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US4665363A Expired / Lapsed US ⏱️ 0.0 years remaining

Optical fibre magnetic gradient detector

Assignee: STC PLC
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Filing: 1986-02-20
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Granted: 1987-05-12
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Expires: 2006-02-20
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Abstract

Abstract Two portions (B,C) of one arm of an optical fibre Mach-Zehnder interferometer are magnetically sensitized and each has applied thereto an a.c. bias fields at a respective different frequency (w 1 , w 2 ). One portion (A) of the other arm of the interferometer is magnetically sensitized and has two a.c. bias fields applied thereto, each at one of the different frequencies (w 1 ,w 2 ). The fields for portion A and C are aligned with a first direction (x) whereas those for A and B are parallel, A and B being separated in a second direction (y). The detected output of the interferometer at frequency w 1 is related to the magnetic gradient in the y direction, whereas the detected output at frequency w 2 is related to the magnetic gradient in the x direction. Thus using two bias frequencies allows one interferometer to be used to detect two gradients (FIG. 8).

Inventors

  • 👤 Philip Extance
  • 👤 Roger E. Jones

Bibliographic Details

Application Number —
Jurisdiction US
Data Source google_patents
Last Synchronized 2026-11-03 08:03
CPC Classifications
G; G01; G01R; G01R33/00; G01R33/02; G01R33/022; G01R33/032; G01R33/0327

