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Dive into the research topics where Allan J. Zuckerwar is active.

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Featured researches published by Allan J. Zuckerwar.


IEEE Transactions on Biomedical Engineering | 1993

Development of a piezopolymer pressure sensor for a portable fetal heart rate monitor

Allan J. Zuckerwar; Robert A. Pretlow; John W. Stoughton; Donald A. Baker

A piezopolymer pressure sensor has been developed for service in a portable 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.<<ETX>>


Journal of the Acoustical Society of America | 1978

Theoretical response of condenser microphones

Allan J. Zuckerwar

Modifications to prior theory yield expressions for the frequency response and equivalent lumped elements of a condenser microphone in terms of its fundamental geometrical and material properties. Results of the analysis show excellent agreement with experimental data taken on B&K pressure microphone types 4134 and 4146.


Journal of the Acoustical Society of America | 1985

Ultrasonic depth gauge for liquids under high pressure

Allan J. Zuckerwar; David S. Mazel

An ultrasonic depth gauge 20 for liquids under high pressure is comprised of a transducer assembly 21 and a supporting electronics unit 22. The transducer assembly is mounted into the bottom wall of a storage vessel 12 with its resonating surface directly exposed to the highly pressurized liquid 13 in the vessel. The transducer assembly consists of a conventional transducer element 38 rigidly bonded to the inside wall of a bored out conventional high-pressure plug 30 thereby forming a composite resonator 50. The element and the plug wall resonate as one upon electrical excitation of the element while the transducer element is completely shielded from any exposure to the liquid under high pressure. The composite resonator sends a vibration up to the surface of the liquid where it is reflected back to the composite resonator. The supporting electronics unit measures the vibration round-trip transit time which is proportional to the depth 15 of the liquid.


Journal of the Acoustical Society of America | 1979

High temperature microphone system

Allan J. Zuckerwar

Apparatus for measuring pressure fluctuations in air or other gases in an area of elevated temperature. A condenser microphone is located in the area of elevated temperature and electronics for processing changes in the microphone capacitance is located outside the area and connected to the microphone by means of a high-temperature cable assembly. The microphone includes apparatus for decreasing the undesirable change in microphone sensitivity at high temperatures. The high-temperature cable assembly operates as a half-wavelength transmission line in an AM carrier system and maintains a large temperature gradient between the two ends of the cable assembly. The processing electronics utilizes a voltage controlled oscillator for automatic tuning thereby increasing the sensitivity of the measuring apparatus.


Journal of the Acoustical Society of America | 1992

Theoretical and experimental study of a fiber optic microphone

Andong Hu; Frank W. Cuomo; Allan J. Zuckerwar

Modifications to condenser microphone theory yield new expressions for the membrane deflections at its center, which provide the basic theory for the fiber optic microphone. The theoretical analysis for the membrane amplitude and the phase response of the fiber optic microphone is given in detail in terms of its basic geometrical quantities. A relevant extension to the original concepts of the optical microphone includes the addition of a backplate with holes similar in design to present condenser microphone technology. This approach generates improved damping characteristics and extended frequency response that were not previously considered. The construction and testing of the improved optical fiber microphone provide experimental data that are in good agreement with the theoretical analysis.


Journal of the Acoustical Society of America | 2006

Calibration of the pressure sensitivity of microphones by a free-field method at frequencies up to 80 kHz

Allan J. Zuckerwar; Gregory C. Herring; Brian R. Elbing

A free-field (FF) substitution method for calibrating the pressure sensitivity of microphones at frequencies up to 80 kHz is demonstrated with both grazing and normal-incidence geometries. The substitution-based method, as opposed to a simultaneous method, avoids problems associated with the nonuniformity of the sound field and, as applied here, uses a 1/4-in. air-condenser pressure microphone as a known reference. Best results were obtained with a centrifugal fan, which is used as a random, broadband sound source. A broadband source minimizes reflection-related interferences that can plague FF measurements. Calibrations were performed on 1/4-in. FF air-condenser, electret, and microelectromechanical systems (MEMS) microphones in an anechoic chamber. The uncertainty of this FF method is estimated by comparing the pressure sensitivity of an air-condenser FF microphone, as derived from the FF measurement, with that of an electrostatic actuator calibration. The root-mean-square difference is found to be +/- 0.3 dB over the range 1-80 kHz, and the combined standard uncertainty of the FF method, including other significant contributions, is +/- 0.41 dB.


