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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 65 (1989), S. 35-40 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An analysis of the in-plane acceleration sensitivity of grooved ST- and SST-cut-quartz surface-wave resonators rigidly supported along the edges is performed. The biasing deformation fields are obtained using a new variational approximation procedure which is very accurate, computationally efficient, and convenient to use. The calculated extensional biasing states are employed in an existing perturbation equation along with the proper continuous representation of the acoustic surface-wave mode shape for arrays of reflecting grooves to calculate the in-plane acceleration sensitivity for both cuts. The calculations reveal that the ST cut is slightly less sensitive than the SST cut and that both are a few parts in 1011 per g.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 64 (1988), S. 4334-4341 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An analysis of the normal acceleration sensitivity of grooved ST-cut quartz surface wave resonators supported along the edges is performed. Both the simply supported and rigidly supported cases are treated. The variational principle with all natural conditions for anisotropic flexure, which is required for the new approximation procedure used in the calculation of the flexural biasing state for the case of rigid supports, is presented. The flexural biasing states are employed in an existing perturbation equation along with the proper continuous representation of the acoustic surface wave mode shape for arrays of reflecting grooves to calculate the normal acceleration sensitivity. It is shown that by appropriate selection of the planar aspect ratio of an ST-cut quartz substrate the normal acceleration sensitivity can be made to vanish.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 68 (1990), S. 5009-5015 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An analysis of PZT-7A plates driven into thickness-extensional trapped energy vibrations by the application of a voltage to strip electrodes and radiating into an adjacent fluid is performed. All previous treatments of thickness-extensional trapped energy modes in piezoelectric plates have ignored the radiation into the surrounding medium and, hence, have been for resonators rather than transducers. The solution consists of a sum of a driven thickness solution and the pertinent plate eigensolutions for shorted electrodes in the electroded region and for zero surface charge in the unelectroded region, including in each instance the radiation into the adjacent fluid. Since the sum of the solutions in each region satisfies the differential equations and boundary conditions on the major surfaces including the fluid loading exactly, the substitution into the appropriate variational principle of linear piezoelectricity yields integral conditions across the thickness of the plate at the edge of the electrodes. The resulting system of inhomogeneous linear algebraic equations yields the response from very low frequency to slightly above the first thickness-extensional frequency of the unelectroded plate.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 68 (1990), S. 4998-5008 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An analysis of PZT-7A plates driven into thickness-extensional trapped energy vibrations by the application of a voltage to strip electrodes is performed. The plate waves in the unelectroded region that carry energy away from the trapped mode are included in the treatment. The solution consists of a sum of the driven thickness solution and the pertinent plate eigensolutions for shorted electrodes in the electroded region and for zero surface charge in the unelectroded region. Since the sum of the solutions in each region satisfies the differential equations and boundary conditions on the major surfaces exactly, the substitution into the appropriate variational principle of linear piezoelectricity yields integral conditions across the thickness of the plate at the edge of the electrodes. The resulting system of inhomogeneous linear algebraic equations yields the response from very low frequency to slightly above the first thickness-extensional frequency of the unelectroded plate.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 67 (1990), S. 2554-2566 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An analysis of the in-plane acceleration sensitivity of ST-cut quartz surface-wave resonators with the substrate extending beyond interior rectangular supports is performed. In the treatment the variational principle with all natural conditions is extended in such a way as to permit interior surfaces of discontinuity with spring supports at which the approximating solution functions need not satisfy the constraint-type conditions. This extension is required for the approximation procedure used in the calculation of the biasing state. The resulting extensional biasing state is employed in an existing perturbation integral along with the proper continuous representation of the acoustic-surface-wave mode shape to calculate the in-plane acceleration sensitivity. The calculated results indicate how to select the distances between the supports so as to minimize the in-plane acceleration sensitivity for a given surface-wave resonator.