A fiber-optic hydrophone with a cylindrical Helmholtz resonator

A passive homodyne Michelson interferometric fiber-optic hydrophone with a single-hole cylindrical Helmholtz resonator has been manufactured. To validate the theoretical results that the fluid coefficient of viscosity has great influence on the maximum sensitivity at the resonant frequency, the acoustic sensitivity frequency response of the fiber-optic hydrophone has been measured in a standing-wave tank filled with castor oil. The viscosity coefficient of castor oil will change with the variation of the temperature. Experimental Results show that the fiber-optic hydrophone frequency responses of different temperature have identical form except that the maximum sensitivities are different. The acoustic sensitivities of low frequency are about -159dB re 1rad/μPa. While the maximum sensitivities near the measured resonant frequency of 800Hz go down with the fall of the temperature, i.e. with the increase of the viscosity coefficient, which is agree with the theoretical conclusions. This fiber-optic hydrophone is a prototype device for a class of sensors that used to eliminate aliasing in the future sonar systems.

[1]  J. Flanagan Acoustic fitters to aid digital voice , 1979, The Bell System Technical Journal.

[2]  G. Stewart,et al.  Stable single-mode operation of a narrow-linewidth, linearly polarized, erbium-fiber ring laser using a saturable absorber , 2006, Journal of Lightwave Technology.

[3]  Hu Yongming Research on the transmission characteristics of underwater perforated-panel structure , 2008 .

[4]  Yoshimura,et al.  Development of an optical fiber hydrophone with fiber Bragg grating , 2000, Ultrasonics.

[5]  H. Chan,et al.  Ultrasonic hydrophone based on distributed Bragg reflector fiber laser , 2005, IEEE Photonics Technology Letters.

[6]  A. Bautista,et al.  Large-scale remotely pumped and interrogated fiber-optic interferometric sensor array , 2003, IEEE Photonics Technology Letters.

[7]  Koji Dobashi,et al.  Design study of an optical hydrophone array , 1993, Optics & Photonics.

[8]  V. Wilkens,et al.  Frequency response of fiber-optic multilayer hydrophones: experimental investigation and finite element simulation , 2002, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[9]  Michael A. Davis,et al.  Fiber grating sensors , 1997 .

[10]  Geoffrey A. Cranch,et al.  Large-scale remotely interrogated arrays of fiber-optic interferometric sensors for underwater acoustic applications , 2003 .

[11]  Michel J. F. Digonnet,et al.  Acoustic fiber sensor arrays , 2004, European Workshop on Optical Fibre Sensors.

[12]  Thomas G. Giallorenzi,et al.  Optical fiber sensor technology , 1982, 1985 International Electron Devices Meeting.

[13]  J. L. Flanagan,et al.  Direct digital-to-analog conversion of acoustic signals , 1980, The Bell System Technical Journal.

[14]  Michel J. F. Digonnet,et al.  Pickup suppression in sagnac-based fiber-optic acoustic sensor array , 2006 .

[15]  HU Yong-ming A J_0-J_1 Method for Measurement of Dynamic Phase Changes in an Interferometric Fiber Sensor , 2007 .

[16]  George Stewart,et al.  Development of a 32-element fiber optic hydrophone system , 2004, SPIE Optics East.

[17]  D.J.W. Hardie,et al.  Review of numerical methods for predicting sonar array performances , 1996 .

[18]  Zefeng Wang,et al.  A fiber-optic hydrophone with an acoustic filter , 2007, SPIE/COS Photonics Asia.

[19]  J. Carroll,et al.  A fiber-optic hydrophone with a mechanical anti-aliasing filter , 1986 .

[20]  A. Kersey,et al.  Bragg grating-based laser sensors systems with interferometric interrogation and wavelength division multiplexing , 1995 .