from 10 to 40 Paṡs. With 200-µs laser pulses, on the other hand, efficient gene expression was observed by the application of LISWs even with a 10-fold-lower peak <span class="hlt">pressure</span> (˜5 MPa), the corresponding impulse being as large as 430 Paṡs. These results indicate that even at low peak <span class="hlt">pressures</span>, efficient transfection can be achieved by extending the <span class="hlt">pressure</span> duration and hence by increasing the impulse of LISWs, while the averaged expression efficiencies were relatively low.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21371762-portable-txrf-spectrometer-sup-detection-limit-portable-xrf-spectromicroscope-sub-mm-spatial-resolution','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21371762-portable-txrf-spectrometer-sup-detection-limit-portable-xrf-spectromicroscope-sub-mm-spatial-resolution"><span><span class="hlt">Portable</span> TXRF Spectrometer with 10{sup -11}g Detection Limit and <span class="hlt">Portable</span> XRF Spectromicroscope with Sub-mm Spatial Resolution</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>Kunimura, Shinsuke; Hatakeyama, So; Sasaki, Nobuharu</p> <p></p> <p>A <span class="hlt">portable</span> total reflection X-ray fluorescence (TXRF) spectrometer that we have developed is applied to trace elemental analysis of water solutions. Although a 5 W X-ray tube is used in the <span class="hlt">portable</span> TXRF spectrometer, detection limits of several ppb are achieved for 3d transition metal elements and trace elements in a leaching solution of soils, a leaching solution of solder, and alcoholic beverages are detected. <span class="hlt">Portable</span> X-ray fluorescence (XRF) spectromicroscopes with a 1 W X-ray tube and an 8 W X-ray tube are also presented. Using the <span class="hlt">portable</span> XRF spectromicroscope with the 1 W X-ray tube, 93 ppm of Crmore » is detected with an about 700 {mu}m spatial resolution. Spatially resolved elemental analysis of a mug painted with blue, red, green, and white is performed using the two <span class="hlt">portable</span> spectromicroscopes, and the difference in elemental composition at each paint is detected.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060040208&hterms=methanol+fuel+cells&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dmethanol%2Bfuel%2Bcells','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060040208&hterms=methanol+fuel+cells&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dmethanol%2Bfuel%2Bcells"><span><span class="hlt">Portable</span> direct methanol fuel cell systems</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Narayanan, S. R.; Valdez, T. I.</p> <p>2002-01-01</p> <p>This article includes discussion of the specific power and power density requirements for various <span class="hlt">portable</span> system applications, the status of stack technology, progress in the implementation of balance-of-plant designs, and a summary of the characteristics of various DMFC <span class="hlt">portable</span> power source demonstrations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Effects+AND+Piracy&id=EJ421758','ERIC'); return false;" href="https://eric.ed.gov/?q=Effects+AND+Piracy&id=EJ421758"><span>The Economics of Educational Software <span class="hlt">Portability</span>.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Oliveira, Joao Batista Araujo e</p> <p>1990-01-01</p> <p>Discusses economic issues that affect the <span class="hlt">portability</span> of educational software. Topics discussed include economic reasons for <span class="hlt">portability</span>, including cost effectiveness; the nature and behavior of educational computer software markets; the role of producers, buyers, and consumers; potential effects of government policies; computer piracy; and…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title46-vol4/pdf/CFR-2013-title46-vol4-sec98-33-5.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title46-vol4/pdf/CFR-2013-title46-vol4-sec98-33-5.pdf"><span>46 CFR 98.33-5 - <span class="hlt">Portable</span> tanks authorized.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... 46 Shipping 4 2013-10-01 2013-10-01 false <span class="hlt">Portable</span> tanks authorized. 98.33-5 Section 98.33-5... CONSTRUCTION, ARRANGEMENT, AND OTHER PROVISIONS FOR CERTAIN DANGEROUS CARGOES IN BULK <span class="hlt">Portable</span> Tanks for Certain Grade E Combustible Liquids and Other Regulated Materials § 98.33-5 <span class="hlt">Portable</span> tanks authorized. The...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title46-vol4/pdf/CFR-2012-title46-vol4-sec98-33-5.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title46-vol4/pdf/CFR-2012-title46-vol4-sec98-33-5.pdf"><span>46 CFR 98.33-5 - <span class="hlt">Portable</span> tanks authorized.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... 46 Shipping 4 2012-10-01 2012-10-01 false <span class="hlt">Portable</span> tanks authorized. 98.33-5 Section 98.33-5... CONSTRUCTION, ARRANGEMENT, AND OTHER PROVISIONS FOR CERTAIN DANGEROUS CARGOES IN BULK <span class="hlt">Portable</span> Tanks for Certain Grade E Combustible Liquids and Other Regulated Materials § 98.33-5 <span class="hlt">Portable</span> tanks authorized. The...</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/17716844','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17716844"><span>Transmission of infrasonic <span class="hlt">pressure</span> <span class="hlt">waves</span> from cerebrospinal to intralabyrinthine fluids through the human cochlear aqueduct: Non-invasive measurements with otoacoustic emissions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Traboulsi, Raghida; Avan, Paul</p> <p>2007-11-01</p> <p>The cochlear aqueduct connecting intralabyrinthine and cerebrospinal fluids (CSF) acts as a low-pass filter that should be able to transmit infrasonic <span class="hlt">pressure</span> <span class="hlt">waves</span> from CSF to cochlea. Recent experiments have shown that otoacoustic emissions generated at 1kHz respond to <span class="hlt">pressure</span>-related stapes impedance changes with a change in phase relative to the generator tones, and provide a non-invasive means of assessing intracochlear <span class="hlt">pressure</span> changes. In order to characterize the transmission to the cochlea of CSF <span class="hlt">pressure</span> <span class="hlt">waves</span> due to respiration, the distortion-product otoacoustic emissions (DPOAE) of 12 subjects were continuously monitored around 1kHz at a rate of 6.25epochs/s, and their phase relative to the stimulus tones was extracted. The subjects breathed normally, in different postures, while thoracic movements were recorded so as to monitor respiration. A correlate of respiration was found in the time variation of DPOAE phase, with an estimated mean amplitude of 10 degrees , i.e. 60mm water, suggesting little attenuation across the aqueduct. Its phase lag relative to thoracic movements varied between 0 degrees and -270 degrees . When fed into a two-compartment model of CSF and labyrinthine spaces, these results suggest that respiration rate at rest is just above the resonance frequency of the CSF compartment, and just below the corner frequency of the cochlear-aqueduct low-pass filter, in line with previous estimates from temporal bone and intracranial measurements. The fact that infrasonic CSF <span class="hlt">waves</span> can be monitored through the cochlea opens diagnostic possibilities in neurology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009PhyA..388.3164Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009PhyA..388.3164Z"><span>Does the market <span class="hlt">maker</span> stabilize the market?