Claims Analysis

Total Claims: 14
Claim 1
Independent Claim 356 words
An optical fibre magnetic gradient detector for detecting two orthogonal magnetic gradients, which detector comprises: first and second optical fibres arranged in the arms of an optical fibre Mach-Zehnder interferometer; a first portion of the first optical fibre and first and second portions of the second optical fibre being magnetically sensitised by association therewith of respective magnetostrictive material such that application of a d.c. magnetic field to said magnetostrictive material causes a corresponding change in optical path length within the respective fibre portion; wherein the first portion of the first optical fibre is spaced apart from the first portion of the second optical fibre in a first direction; wherein the first portion of the first optical fibre is spaced apart from the second portion of the second optical fibre in a second direction, which first and second directions are orthogonal; the first and second portions of the second optical fibre each being disposed within respective solenoid means to which respective a.c. signals are applied such that respective bias fields oscillating at first and second differing frequencies are provided thereat; the first portion of the first optical fibre being provided with solenoid means so as to provide thereat two bias fields, one oscillating at said first frequency and the other oscillating at said second frequency, the bias fields of the first portion of said first optical fibre and the second portion of said second optical fibre being aligned with the second direction, and the bias fields of the first portion of said first optical fibre and the first portion of said second optical fibre being parallel; and wherein in use each said fibre portion has an output including a component at the or each respective a.c. frequency which is proportional to the d.c. magnetic field threreat and from which the magnitude of the two orthogonal magnetic gradients can be determined, the first portions of the first and second optical fibres responding to one of said two orthogonal magnetic gradients and the first portion of the first optical fibre and the second portion of the second optical fibre responding to the other of said two orthogonal magnetic gradients.
Claim 2
Dependent Claim 356 words
An optical fibre magnetic gradient detector for detecting two orthogonal magnetic gradients, which detector comprises: first and second optical fibres arranged in the arms of an optical fibre Mach-Zehnder interferometer; a first portion of the first optical fibre and first and second portions of the second optical fibre being magnetically sensitised by association therewith of respective magnetostrictive material such that application of a d.c. magnetic field to said magnetostrictive material causes a corresponding change in optical path length within the respective fibre portion; wherein the first portion of the first optical fibre is spaced apart from the first portion of the second optical fibre in a first direction; wherein the first portion of the first optical fibre is spaced apart from the second portion of the second optical fibre in a second direction, which first and second directions are orthogonal; the first and second portions of the second optical fibre each being disposed within respective solenoid means to which respective a.c. signals are applied such that respective bias fields oscillating at first and second differing frequencies are provided thereat; the first portion of the first optical fibre being provided with solenoid means so as to provide thereat two bias fields, one oscillating at said first frequency and the other oscillating at said second frequency, the bias fields of the first portion of said first optical fibre and the second portion of said second optical fibre being aligned with the second direction, and the bias fields of the first portion of said first optical fibre and the first portion of said second optical fibre being parallel; and wherein in use each said fibre portion has an output including a component at the or each respective a.c. frequency which is proportional to the d.c. magnetic field threreat and from which the magnitude of the two orthogonal magnetic gradients can be determined, the first portions of the first and second optical fibres responding to one of said two orthogonal magnetic gradients and the first portion of the first optical fibre and the second portion of the second optical fibre responding to the other of said two orthogonal magnetic gradients.
Claim 3
Dependent Claim 69 words
An optical fibre magnetic gradient detector as claimed in claim 1, including means for coupling a light source to input ends of the first and second fibres and means for detecting light from output ends thereof, detected signals at the first frequency being related to the magnetic gradient in the first direction and detected signals at the second frequency being related to the magnetic gradient in the second direction.
Claim 4
Dependent Claim 20 words
An optical fibre magnetic gradient detector as claimed in claim 1 wherein the a.c. signals comprise digitally generated sine waves.
Claim 5
Dependent Claim 31 words
An optical fibre magnetic gradient detector as claimed in claim 1 wherein the magnetically sensitised fibre portions comprise planar sensing coils disposed in the plane including the first and second directions.
Claim 6
Dependent Claim 61 words
An optical fibre magnetic gradient detector as claimed in claim 4, wherein the fibre of the coils is magnetically sensitised by the application of a magnetostrictive coating material thereto, the thickness of the coating being as thin as possible to minimise the effect of the demagnetising field and thick enough to maximise the effect of mass loading on the magnetostrictive strain.
Claim 7
Dependent Claim 35 words
An optical fibre magnetic gradient detector as claimed in claim 2 and including a piezoelectric phase modulator associated with the first fibre and controlled by the detector means output and serving to control the interferometer.
Claim 8
Dependent Claim 39 words
An optical fibre magnetic gradient detector as claimed in claim 1 and including means to apply known field gradient whereby to cancel each magnetic gradient to be detected and thus provide a measure of the gradient to be detected.
Claim 9
Independent Claim 385 words
