By D. S. Ballantine Jr., Robert M. White, S. J. Martin, Antonio J. Ricco, E. T. Zellers, G. C. Frye, H. Wohltjen
Written via an interdisciplinary crew of specialists from either and academia, Acoustic Wave Sensors presents an in-depth examine the present nation of acoustic wave units and the scape in their use in chemical, biochemical, and actual measurements, in addition to in engineering purposes. as a result of the inherent interdisciplinary functions of those units, this booklet might be helpful for the chemist and biochemist drawn to the use and improvement of those sensors; engineer considering their layout and development; the chemical engineer and the biotechnologist drawn to utilizing them for strategy tracking and keep watch over; and the sensor neighborhood at huge.
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Additional resources for Acoustic Wave Sensors: Theory, Design, and Physico-Chemical Applications
The figure indicates the series (fs) and parallel (fp) resonances, where the admittance phase angle ( / Y ) is zero and device reactance is zero. The admittance magnitude [Y[ is near maximum at fs and near minimum at fp. 14) using best-fit values of Co, Cp, fs, and Rl. , the impedance or admittance. By using a continuum model that describes the coupled mechanical displacement and electrical potential, the electrical characteristics can be related to the properties of the perturbing mass or liquid layer [I0].
4 3. Acoustic Wave Sensors and Responses ELECTRICAL CHARACTERISTICS AN IDEAL MASS LAYER OF TSM RESONATOR WITH An ideal mass layer is assumed to have an infinitesimal thickness, yet contribute a finite areal mass density to the device surface. 1, we noted that this criterion holds as long as the acoustic phase shift across the film ~ is small compared with It. The equivalent-circuit model for the mass-loaded resonator can be determined from the surface mechanical impedance Zs contributed by a surface perturbation.
48 represents a fundamental relation between wave velocity and energy density for a system excited at a given frequency: the fractional change in wave velocity is equal to the negative of the fractional change in wave energy density. This may seem reasonable if one considers that in a system excited at a given frequency, the wavelength adjusts so that the peak kinetic energy equals the peak potential energy of the wave. The result is that changes of the medium that affect the wave energy density will cause changes of the wave velocity.
Acoustic Wave Sensors: Theory, Design, and Physico-Chemical Applications by D. S. Ballantine Jr., Robert M. White, S. J. Martin, Antonio J. Ricco, E. T. Zellers, G. C. Frye, H. Wohltjen