Fiber optic sensor with enhanced immunity to random environmental perturbations

• US 4,442,350 A
• Filed: 08/17/1981
• Issued: 04/10/1984
• Est. Priority Date: 08/17/1981
• Status: Expired due to Fees

• Current Assignee: The United States of America As Represented By The Secretary of Agriculture
• Original Assignee: the united states of america as represented by the secretary of the navy
• Inventors: Rashleigh, Scott C.
• Primary Examiner(s): Nelms, David C.
• Assistant Examiner(s): Westin, Edward P.
• Application Number:
  US06/293,589
• Time in Patent Office: 967 Days
• Field of Search: 250/227, 250/231 R, 356/33, 356/73.1, 350/375, 350/96.29, 350/96.3, 324/96, 324/244, 73/655-657
• US Class Current: 250/227.17
• CPC Class Codes: G01H 9/004 using fibre optic sensors light guides per se G02B6/00, acousto-optical devices specially adapted for gating or modulating in optical wave guides G02F1/125
• CPC Class Codes: G01P 15/093 by photoelectric pick-up
• CPC Class Codes: G01R 33/0327 with application of magnetostriction

Abstract

A sensor is provided for sensing or detecting the presence of an environmental field condition such as acceleration, temperature change, magnetic or acoustic fields. The field is sensed by interference between two mutually orthogonal polarized eigenmodes in a single monomode optical fiber which may be disposed either linearly or wound on a mandrel made of compliant material for sensing an acoustic field, or made of magnetostrictive material for sensing a magnetic field. Polarized light propagated through the optical fiber is detected at its outlet independent of environmentally induced low frequency variations whereby the sensor may be maintained at quadrature and maximum sensitivity.

Claims

1. A method of sensing a field condition with minimum disturbance from low frequency environmentally induced perturbations comprising the steps of:

propagating polarized light through an optical fiber made birefringent to have two orthogonally disposed modes oriented respectively along fast and slow axes;

allowing a field condition to stress a length of the optical fiber in axes directions for changing its birefringence;

splitting one portion of the light emanating from the optical fiber into first and second components of linearly polarized light;

phase shifting another portion of the light emanating from the optical fiber by 90° and

splitting it into a third component of left circularly polarized light and a fourth component of right circularly polarized light;

monitoring the intensities of the first and second linearly polarized orthogonal light components to produce respective first and second electrical signals and combining the first and second electrical signals to filter out low frequency perturbations to provide a third electrical signal proportional to the field condition induced stresses in the optical fiber;

at the same time monitoring the intensities of the third and fourth circularly polarized light components to produce respective fourth and fifth electrical signals and combining the fourth and fifth electrical signals to filter out low frequency perturbations to provide a sixth electrical signal proportional to the field condition induced stresses in the optical fiber, and which the sixth electrical signal is shifted in phase by 90°

relative to the third electrical signal; and

,

combining the third and sixth electrical signals to produce an output electrical signal which is independent of low frequency environmentally induced perturbations.

2. The method according to claim 1 further defined by the step of tension coiling the optical fiber to a small diameter to make it birefringent.

3. The method according to claim 1 or 2, wherein:

said step of combining said first and second electrical signals to provide said third electrical signal comprises the step of dividing the difference between said first and second electrical signals by the sum of said first and second electrical signals;

said step of combining said fourth and fifth electrical signals to provide said sixth electrical signal comprises the step of dividing the difference between said fourth and fifth electrical signals by the sum of said fourth and fifth electrical signals; and

said step of combining said third and sixth electrical signals to produce said output electrical signal comprises the step of taking the square root of the sum of the squares of said third and sixth electrical signals.

4. The method of claim 1 or 2 further defined by the step of exciting both orthogonal modes equally in propagating polarized light through the optical fiber.

5. The method according to claim 1 or 2 further defined by launching polarized light into the optical fiber at 45°

relative to its fast and slow axes.

6. The method according to claim 1 or 2 wherein a length of the optical fiber is stressed by coiling it about a pressure compliant cylindrical member and exposing it to an acoustic field condition.

7. The method according to claim 1 or 2 wherein a length of the optical fiber is stressed by tension coiling it about a cylindrical member of magnetostrictive material and exposing it to a magnetic field condition.

8. The method according to claim 1 or 2 further defined by splitting the linear polarized light at 45°

to the fibers fast and slow axes.

9. The method according to claim 1 or 2 further defined by the step of field condition stressing a length of the optical fiber transversely to its fast axis for increasing its birefringence.

10. The method according to claim 1 or 2 further defined by the step of field condition stressing a length of the optical fiber in a direction aligned with its fast axis for decreasing its birefringence.

11. A sensor for sensing a field condition with minimum disturbance from environmentally induced perturbations comprising:

a sensing region defined by a length of single mode birefringent optical fiber made birefringent to have two orthogonally disposed eigenmodes oriented respectively along fast and slow axes, said optical fiber being disposed on a carrier;

means for launching linear polarized light into one end of the optical fiber at 45°

to its fast and slow axes for propagation therethrough along its length and emanating at the other end;

said carrier adapted to undergo dimensional changes in response to the field condition to strain the birefringent fiber relative to its axes for changing the birefringence thereof;

means for splitting one portion of the light emanating from the optical fiber other end into first and second components of linearly polarized light which are at 45°

to the optical fiber fast and slow axes;

a quarter wave plate in another portion of the polarized light emanating from the optical fiber end for introducing a differential 90°

phase shift therein;

means for splitting the phase shifted light into a third component of left circularly polarized light and a fourth component of right circularly polarized light;

means for monitoring the intensities of the first and second linearly polarized light components to produce first and second electrical signals respectively and for combining the first and second electrical signals to filter out low frequency perturbations to provide a third electrical signal proportional to stresses in the optical fiber induced by the field condition;

means for monitoring the intensities of the third and fourth circularly polarized light components to produce fourth and fifth electrical signals respectively and for combining the fourth and fifth electrical signals to filter out low frequency perturbations to provide a stress induced sixth electrical signal which is phase shifted by 90°

relative to the third electrical signal;

means for combining the third and sixth electrical signals to produce an output electrical signal which is independent of low frequency environmentally induced perturbations.

12. The invention according to claim 11 wherein the carrier is a pressure complaint mandrel having a cylindrical surface on which the optical fiber is tension wound whereby acoustic waves are adapted to cause the mandrel to strain the optical fiber.

13. The invention according to claim 11 wherein the carrier is a tubular mandrel member of magnetostrictive material and the optical fiber is tension wound about the wall thereof to strain it to induce birefringence whereby a magnetic field condition causes the material to undergo dimensional changes to further strain the optical fiber relative to its axes.

14. The invention according to claim 13 wherein the optical fiber is disposed in the wall of the magnetostrictive tubular member.

15. The invention according to claim 14 wherein the optical fiber is secured to the magnetostrictive material in the wall.

16. The invention according to claim 12, 13, 14 or 15 wherein the optical fiber fast axis is disposed normal to the mandrel surface whereby dimensional changes thereof change fiber birefringence.

17. The invention according to claim 11 wherein the carrier is an elongate elliptical body of magnetostrictive material coextensively surrounding an intrinsically birefringent optical fiber having orthogonally disposed fast and slow axes.

18. The invention according to claim 17 wherein major and minor axes of the elliptical body are aligned with the fast and slow axes of the intrinsically birefringent optical fiber wherein dimensional changes in the elliptical body induced by a magnetic field condition cause the elliptical body to strain the fiber along its axes to change its birefringence.