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, Mei; Chiarella, Carl; He, Xue-Zhong; Wang, Duo</p> <p>2009-08-01</p> <p>The market <span class="hlt">maker</span> plays an important role in price formation, but his/her behavior and stabilizing impact on the market are relatively unclear, in particular in speculative markets. This paper develops a financial market model that examines the impact on market stability of the market <span class="hlt">maker</span>, who acts as both a liquidity provider and an active investor in a market consisting of two types of boundedly rational speculative investors-the fundamentalists and trend followers. We show that the market <span class="hlt">maker</span> does not necessarily stabilize the market when he/she actively manages the inventory to maximize profits, and that rather the market maker’s impact depends on the behavior of the speculators. Numerical simulations show that the model is able to generate outcomes for asset returns and market inventories that are consistent with empirical findings.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29538723','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29538723"><span>The utilization of research evidence in Health Workforce Policies: the perspectives of Portuguese and Brazilian National Policy-<span class="hlt">Makers</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Craveiro, Isabel; Hortale, Virginia; Oliveira, Ana Paula Cavalcante de; Dal Poz, Mario; Portela, Gustavo; Dussault, Gilles</p> <p>2018-03-01</p> <p>The production of knowledge on Human Resources for Health (HRH) issues has increased exponentially since 2000 but integration of the research in the policy-making process is often lagging. We looked at how research on HRH contributes or not to inform policy decisions and interventions affecting the health workforce in Portugal and Brazil. We designed a comparative case study of semi-structured interviews with present and past national decision-<span class="hlt">makers</span>, policy advisors and researchers. Issues explored included the existence of a national HRH policy and the use, or non-use, of research evidence by policy <span class="hlt">makers</span> and reasons to do so. Interviews were audio recorded, transcribed, anonymized and analysed thematically. Policy-<span class="hlt">makers</span> in Brazil recognize a greater use of evidence in the process of defining HRH policy when compared to Portugal's. But the existence of formal instruments to support policy development is not sufficient to ensure that policies are informed by evidence. In both countries the importance of the use of evidence in the formulation of policies was recognized by policy-<span class="hlt">makers</span>. However, the influence of other factors, such as political <span class="hlt">pressures</span> from various lobby groups and from the media and the policy short timeframe which requires rapid responses, is predominant.</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-<span class="hlt">wave</span>-induced adverse <span class="hlt">pressure</span> gradient. 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-<span class="hlt">wave</span>-induced adverse <span class="hlt">pressure</span> gradient 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> gradient was induced by an externally generated conical shock <span class="hlt">wave</span>. 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> gradient. 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-<span class="hlt">wave</span> - boundary-layer interaction significantly alters the turbulent mixing characteristics of the boundary layer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005ApPhL..86u1502N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005ApPhL..86u1502N"><span>Effects of oxygen radicals in low-<span class="hlt">pressure</span> surface-<span class="hlt">wave</span> plasma on sterilization</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nagatsu, Masaaki; Terashita, Fumie; Nonaka, Hiroyuki; Xu, Lei; Nagata, Toshi; Koide, Yukio</p> <p>2005-05-01</p> <p>The effects of oxygen radicals on sterilization were studied using a 2.45GHz surface-<span class="hlt">wave</span> oxygen plasma. A population of 1.5×106 Bacillus stearothermophilus spores was irradiated for 3min or more with oxygen plasma, generated at <span class="hlt">pressures</span> between 6 and 14Pa. The decimal reduction value (D value), a measure of the effectiveness of sterilization, was determined to be about 15-25s. Using only oxygen radicals, excluding all charged particles, the 1.5×106 spores were sterilized with a D value of 30-45s after 5min or more of irradiation. On scanning electron microscopy, the length and width of the spores changed significantly due to chemical etching by oxygen radicals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19830000483&hterms=plating&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dplating','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19830000483&hterms=plating&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dplating"><span><span class="hlt">Portable</span> Plating System</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Flores, R.</p> <p>1984-01-01</p> <p>Plating system mounted on <span class="hlt">portable</span> cart includes 30-gallon (23.5 liter) electrolyte tank, filler pump, heaters, replenishing anodes, plating rectifiers and tank rectifier to continously remove contaminants.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title46-vol4/pdf/CFR-2014-title46-vol4-sec107-235.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title46-vol4/pdf/CFR-2014-title46-vol4-sec107-235.pdf"><span>46 CFR 107.235 - Servicing of hand <span class="hlt">portable</span> fire extinguishers, semi-<span class="hlt">portable</span> fire extinguishers and fixed fire...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-10-01</p> <p>... 46 Shipping 4 2014-10-01 2014-10-01 false Servicing of hand <span class="hlt">portable</span> fire extinguishers, semi-<span class="hlt">portable</span> fire extinguishers and fixed fire extinguishing systems. 107.235 Section 107.235 Shipping COAST GUARD, DEPARTMENT OF HOMELAND SECURITY (CONTINUED) A-MOBILE OFFSHORE DRILLING UNITS INSPECTION AND...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title46-vol4/pdf/CFR-2011-title46-vol4-sec107-235.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title46-vol4/pdf/CFR-2011-title46-vol4-sec107-235.pdf"><span>46 CFR 107.235 - Servicing of hand <span class="hlt">portable</span> fire extinguishers, semi-<span class="hlt">portable</span> fire extinguishers and fixed fire...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-10-01</p> <p>... 46 Shipping 4 2011-10-01 2011-10-01 false Servicing of hand <span class="hlt">portable</span> fire extinguishers, semi-<span class="hlt">portable</span> fire extinguishers and fixed fire-extinguishing systems. 107.235 Section 107.235 Shipping COAST GUARD, DEPARTMENT OF HOMELAND SECURITY (CONTINUED) A-MOBILE OFFSHORE DRILLING UNITS INSPECTION AND...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol4/pdf/CFR-2010-title46-vol4-sec107-235.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol4/pdf/CFR-2010-title46-vol4-sec107-235.pdf"><span>46 CFR 107.235 - Servicing of hand <span class="hlt">portable</span> fire extinguishers, semi-<span class="hlt">portable</span> fire extinguishers and fixed fire...