Fiber optic magnetic field sensor

• US 4,675,522 A
• Filed: 10/09/1985
• Issued: 06/23/1987
• Est. Priority Date: 10/09/1985
• Status: Expired due to Fees

• Current Assignee: Spectron Development Laboratories
• Original Assignee: Spectron Development Laboratories
• Inventors: Arunkumar, Koovappadi A.
• Primary Examiner(s): LaRoche, Eugene R.
• Assistant Examiner(s): Lee, James C.
• Application Number:
  US06/785,739
• Time in Patent Office: 622 Days
• Field of Search: 250/227, 250/231 R, 324/96, 324/244, 356/345
• US Class Current: 250/227.19
• CPC Class Codes: G01R 33/0327 with application of magnetostriction

Abstract

The present invention provides an improved fiber optic magnetometer having particular application for use in environments having large magnetic field ranges and gradients, such as space based applications. The magnetometer includes a laser which generates a coherent beam of light which is split by a beam splitter into first and second beams. The first beam is passed through a single mode fiber optic having a short metallic conductor attached to it. This fiber is referred to as the "sensor arm" of the magnetometer. The second beam is passed through another single mode fiber which is wrapped around a modulator that is coupled to a feedback circuit. This adjusts the magnetometer such that ambient system noise is filtered and the device is maintained at maximum sensitivity. The output of the two fibers is combined forming a Mach-Zehnder interferometer. A current I is passed through the conductor in the sensor arm. If this fiber is in the vicinity of a magnetic field, displacement of the current carrying conductor will cause the fiber to bow. The resulting stretching of the fiber increases the pathlength for the light beam traversing through the sensor arm. The subsequent phase change measured by the Mach-Zehnder is related to the force exerted by the magnetic field on the conductor. The direction in which the fiber bows is dependent upon the magnetic field direction. The present invention also discloses an improved modulator for maintaining the present invention at the point of optimum operation.

Claims

1. A fiber optic transducer comprising:

light generation means for generating first and second coherent beams of light;

a first single mode optical fiber optically coupled to said first beam, said first optical fiber having a non-magnetic metallic conductor attached to a portion of said fiber;

current generating means coupled to said conductor for selectively passing a current I through said conductor;

a second single mode optical fiber optically coupled to said second beam;

light combining means in optical alignment with said first and second beams after said beams pass through said respective fibers for combining said beams and forming an interferance pattern between said beams;

sensing means for sensing phase differences between said combined beams from said interference pattern, said phase differences resulting from the physical displacement of said first optical fiber in the presence of a magnetic field B from said current I passing through said non-magnetic conductor in the presence of said magnetic field, said conductor returning to its original position once said magnetic field B is removed.

2. The transducer as defined by claim 1, wherein said non-magnetic conductor has a length l.

3. The transducer as defined by claim 2, further including modulator means coupled to said second optical fiber for selectively altering the path length of said second fiber to cancel spurious noise signals in said transducer, and maintain said transducer at a quadrature point.

4. The transducer as defined by claim 3, further including a stopper disposed adjacent to said metallic conductor to limit movement of said first fiber to one direction.

5. The transducer as defined by claim 4, wherein said sensing means includes photodiode detectors.

6. The transducer as defined by claim 5, wherein said metallic conductor is disposed longitudinally along said first fiber.

7. The transducer as defined by claim 5, wherein said metallic conductor is disposed perpendicular to said first fiber.

8. The transducer as defined by claim 3, wherein the magnetic field strength B is determined from the expression:

##EQU7## where;

I=current passing through said conductor attached to a portion of said first fiber;

λ

=wavelength of said first and second coherent beams of light;

L=length of said first fiber;

l=length of said conductor;

r=radius of said first and second fibers;

δ

φ

=phase difference between said first and second beams sensed by said sensing means.

9. The transducer as defined by claim 8, wherein said phase differences between said first and second beams sensed by said sensing means is defined by:

##EQU8## where;

67 L=extra path length induced in said first fiber by a magnetic field B through physical displacement.

10. The transducer as defined by claim 9, wherein said light generation means comprises a laser.

11. A method for sensing physical parameters in an ambient environment using a fiber optic transducer comprising the steps of:

generating first and second coherent beams of light;

passing said first beam through a single mode optical fiber having a non-magnetic metallic conductor attached to a portion of said fiber;

passing said second beam through a second single mode optical fiber;

combining said first and second beams passed through said respective fibers to form an interference pattern between said beams;

sensing phase differences between said beams, said phase differences resulting from the physical displacement of said first optical fiber in the presence of a magnetic field B from said current passing through said non-magnetic conductor in the presence of said magnetic field, said conductor returning to its original position once said magnetic field B is removed.

12. The method as defined by claim 11, further including the step of selectively altering the path length of said second fiber to cancel spurious noise signals in said transducer, and maintain said transducer at a quadrature point.

13. The method as defined by claim 12, including the step of limiting the physical displacement of said first fiber to one direction.

14. The method as defined by claim 11, wherein magnetic field strength B is derived from the expression:

##EQU9## where;

I=current passing through said conductor attached to a portion of said first fiber;

λ

=wavelength of said first and second coherent beams of light;

L=length of said first fiber;

l=length of said conductor;

r=radius of said first and second fibers;

δ

φ

=phase difference between said first and second beams sensed by said sensing means.

15. The method as defined by claim 14, wherein said phase differences between said first and second beams sensed by said sensing means is defined by:

##EQU10## where;

16. L=extra path length induced in said first fiber by an ambient magnetic field B through physical displacement.