1974
DOI: 10.1109/proc.1974.9483
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Practical surface acoustic wave devices

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Cited by 54 publications
(6 citation statements)
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“…Subscripts 'a' and 'b' in Eqs. (21) and (23) refer to the sensors design previously described, and denoted as 'sensor ðaÞ' and 'sensor ðbÞ.' One note, is the fact that while the practical implementation of sensor ðaÞ is not feasible, the evaluation of its performance through the considered approach and Eq.…”
Section: B Sampling Of Measurement Grid and Evaluation Of The Spiralmentioning
confidence: 99%
See 1 more Smart Citation
“…Subscripts 'a' and 'b' in Eqs. (21) and (23) refer to the sensors design previously described, and denoted as 'sensor ðaÞ' and 'sensor ðbÞ.' One note, is the fact that while the practical implementation of sensor ðaÞ is not feasible, the evaluation of its performance through the considered approach and Eq.…”
Section: B Sampling Of Measurement Grid and Evaluation Of The Spiralmentioning
confidence: 99%
“…This basic idea has been widely exploited for the design of interdigitated transducers (IDTs) used as part of surface acoustic wave (SAW) devices. 21 While linear IDT configurations are commonly employed for selective generation and detection of surface waves, other alternative configuration, such as the slanted IDT described for example in Ref. 22, and the annular IDTs proposed in Ref.…”
mentioning
confidence: 99%
“…For curved surfaces, however, the generation of surface waves with these methods is less practical. An interdigital transduction (IDT) method commonly used in telecommunication filtering devices was adapted for the current application [3][4][5] . Based on the same transduction principles, a narrow band IDT sensor with a resonance frequency in the range of 3 MHz was designed and fabricated.…”
Section: Idt Sensorsmentioning
confidence: 99%
“…The observed changes wrn qualitatively and jdantieatlvely veil characterized In t*rnw of the tima changing tim^ei'ature of the vibratin;; quartz and its effect on frequency. Tliercnl transient inJuccd frequency chancer, in AT cut resonator* were observed as early fo 1939 5 And described empirically as a function of the tine changing *1hts work was supported by the U.S. Oopartwent of Energy, ambient.'' Holland's' work on thermal gradi ent effects in thickness 3hear resonators led to the TTC cut, which is approximately rquivalent to EcrNiase's stress compou-.Jted, SC, cut.° Holland's calculations d(;al with thermal gradi ents in the chicVncns direction while, in the present work, the thermal modelling of the reso nator structure ia concerned with radial heat flow and relates the inst.nnrar.oou9 frequency change linearly to the rr.te of change of tem perature -t the oscillating boundary.…”
Section: Introductionmentioning
confidence: 99%