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 46 Shipping 4 2010-10-01 2010-10-01 false Servicing of hand <span class="hlt">portable</span> fire extinguishers, semi-<span class="hlt">portable</span> fire extinguishers and fixed fire-extinguishing systems. 107.235 Section 107.235 Shipping COAST GUARD, DEPARTMENT OF HOMELAND SECURITY (CONTINUED) A-MOBILE OFFSHORE DRILLING UNITS INSPECTION AND...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title46-vol4/pdf/CFR-2012-title46-vol4-sec107-235.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title46-vol4/pdf/CFR-2012-title46-vol4-sec107-235.pdf"><span>46 CFR 107.235 - Servicing of hand <span class="hlt">portable</span> fire extinguishers, semi-<span class="hlt">portable</span> fire extinguishers and fixed fire...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... 46 Shipping 4 2012-10-01 2012-10-01 false Servicing of hand <span class="hlt">portable</span> fire extinguishers, semi-<span class="hlt">portable</span> fire extinguishers and fixed fire extinguishing systems. 107.235 Section 107.235 Shipping COAST GUARD, DEPARTMENT OF HOMELAND SECURITY (CONTINUED) A-MOBILE OFFSHORE DRILLING UNITS INSPECTION AND...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title46-vol4/pdf/CFR-2013-title46-vol4-sec107-235.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title46-vol4/pdf/CFR-2013-title46-vol4-sec107-235.pdf"><span>46 CFR 107.235 - Servicing of hand <span class="hlt">portable</span> fire extinguishers, semi-<span class="hlt">portable</span> fire extinguishers and fixed fire...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... 46 Shipping 4 2013-10-01 2013-10-01 false Servicing of hand <span class="hlt">portable</span> fire extinguishers, semi-<span class="hlt">portable</span> fire extinguishers and fixed fire extinguishing systems. 107.235 Section 107.235 Shipping COAST GUARD, DEPARTMENT OF HOMELAND SECURITY (CONTINUED) A-MOBILE OFFSHORE DRILLING UNITS INSPECTION AND...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170010284','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170010284"><span>Development Specification for RV-346/348 Positive <span class="hlt">Pressure</span> Relief Valves (PPRV)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ralston, Russell L.</p> <p>2017-01-01</p> <p>This specification establishes the requirements for design, performance, safety, testing, and manufacture of the RV-346 and RV-348, Positive <span class="hlt">Pressure</span> Relief Valve (PPRV) as part of the Advanced Extravehicular Mobility Unit (EMU)(AEMU) <span class="hlt">Portable</span> Life Support System (PLSS). The RV-346 serves as the Positive <span class="hlt">Pressure</span> Relief Valve (PPRV), and the RV-348 serves as the Secondary Positive <span class="hlt">Pressure</span> Relief Valve (SPPRV).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/969240','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/969240"><span><span class="hlt">Pressure</span> dependence of the optical properties of the charge-density-<span class="hlt">wave</span> compound LaTe2</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>Lavagnini, M.; Sacchetti, A.; Degiorgi, L.</p> <p>2009-12-14</p> <p>We report the <span class="hlt">pressure</span> dependence of the optical response of LaTe{sub 2}, which is deep in the charge-density-<span class="hlt">wave</span> (CDW) ground state even at 300 K. The reflectivity spectrum is collected in the mid-infrared spectral range at room temperature and at <span class="hlt">pressures</span> between 0 and 7 GPa. We extract the energy scale due to the single particle excitation across the CDW gap and the Drude weight. We establish that the gap decreases upon compressing the lattice, while the Drude weight increases. This signals a reduction in the quality of nesting upon applying <span class="hlt">pressure</span>, therefore inducing a lesser impact of the CDWmore » condensate on the electronic properties of LaTe{sub 2}. The consequent suppression of the CDW gap leads to a release of additional charge carriers, manifested by the shift of weight from the gap feature into the metallic component of the optical response. On the contrary, the power-law behavior, seen in the optical conductivity at energies above the gap excitation and indicating a weakly interacting limit within the Tomonaga-Luttinger liquid scenario, seems to be only moderately dependent on <span class="hlt">pressure</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.loc.gov/pictures/collection/hh/item/hi0052.photos.058589p/','SCIGOV-HHH'); return false;" href="https://www.loc.gov/pictures/collection/hh/item/hi0052.photos.058589p/"><span>9. RW Meyer Sugar Mill: 18761889. Locomotivetype, firetube, <span class="hlt">portable</span> boiler, ...</span></a></p> <p><a target="_blank" href="http://www.loc.gov/pictures/collection/hh/">Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey</a></p> <p></p> <p></p> <p>9. RW Meyer Sugar Mill: 1876-1889. Locomotive-type, fire-tube, <span class="hlt">portable</span> boiler, No. 1 model. Manufactured by Ames Iron Works, Oswego, New York, 1879. 120 lbs/sq. inch working <span class="hlt">pressure</span>, 66 sq. ft. heating surface in tubes. View: from side. The boiler provided steam for steam engine which in turn powered the mill's centrifugals. The section on the left side included the firebox with its surrounding water-legs. The fluted chimney-type structure is the steam port, safety valve, and whistle. Column projecting from side was part of steam <span class="hlt">pressure</span> and water gauge. Pipe running above boiler carried steam to the engine. Pipe running below boiler provided the boiler feed-water. Cylindrical section included 22 fire-tube surrounded by water. The far right ... - R. W. Meyer Sugar Mill, State Route 47, Kualapuu, Maui County, HI</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5222553','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5222553"><span>Forward and Backward <span class="hlt">Pressure</span> Waveform Morphology in Hypertension</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Li, Ye; Gu, Haotian; Fok, Henry; Alastruey, Jordi</p> <p>2017-01-01</p> <p>We tested the hypothesis that increased pulse <span class="hlt">wave</span> reflection and altered backward waveform morphology contribute to increased pulse <span class="hlt">pressure</span> in subjects with higher pulse <span class="hlt">pressure</span> compared with lower pulse <span class="hlt">pressure</span> and to actions of vasoactive drugs to increase pulse <span class="hlt">pressure</span>. We examined the relationship of backward to forward <span class="hlt">wave</span> morphology in 158 subjects who were evaluated for hypertension (including some normotensive subjects) divided into 3 groups by central pulse <span class="hlt">pressure</span>: group 1, 33±6.5 mm Hg; group 2, 45±4.1 mm Hg; and group 3, 64±12.9 mm Hg (means±SD) and in healthy normotensive subjects during administration of inotropic and vasomotor drugs. Aortic <span class="hlt">pressure</span> and flow in the aortic root were estimated by carotid tonometry and Doppler sonography, respectively. Morphology of the backward <span class="hlt">wave</span> relative to the forward <span class="hlt">wave</span> was similar in subjects in the lowest and highest tertiles of pulse <span class="hlt">pressure</span>. Similar results were seen with the inotropic, vasopressor and vasodilator drugs, dobutamine, norepinephrine, and phentolamine, with the backward <span class="hlt">wave</span> maintaining a constant ratio to the forward <span class="hlt">wave</span>. However, nitroglycerin, a drug with a specific action to dilate muscular conduit arteries, reduced the amplitude of the backward <span class="hlt">wave</span> relative to the forward <span class="hlt">wave</span> from 0.26±0.018 at baseline to 0.19±0.019 during nitroglycerin 30 μg/min IV (P<0.01). These results are best explained by an approximately constant amount of reflection of the forward <span class="hlt">wave</span> from the peripheral vasculature. The amount of reflection can be modified by dilation of peripheral muscular conduit arteries but contributes little to increased pulse <span class="hlt">pressure</span> in hypertension. PMID:27920128</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27920128','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27920128"><span>Forward and Backward <span class="hlt">Pressure</span> Waveform Morphology in Hypertension.