Journal of the Acoustical Society of America | 2005

Compact nonporous windscreen for infrasonic measurements

Qamar A. Shams; Allan J. Zuckerwar; Bradley S. Sealey

Infrasonic windscreens, designed for service at frequencies below 20Hz, were fabricated from a variety of materials having a low acoustic impedance, and tested against four specifications (the first three in a small wind tunnel): (1) wind-generated noise reduction (“insertion loss”) at a free-stream wind speed of 9.3m∕s, (2) transmission of low-frequency sound from a known source (subwoofer), (3) spectrum of sound generated from trailing vortices (aeolian tones), and (4) water absorption (to determine suitability for all-weather service). The operating principle is based on the high penetrating capability of infrasound through solid barriers. Windscreen materials included three woods (pine, cedar, and balsa), closed-cell polyurethane foam, and Space Shuttle tile material. The windscreen inside diameter ranged from 0.0254to0.1016m (1to4in.), and wall thickness from 0.003175to0.01905m (18to34in.). A windscreen made of closed-cell polyurethane foam revealed a wind noise reduction of 10–20dB from 0.7to25Hz, t...


Journal of the Acoustical Society of America | 1985

Low-frequency absorption of sound in air

Allan J. Zuckerwar; Roger W. Meredith

An extensive series of sound absorption measurements were taken in air over a range of frequencies from 10–2500 Hz, of temperature from 10°–50 °C, and of relative humidity from 0.3%–92%, all at a pressure of 1 atm. The N2 and O2 vibrational absorption components were extracted from a relatively large background absorption by means of a differential technique using a background gas, 89.5% N2–10.5% Ar, which matches the sound speed of air but has no molecular absorption over the range of experimental frequencies. The measurements reveal: (1) The humidity dependence of the relaxation frequency of N2 in air exceeds that in binary N2–H2O mixtures, possibly because the vibrational modes of CO2 provide a competing relaxation path for V–V exchange between N2 and H2O molecules; (2) the temperature dependence of the relaxation frequency of humid N2 is nearly the same in air as in binary mixtures; and (3) at very low humidities the relaxation frequency of O2 appears to approach a limiting value much lower than that ...


Physics of Fluids | 2006

Variational approach to the volume viscosity of fluids

Allan J. Zuckerwar; Robert L. Ash

The variational principle of Hamilton is applied to develop an analytical formulation to describe the volume viscosity in fluids. The procedure described here differs from those used in the past in that a dissipative process is represented by the chemical affinity and progress variable (sometimes called “order parameter”) of a reacting species. These state variables appear in the variational integral in two places: first, in the expression for the internal energy, and second, in a subsidiary condition accounting for the conservation of the reacting species. As a result of the variational procedure, two dissipative terms appear in the Navier-Stokes equation. The first is the traditional volume viscosity term, proportional to the dilatational component of velocity; the second term is proportional to the material time derivative of the pressure gradient. Values of the respective volume viscosity coefficients are determined by applying the resulting volume-viscous Navier-Stokes equation to the case of acousti...


Journal of the Acoustical Society of America | 1995

High‐temperature fiber‐optic lever microphone

Allan J. Zuckerwar; Frank W. Cuomo; Trung D. Nguyen; Stephen A. Rizzi; Sherman A. Clevenson

The design and construction of a fiber‐optic lever microphone, capable of operating continuously at temperatures up to 538 °C (1000 °F), are described. The design is based on the theoretical sensitivities of each of the microphone system components, namely, a cartridge containing a stretched membrane, an optical fiber probe, and an optoelectronic amplifier. Laboratory calibrations include the pistonphone sensitivity and harmonic distortion at ambient temperature, and frequency response, background noise, and optical power transmission at both ambient and elevated temperatures. A field test in the Thermal Acoustic Fatigue Apparatus at Langley Research Center, in which the microphone was subjected to overall sound‐pressure levels in the range of 130–160 dB and at temperatures from ambient to 538 °C, revealed good agreement with a standard probe microphone.

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Frank W. Cuomo

University of Rhode Island

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Andong Hu

University of Rhode Island

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