Fig. 3. Measurement set-up for temperature dependent material properties of the acoustic sensor materials.
Fig. 4. Admittance curves of PZT hydrophone sphere with temperature change: -2 ℃, 15 ℃, 35 ℃.
Fig. 5. Finite element model: (a) low⋅mid frequency sensor, (b) high frequency sensor.
Fig. 6. Simulated RVS curves with respect to the temperature dependent material properties of polyurethane: (a) low⋅mid frequency sensor, (b) high frequency sensor.
Fig. 7. Simulated RVS curves with respect to the temperature dependent material properties of vulkollan (a) low⋅mid frequency sensor, (b) high frequency sensor.
Fig. 8. Experimental set-ups for temperature dependent RVS measurement of acoustic sensors.
Fig. 9. Transmission characteristics of the acoustic chamber: (a) free-field rvs and in-chamber rvs of low·mid frequency sensors (b) free-field RVS and In-chamber RVS of high frequency sensors (c) theoretical and measured transmission loss of the acoustic chamber.
Fig. 10. Measured RVS curves with respect to temperature change: (a) low·mid frequency sensors (b) high frequency sensors.
Fig. 1. (a) Global sea surface temperature map in September, 2015 and (b) sea depth temperature profile.[2]
Fig. 2. Configuration of the acoustic sensors: (a) low·mid frequency acoustic sensor (b) high frequency acoustic sensor.
Table 1. Materials used in the acoustic sensors and their acoustic properties.[10]
Table 2. Piezoelectric coefficient, dielectric constant, and sensitivity of the spherical hydrophone with temperature change: -2 ℃, 15 ℃, 35 ℃.
Table 3. Sound speed of polyurethane and vulkollan with temperature change: -2 ℃, 15 ℃, 35 ℃.
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