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Ye; Gu, Haotian; Fok, Henry; Alastruey, Jordi; Chowienczyk, Philip</p> <p>2017-02-01</p> <p>We tested the hypothesis that increased pulse <span class="hlt">wave</span> reflection and altered backward waveform morphology contribute to increased pulse <span class="hlt">pressure</span> in subjects with higher pulse <span class="hlt">pressure</span> compared with lower pulse <span class="hlt">pressure</span> and to actions of vasoactive drugs to increase pulse <span class="hlt">pressure</span>. We examined the relationship of backward to forward <span class="hlt">wave</span> morphology in 158 subjects who were evaluated for hypertension (including some normotensive subjects) divided into 3 groups by central pulse <span class="hlt">pressure</span>: group 1, 33±6.5 mm Hg; group 2, 45±4.1 mm Hg; and group 3, 64±12.9 mm Hg (means±SD) and in healthy normotensive subjects during administration of inotropic and vasomotor drugs. Aortic <span class="hlt">pressure</span> and flow in the aortic root were estimated by carotid tonometry and Doppler sonography, respectively. Morphology of the backward <span class="hlt">wave</span> relative to the forward <span class="hlt">wave</span> was similar in subjects in the lowest and highest tertiles of pulse <span class="hlt">pressure</span>. Similar results were seen with the inotropic, vasopressor and vasodilator drugs, dobutamine, norepinephrine, and phentolamine, with the backward <span class="hlt">wave</span> maintaining a constant ratio to the forward <span class="hlt">wave</span>. However, nitroglycerin, a drug with a specific action to dilate muscular conduit arteries, reduced the amplitude of the backward <span class="hlt">wave</span> relative to the forward <span class="hlt">wave</span> from 0.26±0.018 at baseline to 0.19±0.019 during nitroglycerin 30 μg/min IV (P<0.01). These results are best explained by an approximately constant amount of reflection of the forward <span class="hlt">wave</span> from the peripheral vasculature. The amount of reflection can be modified by dilation of peripheral muscular conduit arteries but contributes little to increased pulse <span class="hlt">pressure</span> in hypertension. © 2016 The Authors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA551992','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA551992"><span>Relationship between Orientation to a Blast and <span class="hlt">Pressure</span> <span class="hlt">Wave</span> Propagation Inside the Rat Brian</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2011-01-01</p> <p>8217·’ 2.9 ± 0.4’ ·• 64 M. Chavko ec at. I j ournal of Neuroscience Mecl1ods 195 (20!1 ) 61-66 A 60 ~ c 60 ~ ------> ------> 40 40 ~ 20 20 v :; VI...WA, Prusaczyk WK. McCarron RM. Measurement or blast <span class="hlt">wave</span> by a miniature fiber optic <span class="hlt">pressure</span> transducer in the rat brain. J Neurosci Methods...AI. Blast related neuro- trauma: a review or cellular injury. Mol Cell Biomech 2008;3: 155-68. ling G. Bandak F, Armonda R, Grant G, Ecklund J</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=role+AND+rational+AND+decision+AND+making&pg=4&id=ED326850','ERIC'); return false;" href="https://eric.ed.gov/?q=role+AND+rational+AND+decision+AND+making&pg=4&id=ED326850"><span>Teacher as Decision-<span class="hlt">Maker</span>.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Smith, Carl B.</p> <p></p> <p>The teacher as decisionmaker is a fairly new concept, and yet the choices teachers make--among alternative approaches--afffect the attitudes, knowledge, and skills students carry into adult life. This booklet's chapter titles are as follows: (1) New Image for Teachers--Decision-<span class="hlt">Maker</span>; (2) Decisions Teachers Make; (3) A Rational Model; (4) Planning…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940034837&hterms=computer+networking&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dcomputer%2Bnetworking','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940034837&hterms=computer+networking&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dcomputer%2Bnetworking"><span>Embedded Data Processor and <span class="hlt">Portable</span> Computer Technology testbeds</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Alena, Richard; Liu, Yuan-Kwei; Goforth, Andre; Fernquist, Alan R.</p> <p>1993-01-01</p> <p>Attention is given to current activities in the Embedded Data Processor and <span class="hlt">Portable</span> Computer Technology testbed configurations that are part of the Advanced Data Systems Architectures Testbed at the Information Sciences Division at NASA Ames Research Center. The Embedded Data Processor Testbed evaluates advanced microprocessors for potential use in mission and payload applications within the Space Station Freedom Program. The <span class="hlt">Portable</span> Computer Technology (PCT) Testbed integrates and demonstrates advanced <span class="hlt">portable</span> computing devices and data system architectures. The PCT Testbed uses both commercial and custom-developed devices to demonstrate the feasibility of functional expansion and networking for <span class="hlt">portable</span> computers in flight missions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=ELEMENTS+AND+OF+AND+THE+AND+DECISION+AND+MAKING+AND+PROCESS&pg=2&id=EJ1130982','ERIC'); return false;" href="https://eric.ed.gov/?q=ELEMENTS+AND+OF+AND+THE+AND+DECISION+AND+MAKING+AND+PROCESS&pg=2&id=EJ1130982"><span><span class="hlt">Maker</span> Principles and Technologies in Teacher Education: A National Survey</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>Cohen, Jonathan</p> <p>2017-01-01</p> <p>Broadly speaking, the <span class="hlt">maker</span> movement is characterized by people who engage in the construction, deconstruction, and reconstruction of physical artifacts, and who share both the process of making and their physical products with the broader community of <span class="hlt">makers</span>. There is growing sentiment that elements of the <span class="hlt">maker</span> movement have the capability of…</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/25988634','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25988634"><span><span class="hlt">Portable</span> infrared pupillometry: a review.