D. S. Ballantine Jr., Robert M. White, S. J. Martin, Antonio's Acoustic Wave Sensors: Theory, Design, and Physico-Chemical PDF

By D. S. Ballantine Jr., Robert M. White, S. J. Martin, Antonio J. Ricco, E. T. Zellers, G. C. Frye, H. Wohltjen

ISBN-10: 0120774607

ISBN-13: 9780120774609

Written by way of an interdisciplinary workforce 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 functions. as a result of the inherent interdisciplinary purposes of those units, this ebook can be worthy for the chemist and biochemist drawn to the use and improvement of those sensors; engineer taken with their layout and development; the chemical engineer and the biotechnologist attracted to utilizing them for procedure tracking and keep an eye on; and the sensor group at huge.

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Extra resources for Acoustic Wave Sensors: Theory, Design, and Physico-Chemical Applications

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C Q. 00 Electrical admittance vs frequency for an unloaded TSM resonator. (Reprinted with permission. See Ref. [9]. ) 50 3. Acoustic Wave Sensors and Responses proximates the electrical characteristics of the TSM resonator for excitation frequencies near resonance [9,11]. 5) can be used to describe the electrical response of the perturbed device. 5b, is most convenient to use. 7. This model contains the elements Co*, LI, Cl, and RI corresponding to the unperturbed resonator. 7a. 20) Vx lY=O where Txy is the sinusoidal steady-state shear stress (force per area in the xdirection on a y-normal plane) imposed on the contacting medium by the resonator, and Vx is the resulting x-directed surface shear particle velocity.

34 were derived for one-sided liquid contact; for two-sided, L2 and R2 are doubled. The motional inductance L2. 23 in agreement with the prediction of Kanazawa and Gordon [18]: ~f,---- L2fs _ 2LI f3/2 . 35) " The motional resistance, R2, represents power radiated into the contacting liquid by the oscillating device surface. " This motional resistance leads to resonance damping. Muramatsu et al. [19] and Beck et al.

N = 1, 3, 5 . . [4]. 65 g/cm 3. 3 Transit of a shear wave, illustrating the resonant condition. 06 MHz. Having derived the condition for crystal resonance allows the displacement profile at resonance to be calculated. When the crystal is operated in air or vacuum, the crystal faces experience no external restoring force and arc considered to be stress-free boundaries; this implies that Oux/Oy = 0 at the upper and lower crystal faces. 4) where uxo is the surface displacement amplitude and kN = NTr/hs.

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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


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