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2238-2249 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The composite resonator consists of a uniform thin layer etched in a small well-defined region of a semiconductor wafer to form a diaphragm, upon which is deposited a thin piezoelectric film along with the electrodes to form a resonant region directly on the wafer. Although the composite resonator, which operates in an essentially thickness-extensional mode, can be constructed to employ energy trapping, almost all existing experimental work in the literature is for the case when trapping is not present. All previous analytical work expressly ignores radiation into the bulk semiconductor except one treatment, which unrealistically ignores the junction between the etched diaphragm and the bulk semiconductor. In this work an analysis of the composite resonator driven into essentially thickness-extensional vibrations by the application of a voltage to strip electrodes is performed. The analysis includes all radiating plate waves in the thick portion of the semiconductor. The solution consists of a sum of terms satisfying all differential equations and boundary conditions on major surfaces exactly and uses the appropriate variational principle of linear piezoelectricity to satisfy the remaining conditions approximately. For the case of the aluminum–nitride film on gallium arsenide the Q is calculated for both the configuration in which the film ends at the edges of the electrodes and in which it continues to the edges of the etched diaphragm when trapping is not present and for the latter configuration when trapping is present. The calculations show that when trapping is not present the Q is a very rapidly varying function of the ratio of the composite resonator thickness to the wafer thickness and that the range of variation is very large, i.e., between one and two orders of magnitude. The calculations also reveal that when trapping is present the Q is always much larger and its range of variation much smaller than when trapping is not present.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 62 (1987), S. 1154-1161 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A variational analysis of the reflection of surface waves by arrays of reflecting grooves is presented. The variational condition results in a system of linear algebraic equations relating the amplitudes of the waves on both sides of the edge of a groove. The influence of transverse moding, which is a result of the finite lateral dimension of the grooves, is included in the treatment, but scattering into bulk waves is not considered. Application of the linear algebraic equations across both edges of a typical groove results in a system of transmission equations, which constitutes a linear difference system for the periodic array. A closed-form continuous representation of the mode shape along the transmission path is obtained from the solution of the system of linear difference equations for the periodic array. The continuous representation is particularly convenient for use in the evaluation of perturbation integrals that arise in the calculation of the change in frequency of surface-wave resonators due to biasing states and for many other purposes. When the resonant surface-wave mode has been found, the reduced resonant frequency and phase velocity are obtained by means of a perturbation procedure. Calculated results are presented for grooved arrays on ST-cut quartz.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 62 (1987), S. 4045-4054 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In a variational analysis of the vibrations of the piezoelectric thin film on semiconductor composite resonator it was shown that the quality factor (Q) due to radiation into the semiconductor wafer is a sharply varying function of the ratio of the thickness of the resonator to that of the film if trapping is not present, but not if trapping is present. The treatment is very cumbersome to use and is restricted to the case of strip electrodes and diaphragms. In this work a perturbation procedure for the calculation of the Q due to radiation into the wafer is presented, which is considerably less cumbersome to use than the earlier treatment and is not restricted to the case of strip electrodes and diaphragms. The resonant mode of interest is determined from an equation for transversely varying thickness modes in composite resonators and simple approximate but accurate conditions at the edges of the diaphragm, from which the radiation into the wafer is obtained using a variational approximation procedure. The resonant mode and resulting radiation field are employed in a perturbation integral to calculate the Q. For the case of strip electrodes and diaphragms the calculated results are shown to be in good agreement with the earlier more cumbersome calculations. In addition the perturbation calculations are performed for the case of rectangular electrodes and diaphragms.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 67 (1990), S. 60-67 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An analysis of the normal acceleration sensitivity of contoured AT- and SC-cut quartz crystal resonators rigidly supported along rectangular edges is performed. The variational principle with all natural conditions for anisotropic static flexure is used in the calculation of the flexural biasing state. However, in this work the biasing shearing stresses with quadratic variation across the thickness of the plate are obtained a posteriori from the flexural solution in the conventional manner. The accompanying quadratically varying biasing shearing strains, which are very important in this work, are obtained from the constitutive equations along with all other quadratically varying strains resulting from the anisotropy. The calculated biasing deformation fields are employed in an existing perturbation equation along with the mode shapes of the contoured resonators to calculate the normal acceleration sensitivities. It is shown that the normal acceleration sensitivity vanishes for many cases and is less than a few parts in 1013 for all cases considered.
    Type of Medium: Electronic Resource
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