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Larson, Merlin D; Behrends, Matthias</p> <p>2015-06-01</p> <p><span class="hlt">Portable</span> infrared pupillometers provide an objective measure of pupil size and pupillary reflexes, which for most clinicians was previously only a visual impression. But despite the fact that pupillometry can uncover aspects of how the human pupil reacts to drugs and noxious stimulation, the use of pupillometry has not gained widespread use among anesthesiologists and critical care physicians. The present review is an introduction to the physiology of pupillary reflexes and the currently established clinical applications of infrared pupillometry, which will hopefully encourage physicians to use this diagnostic tool in their clinical practice. <span class="hlt">Portable</span> infrared pupillometry was introduced in 1989. The technology involves flooding the eye with infrared light and then measuring the reflected image on an infrared sensor. Pupil size, along with variables of the pupillary light reflex and pupillary reflex dilation, is calculated by the instrument and displayed on a screen immediately after each time-stamped measurement. Use of these instruments has uncovered aspects of how the human pupil reacts to drugs and noxious stimulation. The primary clinical applications for <span class="hlt">portable</span> pupillometry have been in the assessment of brainstem function. <span class="hlt">Portable</span> pupillometry is useful in the management of pain because it allows for assessments of the effect of opioids and in the titration of combined regional-general anesthetics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18664288','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18664288"><span>The velocity of the arterial pulse <span class="hlt">wave</span>: a viscous-fluid shock <span class="hlt">wave</span> in an elastic tube.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Painter, Page R</p> <p>2008-07-29</p> <p>The arterial pulse is a viscous-fluid shock <span class="hlt">wave</span> that is initiated by blood ejected from the heart. This <span class="hlt">wave</span> travels away from the heart at a speed termed the pulse <span class="hlt">wave</span> velocity (PWV). The PWV increases during the course of a number of diseases, and this increase is often attributed to arterial stiffness. As the pulse <span class="hlt">wave</span> approaches a point in an artery, the <span class="hlt">pressure</span> rises as does the <span class="hlt">pressure</span> gradient. This <span class="hlt">pressure</span> gradient increases the rate of blood flow ahead of the <span class="hlt">wave</span>. The rate of blood flow ahead of the <span class="hlt">wave</span> decreases with distance because the <span class="hlt">pressure</span> gradient also decreases with distance ahead of the <span class="hlt">wave</span>. Consequently, the amount of blood per unit length in a segment of an artery increases ahead of the <span class="hlt">wave</span>, and this increase stretches the wall of the artery. As a result, the tension in the wall increases, and this results in an increase in the <span class="hlt">pressure</span> of blood in the artery. An expression for the PWV is derived from an equation describing the flow-<span class="hlt">pressure</span> coupling (FPC) for a pulse <span class="hlt">wave</span> in an incompressible, viscous fluid in an elastic tube. The initial increase in force of the fluid in the tube is described by an increasing exponential function of time. The relationship between force gradient and fluid flow is approximated by an expression known to hold for a rigid tube. For large arteries, the PWV derived by this method agrees with the Korteweg-Moens equation for the PWV in a non-viscous fluid. For small arteries, the PWV is approximately proportional to the Korteweg-Moens velocity divided by the radius of the artery. The PWV in small arteries is also predicted to increase when the specific rate of increase in <span class="hlt">pressure</span> as a function of time decreases. This rate decreases with increasing myocardial ischemia, suggesting an explanation for the observation that an increase in the PWV is a predictor of future myocardial infarction. The derivation of the equation for the PWV that has been used for more than fifty years is analyzed and shown to yield</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/867216','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/867216"><span><span class="hlt">Portable</span> system and method combining chromatography and array of electrochemical sensors</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Zaromb, Solomon; Stetter, Joseph R.</p> <p>1989-01-01</p> <p>A <span class="hlt">portable</span> system for analyzing a fluid sample includes a small, <span class="hlt">portable</span>, low-<span class="hlt">pressure</span> and low-power chromatographic analyzer and a chemical parameter spectrometry monitor including an array of sensors for detecting, identifying and measuring the concentrations of a variety of components in the eluent from the chromatographic analyzer. The monitor includes one or more operating condition controllers which may be used to change one or more of the operating conditions during exposure of the sensors to the eluent from the chromatography analyzer to form a response pattern which is then compared with a library of previously established patterns. Gas and liquid chromatographic embodiments are disclosed. In the gas embodiment, the operating condition controllers include heated filaments which may convert electrochemically inactive components to electrochemically active products. In the liquid chromatography embodiment, low-power, liquid-phase equivalents of heated filaments are used with appropriate sensors. The library response patterns may be divided into subsets and the formed pattern may be assigned for comparison only with the patterns of a particular subset.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3462261','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3462261"><span>Stone Comminution Correlates with the Average Peak <span class="hlt">Pressure</span> Incident on a Stone during Shock <span class="hlt">Wave</span> Lithotripsy</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Smith, N.; Zhong, P.</p> <p>2012-01-01</p> <p>To investigate the roles of lithotripter shock <span class="hlt">wave</span> (LSW) parameters and cavitation in stone comminution, a series of in vitro fragmentation experiments have been conducted in water and 1,3-butanediol (a cavitation-suppressive fluid) at a variety of acoustic field positions of an electromagnetic shock <span class="hlt">wave</span> lithotripter. Using field mapping data and integrated parameters averaged over a circular stone holder area (Rh = 7 mm), close logarithmic correlations between the average peak <span class="hlt">pressure</span> (P+(avg)) incident on the stone (D = 10 mm BegoStone) and comminution efficiency after 500 and 1,000 shocks have been identified. Moreover, the correlations have demonstrated distinctive thresholds in P+(avg) (5.3 MPa and 7.6 MPa for soft and hard stones, respectively), that are required to initiate stone fragmentation independent of surrounding fluid medium and LSW dose. These observations, should they be confirmed using other shock <span class="hlt">wave</span> lithotripters, may provide an important field parameter (i.e., P+(avg)) to guide appropriate application of SWL in clinics, and facilitate device comparison and design improvements in future lithotripters. PMID:22935690</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22935690','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22935690"><span>Stone comminution correlates with the average peak <span class="hlt">pressure</span> incident on a stone during shock <span