Acoustic vibration sensor and sensing system

Claim 2

An acoustic vibration sensor comprising: A. a first single mode optical fiber extending to the sensing region, B. a second single mode optical fiber extending to said sensing region, C. means at said sensing region coupling optical energy from said first fiber to said second fiber including a first partially reflecting discontinuity which reflects optical energy in said first fiber backward from the sensing region, D. means at said sensing region coupling optical energy from said second fiber to said first fiber including a second partially reflecting discontinuity which reflects optical energy in said second fiber backward from the sensing region, and E. means for modulating the length of said optical coupling paths between fibers in response to the acoustic vibrations in said sensing means.

Claim 3

A sensor as set forth in claim 1 wherein said first partially reflecting discontinuity is the end of said first fiber at the sensing region, said second partially reflecting discontinuity is the end of said second fiber at the sensing region and the optical path coupling said fiber ends is said modulating path.

Claim 4

A sensor as set forth in claim 2 wherein said coupling path length modulating means comprises: A. means for supporting one fiber with freedom to be displaced along the optical path to the other fiber, and B. means for coupling acoustic energy to said support to cause said displacement in response to incident acoustic energy.

Claim 5

A sensor as set forth in claim 2 wherein said coupling path length modulating means comprises: A. means for supporting each fiber with freedom to be displaced along the optical path to the other fiber, and B. means for coupling acoustic energy to said supports to cause said displacements in response to incident acoustic energy.

Claim 6

A sensor as set forth in claim 4 wherein said fibers are coaxially supported with abutting fiber ends, each support comprising a resilient diaphragm allowing mutual displacement of the fiber ends in response to incident acoustic energy.

Claim 7

A sensor as set forth in claim 1 wherein the optical coupling paths between fibers is a coiled single mode optical fiber subject to said acoustic vibrations.

Claim 8

A sensor as set forth in claim 7 wherein said first partially reflecting discontinuity is an end of said first fiber optically coupled to one end of said coiled fiber, and said second partially reflecting discontinuity is an end of said second fiber optically coupled to the other end of said coiled fiber.

Claim 9

A hydrophone system comprising: A. a sensor as set forth in claim 1, B. a coherent optical light source producing a first beam having an optical frequency (f o ), C. an optical modulator for producing a second beam having an optical frequency (f o +f w ), D. a first beamsplitting means for coupling energy (f o ) from said light source in a first sense through said first beamsplitting means into said first fiber for application to said sensor, the energy out of said second fiber, which includes energy (f o +f w ) reflected back from said second partially reflecting discontinuity and energy (f o ) coupled from said first fiber, impinging in an opposite sense on said beamsplitting means, E. a first photodetector responding to energy at the difference frequency (f w ) impinging in said opposite sense on said first beamsplitting means, F. a second photodetector responding to energy at the difference frequency (f w ) impinging in said opposite sense on said second beamsplitting means, and G. means for determining the instantaneous phase or frequency difference between the output of said respective photodetectors to obtain an acoustic measurement primarily dependent on changes in the optical path length occurring between said partially reflecting discontinuities at said sensor.

Claim 10

A hydrophone system comprising: A. a sensor as set forth in claim 1, B. a coherent optical light source having an optical frequency (f o ), C. a first optical modulator coupled to said coherent light source for producing a first beam having an optical frequency (f o +f 1 ), D. a second optical modulator coupled to said coherent light source for producing a second beam having an optical frequency (f o +f 2 ), E. A first beamsplitting means for coupling energy at frequency (f o +f 1 ) from said first modulator in a first sense through said first beamsplitting means into said first fiber, which includes energy at frequency (f o +f 1 ) reflected back from said partially reflecting discontinuity and energy at frequency (f o +f 2 ) coupled from said second fiber, impinging in an opposite sense on said first beamsplitting means, F. a second beamsplitting means for coupling energy at frequency (f o +f 2 ) from said second modulator in a first sense through said second beamsplitting means to said second fiber for application to said sensor, the energy out of said second fiber, which includes energy at frequency (f o +f 2 ) reflected back from said second partially reflecting discontinuity and energy at frequency (f o +f 1 ) coupled from said first fiber, impinging in an opposite sense on said beamsplitting means, G. a first photodetector responding to energy at the difference frequency (f 1 -f 2 ) impinging in said opposite sense on said first beamsplitting means, H. a second photodetector responding to energy at the difference frequency (f 1 -f 2 ) impinging in said opposite sense on said second beamsplitting means, and I. means for determining the instantaneous phase or frequency difference between the output of said respective photodetectors to obtain an acoustic measurement primarily dependent on changes in the optical path length occurring between said partially reflecting discontinuities at said sensor.

Claim 11

A hydrophone system comprising: A. a sensor as set forth in claim 1, B. a coherent optical light source producing a first beam having an optical frequency (f o ), C. a first and a second four port directional coupling light modulator in which diagonal pairs or ports (a, b; c, d) have maximum light coupling means when acoustic energy is not present; in which two adjacent pairs of ports (a, d; c, b) have partial light coupling when acoustic energy is present, the coupling producing acoustic light modulation, and in which two adjacent pairs of ports (a, c; b, d) are uncoupled. D. means for coupling optical energy from said light source to one port (a) of each modulator, E. means coupling the first fiber of said sensor to the port (d) of said first modulator at which acoustically Bragg modulated light appears; means coupling the second fiber of said sensor to the port (d) of said second modulator at which acoustically Bragg modulated light appears, F. means coupling a first photodetector to the port (c) diagonal to said first fiber connected port (d) of said first modulator for coupling energy from said first fiber thereto; means coupling a second photodetector to the port (c) diagonal to said second fiber connected port (d) of said second modulator for coupling energy from said second fiber thereto. G. means for determining the instantaneous phase or frequency difference between the output of said respective photodetectors to obtain an acoustic measurement primarily dependent on changes in the optical path length occurring between said partially reflecting discontinuities at said sensor, and H. means for dissipating the optical energy out of port (b) of said first and second modulators so that no energy is reflected back into port (b) of said first and second modulators.