1999
DOI: 10.1121/1.427091
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Porous piezoelectric ceramic hydrophone

Abstract: The construction and evaluation of a hydrophone based on porous piezoelectric ceramics with high d h g h figure of merit ͑FOM͒ is described. It has been shown that, in order to improve the hydrophone signal-to-noise ratio, a piezoelectric material with a high FOM should be employed. A porous piezoelectric material has been prepared by mixing calcined lead zirconate titanate ͑PZT͒ powder with fine particle starch powder. Square plate samples have been cold pressed from this material, which were then heated to e… Show more

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Cited by 58 publications
(56 citation statements)
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“…Another important application is underwater acoustics for which hydrostatic properties of the porous piezoelectric material are the key parameters [39][40][41][42]. An active transducer sensitivity can be characterised by the hydrostatic strain coefficient d h defined by :…”
Section: Modellingmentioning
confidence: 99%
“…Another important application is underwater acoustics for which hydrostatic properties of the porous piezoelectric material are the key parameters [39][40][41][42]. An active transducer sensitivity can be characterised by the hydrostatic strain coefficient d h defined by :…”
Section: Modellingmentioning
confidence: 99%
“…It is well-known that the porous piezoceramics have enhanced properties with respect to dense ceramics for applications like some types of low frequency hydrophones and sensors, due to their better hydrostatic figures of merit (d h g h ) [10][11][12]. However, the porous ceramics characteristics, namely, the low mechanical quality factors and electromechanical coupling coefficients, limit the application of the 1987 IEEE [2] and CENELEC [3] Standard measurement methods in their characterization.…”
Section: Introductionmentioning
confidence: 99%
“…The behaviour of coupling or decoupling of the algebraic system remains the same in pure piezoelectric and PPM cases. The mutual angles θ 13 , θ 14 and θ 34 , corresponding to the pure piezoelectric case, have been computed for all the above-mentioned crystal classes and planes of propagation. Unlike the PPMs all three waves are found to be mutually orthogonal in all the crystal classes and planes of propagation (figure 14).…”
Section: Wave Propagation In the X 1 -X 2 Planementioning
confidence: 99%