class="hlt">wave</span> lithotripsy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Smith, N; Zhong, P</p> <p>2012-10-11</p> <p>To investigate the roles of lithotripter shock <span class="hlt">wave</span> (LSW) parameters and cavitation in stone comminution, a series of in vitro fragmentation experiments have been conducted in water and 1,3-butanediol (a cavitation-suppressive fluid) at a variety of acoustic field positions of an electromagnetic shock <span class="hlt">wave</span> lithotripter. Using field mapping data and integrated parameters averaged over a circular stone holder area (R(h)=7 mm), close logarithmic correlations between the average peak <span class="hlt">pressure</span> (P(+(avg))) incident on the stone (D=10 mm BegoStone) and comminution efficiency after 500 and 1000 shocks have been identified. Moreover, the correlations have demonstrated distinctive thresholds in P(+(avg)) (5.3 MPa and 7.6 MPa for soft and hard stones, respectively), that are required to initiate stone fragmentation independent of surrounding fluid medium and LSW dose. These observations, should they be confirmed using other shock <span class="hlt">wave</span> lithotripters, may provide an important field parameter (i.e., P(+(avg))) to guide appropriate application of SWL in clinics, and facilitate device comparison and design improvements in future lithotripters. Copyright © 2012 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22594614-influence-field-emission-propagation-cylindrical-fast-ionization-wave-atmospheric-pressure-nitrogen','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22594614-influence-field-emission-propagation-cylindrical-fast-ionization-wave-atmospheric-pressure-nitrogen"><span>Influence of field emission on the propagation of cylindrical fast ionization <span class="hlt">wave</span> in atmospheric-<span class="hlt">pressure</span> nitrogen</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>Levko, Dmitry; Raja, Laxminarayan L.</p> <p>2016-04-21</p> <p>The influence of field emission of electrons from surfaces on the fast ionization <span class="hlt">wave</span> (FIW) propagation in high-voltage nanosecond pulse discharge in the atmospheric-<span class="hlt">pressure</span> nitrogen is studied by a one-dimensional Particle-in-Cell Monte Carlo Collisions model. A strong influence of field emission on the FIW dynamics and plasma parameters is obtained. Namely, the accounting for the field emission makes possible the bridging of the cathode–anode gap by rather dense plasma (∼10{sup 13 }cm{sup −3}) in less than 1 ns. This is explained by the generation of runaway electrons from the field emitted electrons. These electrons are able to cross the entire gap pre-ionizingmore » it and promoting the ionization <span class="hlt">wave</span> propagation. We have found that the propagation of runaway electrons through the gap cannot be accompanied by the streamer propagation, because the runaway electrons align the plasma density gradients. In addition, we have obtained that the field enhancement factor allows controlling the speed of ionization <span class="hlt">wave</span> propagation.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26592464','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26592464"><span>Hand-<span class="hlt">portable</span> liquid chromatographic instrumentation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sharma, Sonika; Tolley, Luke T; Tolley, H Dennis; Plistil, Alex; Stearns, Stanley D; Lee, Milton L</p> <p>2015-11-20</p> <p>Over the last four decades, liquid chromatography (LC) has experienced an evolution to smaller columns and particles, new stationary phases and low flow rate instrumentation. However, the development of person-<span class="hlt">portable</span> LC has not followed, mainly due to difficulties encountered in miniaturizing pumps and detectors, and in reducing solvent consumption. The recent introduction of small, non-splitting pumping systems and UV-absorption detectors for use with capillary columns has finally provided miniaturized instrumentation suitable for high-performance hand-<span class="hlt">portable</span> LC. Fully integrated microfabricated LC still remains a significant challenge. Ion chromatography (IC) has been successfully miniaturized and applied for field analysis; however, applications are mostly limited to inorganic and small organic ions. This review covers advancements that make possible more rapid expansion of <span class="hlt">portable</span> forms of LC and IC. Copyright © 2015 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100020863','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100020863"><span>Space Suit <span class="hlt">Portable</span> Life Support System Rapid Cycle Amine Repackaging and Sub-Scale Test Results</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Paul, Heather L.; Rivera, Fatonia L.</p> <p>2010-01-01</p> <p>NASA is developing technologies to meet requirements for an extravehicular activity (EVA) <span class="hlt">Portable</span> Life Support System (PLSS) for exploration. The PLSS Ventilation Subsystem transports clean, conditioned oxygen to the <span class="hlt">pressure</span> garment for space suit <span class="hlt">pressurization</span> and human consumption, and recycles the ventilation gas, removing carbon dioxide, humidity, and trace contaminants. This paper provides an overview of the development efforts conducted at the NASA Johnson Space Center to redesign the Rapid Cycle Amine (RCA) canister and valve assembly into a radial flow, cylindrical package for carbon dioxide and humidity control of the PLSS ventilation loop. Future work is also discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19740029285&hterms=falling+meteors&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfalling%2Bmeteors','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19740029285&hterms=falling+meteors&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfalling%2Bmeteors"><span>Upper atmospheric planetary-<span class="hlt">wave</span> and gravity-<span class="hlt">wave</span> observations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Justus, C. G.; Woodrum, A.</p> <p>1973-01-01</p> <p>Previously collected data on atmospheric <span class="hlt">pressure</span>, density, temperature and winds between 25 and 200 km from sources including Meteorological Rocket Network data, ROBIN falling sphere data, grenade release and pitot tube data, meteor winds, chemical release winds, satellite data, and others were analyzed by a daily-difference method, and results on the magnitude of atmospheric perturbations interpreted as gravity <span class="hlt">waves</span> and planetary <span class="hlt">waves</span> are presented. Traveling planetary-<span class="hlt">wave</span> contributions in the 25-85 km range were found to have significant height and latitudinal variation. It was found that observed gravity-<span class="hlt">wave</span> density perturbations and wind are related to one another in the manner predicted by gravity-<span class="hlt">wave</span> theory. It was determined that, on the average, gravity-<span class="hlt">wave</span> energy deposition or reflection occurs at all altitudes except the 55-75 km region of the mesosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25219240','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25219240"><span>[Research and development of <span class="hlt">portable</span> hypertension therapeutic apparatus based on biofeedback mechanism].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Huang, Rong; He, Hongmei; Pi, Xitian; Diao, Ziji; Zhao, Suwen</p> <p>2014-06-01</p> <p>Non-drug treatment of hypertension has become a research hotspot, which might overcome the heavy economic burden and side effects of drug treatment for the patients. Because of the good treatment effect and convenient operation, a new treatment based on slow breathing training is increasingly becoming a kind of physical therapy for hypertension. This paper explains the principle of hypertension treatment based on slow breathing training method, and introduces the overall structure of the <span class="hlt">portable</span> blood <span class="hlt">pressure</span> controlling instrument, including breathing detection circuit, the core control module, audio module, memory module and man-machine interaction module. We give a brief introduction to the instrument and the software in this paper. The prototype testing results showed that the treatment had a significant effect on controlling the blood <span class="hlt">pressure</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29202078','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29202078"><span>Global climate change: impact of heat <span class="hlt">waves</span> under different definitions on daily mortality in Wuhan, China.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Yunquan; Feng, Renjie; Wu, Ran; Zhong, Peirong; Tan, Xiaodong; Wu, Kai; Ma, Lu</p> <p>2017-01-01</p> <p>There was no consistent definition for heat <span class="hlt">wave</span> worldwide, while a limited number of studies have compared the mortality effect of heat <span class="hlt">wave</span> as defined differently. This paper aimed to provide epidemiological evidence for policy <span class="hlt">makers</span> to determine the most appropriate definition for local heat <span class="hlt">wave</span> warning systems. We developed 45 heat <span class="hlt">wave</span> definitions (HWs) combining temperature indicators and temperature thresholds with durations. We then assessed the impact of heat <span class="hlt">waves</span> under various definitions on non-accidental mortality in hot season (May-September) in Wuhan, China during 2003-2010. Heat <span class="hlt">waves</span> defined by HW14 (daily mean temperature ≥ 99.0th percentile and duration ≥ 3 days) had the best predictive ability in assessing the mortality effects of heat <span class="hlt">wave</span> with the relative risk of 1.63 (95% CI : 1.43, 1.89) for total mortality. The group-specific mortality risk using official heat <span class="hlt">wave</span> definition of Chinese Meteorological Administration was much smaller than that using HW14. We also found that women, and the elderly (age ≥ 65) were more susceptible to heat <span class="hlt">wave</span> effects which were stronger and longer lasting. These findings suggest that region specific heat <span class="hlt">wave</span> definitions are crucial and necessary for developing efficient local heat warning systems and for providing evidence for policy <span class="hlt">makers</span> to protect the vulnerable population.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27548787','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27548787"><span>High-Intensity Interval Cycling Exercise on <span class="hlt">Wave</span> Reflection and Pulse <span class="hlt">Wave</span> Velocity.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kingsley, J Derek; Tai, Yu Lun; Vaughan, Jeremiah A; Mayo, Xián</p> <p>2017-05-01</p> <p>Kingsley, JD, Tai, YL, Vaughan, J, and Mayo, X. High-intensity interval cycling exercise on <span class="hlt">wave</span> reflection and pulse <span class="hlt">wave</span> velocity. J Strength Cond Res 31(5): 1313-1320, 2017-The purpose of this study was to assess the effects of high-intensity exercise on <span class="hlt">wave</span> reflection and aortic stiffness. Nine young, healthy men (mean ± SD: age: 22 ± 2 years) participated in the study. The high-intensity interval cycling exercise consisted of 3 sets of Wingate Anaerobic Tests (WATs) with 7.5% of bodyweight as resistance and 2 minutes of rest between each set. Measurements were taken at rest and 1 minute after completion of the WATs. Brachial and aortic blood <span class="hlt">pressures</span>, as well as <span class="hlt">wave</span> reflection characteristics, were measured through pulse <span class="hlt">wave</span> analysis. Aortic stiffness was assessed through carotid-femoral pulse <span class="hlt">wave</span> velocity (cfPWV). A repeated-measures analysis of variance was used to investigate the effects of the WATs on blood <span class="hlt">pressure</span> and vascular function across time. There was no change in brachial or aortic systolic <span class="hlt">pressure</span> from rest to recovery. There was a significant (p ≤ 0.05) decrease in brachial diastolic <span class="hlt">pressure</span> (rest: 73 ± 6 mm Hg; recovery: 67 ± 9 mm Hg) and aortic diastolic <span class="hlt">pressure</span> (rest: 75 ± 6 mm Hg; recovery: 70 ± 9 mm Hg) from rest to recovery. In addition, there was no significant change in the augmentation index (rest: 111.4 ± 6.5%; recovery: 109.8 ± 5.8%, p = 0.65) from rest to recovery. However, there was a significant (p ≤ 0.05) increase in the augmentation index normalized at 75 b·min (rest: 3.29 ± 9.82; recovery 21.21 ± 10.87) during recovery compared with rest. There was no change in cfPWV (rest: 5.3 ± 0.8 m·s; recovery: 5.7 ± 0.5m·s; p = 0.09) in response to the WAT. These data demonstrate that high-intensity interval cycling exercise with short rest periods has a nonsignificant effect on vascular function.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28012054','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28012054"><span>Licensing Surrogate Decision-<span class="hlt">Makers</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rosoff, Philip M</p> <p>2017-06-01</p> <p>As medical technology continues to improve, more people will live longer lives with multiple chronic illnesses with increasing cumulative debilitation, including cognitive dysfunction. Combined with the aging of society in most developed countries, an ever-growing number of patients will require surrogate decision-<span class="hlt">makers</span>. While advance care planning by patients still capable of expressing their preferences about medical interventions and end-of-life care can improve the quality and accuracy of surrogate decisions, this is often not the case, not infrequently leading to demands for ineffective, inappropriate and prolonged interventions. In 1980 LaFollette called for the licensing of prospective parents, basing his argument on the harm they can do to vulnerable people (children). In this paper, I apply his arguments to surrogate decision-<span class="hlt">makers</span> for cognitively incapacitated patients, rhetorically suggesting that we require potential surrogates to qualify for this position by demonstrating their ability to make reasonable and rational decisions for others. I employ this theoretical approach to argue that the loose criteria by which we authorize surrogates' generally unchallenged power should be reconsidered.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29394452','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29394452"><span>Development of a <span class="hlt">portable</span> quality control application using a tablet-type electronic device.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ono, Tomohiro; Miyabe, Yuki; Akimoto, Mami; Mukumoto, Nobutaka; Ishihara, Yoshitomo; Nakamura, Mitsuhiro; Mizowaki, Takashi</p> <p>2018-03-01</p> <p>Our aim was to develop a <span class="hlt">portable</span> quality control (QC) application using a thermometer, a barometer, an angle gauge, and a range finder implemented in a tablet-type consumer electronic device (CED) and to assess the accuracies of the measurements made. The QC application was programmed using Java and OpenCV libraries. First, temperature and atmospheric <span class="hlt">pressure</span> were measured over 30 days using the temperature and <span class="hlt">pressure</span> sensors of the CED and compared with those measured by a double-tube thermometer and a digital barometer. Second, the angle gauge was developed using the accelerometer of the CED. The roll and pitch angles of the CED were measured from 0 to 90° at intervals of 10° in the clockwise (CW) and counterclockwise (CCW) directions. The values were compared with those measured by a digital angle gauge. Third, a range finder was developed using the tablet's built-in camera and image-processing capacities. Surrogate markers were detected by the camera and their positions converted to actual positions using a homographic transformation method. Fiducial markers were placed on a treatment couch and moved 100 mm in 10-mm steps in both the lateral and longitudinal directions. The values were compared with those measured by the digital output of the treatment couch. The differences between CED values and those of other devices were compared by calculating means ± standard deviations (SDs). The means ± SDs of differences in temperature and atmospheric <span class="hlt">pressure</span> were -0.07 ± 0.25°C and 0.05 ± 0.10 hPa, respectively. The means ± SDs of the difference in angle was -0.17 ± 0.87° (0.15 ± 0.23° degrees excluding the 90° angle). The means ± SDs of distances were 0.01 ± 0.07 mm in both the lateral and longitudinal directions. Our <span class="hlt">portable</span> QC application was accurate and may be used instead of standard measuring devices. Our <span class="hlt">portable</span> CED is efficient and simple when used in the field of medical physics. © 2018 American Association of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title49-vol3/pdf/CFR-2014-title49-vol3-sec178-255.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title49-vol3/pdf/CFR-2014-title49-vol3-sec178-255.pdf"><span>49 CFR 178.255 - Specification 60; steel <span class="hlt">portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-10-01</p> <p>... 49 Transportation 3 2014-10-01 2014-10-01 false Specification 60; steel <span class="hlt">portable</span> tanks. 178.255 Section 178.255 Transportation Other Regulations Relating to Transportation (Continued) PIPELINE AND... PACKAGINGS Specifications for <span class="hlt">Portable</span> Tanks § 178.255 Specification 60; steel <span class="hlt">portable</span> tanks. ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title49-vol3/pdf/CFR-2013-title49-vol3-sec178-255.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title49-vol3/pdf/CFR-2013-title49-vol3-sec178-255.pdf"><span>49 CFR 178.255 - Specification 60; steel <span class="hlt">portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-10-01</p> <p>... 49 Transportation 3 2013-10-01 2013-10-01 false Specification 60; steel <span class="hlt">portable</span> tanks. 178.255 Section 178.255 Transportation Other Regulations Relating to Transportation (Continued) PIPELINE AND... PACKAGINGS Specifications for <span class="hlt">Portable</span> Tanks § 178.255 Specification 60; steel <span class="hlt">portable</span> tanks. ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title49-vol2/pdf/CFR-2010-title49-vol2-sec178-255.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title49-vol2/pdf/CFR-2010-title49-vol2-sec178-255.pdf"><span>49 CFR 178.255 - Specification 60; steel <span class="hlt">portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 49 Transportation 2 2010-10-01 2010-10-01 false Specification 60; steel <span class="hlt">portable</span> tanks. 178.255 Section 178.255 Transportation Other Regulations Relating to Transportation PIPELINE AND HAZARDOUS... FOR PACKAGINGS Specifications for <span class="hlt">Portable</span> Tanks § 178.255 Specification 60; steel <span class="hlt">portable</span> tanks. ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title49-vol3/pdf/CFR-2011-title49-vol3-sec178-255.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title49-vol3/pdf/CFR-2011-title49-vol3-sec178-255.pdf"><span>49 CFR 178.255 - Specification 60; steel <span class="hlt">portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-10-01</p> <p>... 49 Transportation 3 2011-10-01 2011-10-01 false Specification 60; steel <span class="hlt">portable</span> tanks. 178.255 Section 178.255 Transportation Other Regulations Relating to Transportation (Continued) PIPELINE AND... PACKAGINGS Specifications for <span class="hlt">Portable</span> Tanks § 178.255 Specification 60; steel <span class="hlt">portable</span> tanks. ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title49-vol3/pdf/CFR-2012-title49-vol3-sec178-255.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title49-vol3/pdf/CFR-2012-title49-vol3-sec178-255.pdf"><span>49 CFR 178.255 - Specification 60; steel <span class="hlt">portable</span> tanks.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... 49 Transportation 3 2012-10-01 2012-10-01 false Specification 60; steel <span class="hlt">portable</span> tanks. 178.255 Section 178.255 Transportation Other Regulations Relating to Transportation (Continued) PIPELINE AND... PACKAGINGS Specifications for <span class="hlt">Portable</span> Tanks § 178.255 Specification 60; steel <span class="hlt">portable</span> tanks. ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4756730','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4756730"><span>Bagworm bags as <span class="hlt">portable</span> armour against invertebrate predators</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2016-01-01</p> <p>Some animals have evolved the use of environmental materials as “<span class="hlt">portable</span> armour” against natural enemies. <span class="hlt">Portable</span> bags that bagworm larvae (Lepidoptera: Psychidae) construct using their own silk and plant parts are generally believed to play an important role as a physical barrier against natural enemies. However, no experimental studies have tested the importance of bags as <span class="hlt">portable</span> armour against predators. To clarify the defensive function, I studied the bagworm Eumeta minuscula and a potential predator Calosoma maximoviczi (Coleoptera: Carabidae). Under laboratory conditions, all bagworm larvae were attacked by carabid adults, but successfully defended themselves against the predators’ mandibles using their own bags. The <span class="hlt">portable</span> bags, which are composed mainly of host plant twigs, may function as a physical barrier against predator mandibles. To test this hypothesis, I removed the twig bags and replaced some with herb leaf bags; all bag-removed larvae were easily caught and predated by carabids, while all bag-replaced larvae could successfully defend themselves against carabid attacks. Therefore, various types of <span class="hlt">portable</span> bags can protect bagworm larvae from carabid attacks. This is the first study to test the defensive function of bagworm <span class="hlt">portable</span> bags against invertebrate predators. PMID:26893969</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. 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