A method of detecting two orthogonal magnetic gradients with first and second optical fibres arranged as the arms of an optical fibre Mach-Zehnder interferometer, a first portion of the first optical fibre and first and second portions of the second optical fibre being magnetically sensitised by association therewith of a respective magnetostrictive material such that application of a d.c. magnetic field to said magnetostrictive material causes a corresponding change in optical path length within the respective fibre portion, including the steps of: spacing the first portion of the first optical fibre apart from the first portion of the second optical fibre in a first direction and spacing the first portion of the first optical fibre apart from the second portion of the second optical fibre in a second direction, which first and second directions are orthogonal; disposing each of the first and second portions of the second optical fibre in respective solenoids; applying respective a.c. signals to the solenoids so as to provide at the first portion of said second optical fibre a bias field oscillating at a first frequency and to provide at the second portion of said second optical fibre a bias field oscillating at a second frequency; disposing the first portion of the first optical fibre in a respective solenoid means; applying a.c. signals to said solenoid means so as to provide at the first portion of the first optical fibre two bias fields, one osillating at the first frequency and one oscillating at said second frequency, the bias fields of said first portion of the first optical fibre and the second portion of the second being aligned with the second direction and the bias fields of the first portion of the first optical fibre and the first portion of the second optical fibre being parallel, the output of each fibre portion including a component at the or each respective a.c. frequency which is proportional to the d.c. magnetic field thereat and from which the magnitude of the two orthogonal magnetic gradients can be determined, the first portions of the first and second optical fibres responding to one of said two orthogonal magnetic gradients and the first portion of the first optical fibre and the second portion of the second optical fibre responding to the other of said two orthogonal magnetic gradients.
Claim 10
Independent Claim 385 words
A method of detecting two orthogonal magnetic gradients with first and second optical fibres arranged as the arms of an optical fibre Mach-Zehnder interferometer, a first portion of the first optical fibre and first and second portions of the second optical fibre being magnetically sensitised by association therewith of a respective magnetostrictive material such that application of a d.c. magnetic field to said magnetostrictive material causes a corresponding change in optical path length within the respective fibre portion, including the steps of: spacing the first portion of the first optical fibre apart from the first portion of the second optical fibre in a first direction and spacing the first portion of the first optical fibre apart from the second portion of the second optical fibre in a second direction, which first and second directions are orthogonal; disposing each of the first and second portions of the second optical fibre in respective solenoids; applying respective a.c. signals to the solenoids so as to provide at the first portion of said second optical fibre a bias field oscillating at a first frequency and to provide at the second portion of said second optical fibre a bias field oscillating at a second frequency; disposing the first portion of the first optical fibre in a respective solenoid means; applying a.c. signals to said solenoid means so as to provide at the first portion of the first optical fibre two bias fields, one osillating at the first frequency and one oscillating at said second frequency, the bias fields of said first portion of the first optical fibre and the second portion of the second being aligned with the second direction and the bias fields of the first portion of the first optical fibre and the first portion of the second optical fibre being parallel, the output of each fibre portion including a component at the or each respective a.c. frequency which is proportional to the d.c. magnetic field thereat and from which the magnitude of the two orthogonal magnetic gradients can be determined, the first portions of the first and second optical fibres responding to one of said two orthogonal magnetic gradients and the first portion of the first optical fibre and the second portion of the second optical fibre responding to the other of said two orthogonal magnetic gradients.
Claim 11
Dependent Claim 62 words
A method as claimed in claim 8, including the steps of applying light to input ends of the first and second fibres, and detecting light from output ends thereof, detected signals at the first frequency being related to the magnetic gradient in the first direction and detected signals at the second frequency being related to the magnetic gradient in the second direction.
Claim 12
Dependent Claim 36 words
A method as claimed in claim 8, including the step of applying a known field gradient whereby to cancel each magnetic gradient to be detected and thus provide a measure of the gradient to be detected.
Claim 13
Dependent Claim 409 words
An optical fibre magnetic gradient detector for detecting two orthogonal magnetic gradients, which detector comprises: first and second optical fibres arranged in the arms of an optical fibre Mach-Zehnder interferometer; a first portion of the first optical fibre and first and second portions of the second optical fibre being magnetically sensitised by association therewith of respective magnetostrictive material such that application of a d.c. magnetic field to said magnetostrictive material causes a corresponding change in optical path length within the respective fibre portion; wherein the first portion of the first optical fibre is spaced apart from the first portion of the second optical fibre in a first direction; wherein the first portion of the first optical fibre is spaced apart from the second portion of the second optical fibre in a second direction, which first and second directions are orthogonal; the first and second portions of the second optical fibre each being disposed within respective solenoid means to which respective a.c. signals are applied such that respective bias fields oscillating at first and second differing frequencies are provided thereat; the first portion of the first optical fibre being provided with solenoid means so as to provide thereat two bias fields, one oscillating at said first frequency and the other oscillating at said second frequency, the bias fields of the first portion of said first optical fibre and the second portion of said second optical fibre being aligned with the second direction, and the bias fields of the first portion of said first optical fibre and the first portion of said second optical fibre being parallel; and wherein in use each said fibre portion has an output including a component at the or each respective a.c. frequency which is proportional to the d.c. magnetic field thereat and from which the magnitude of the two orthogonal magnetic gradients can be determined, the first portions of the first and second optical fibres responding to one of said two orthogonal magnetic gradients and the first portion of the first optical fibre and the second portion of the second optical fibre responding to the other of said two orthogonal magnetic gradients, and including means for coupling a light source to input ends of the first and second optical fibres and means for detecting light from output ends thereof, detected signals at the first frequency being related to the magnetic gradient in the second direction, and wherein the a.c. signals comprise digitally generated sine waves.
Claim 14
Dependent Claim 409 words
An optical fibre magnetic gradient detector for detecting two orthogonal magnetic gradients, which detector comprises: first and second optical fibres arranged in the arms of an optical fibre Mach-Zehnder interferometer; a first portion of the first optical fibre and first and second portions of the second optical fibre being magnetically sensitised by association therewith of respective magnetostrictive material such that application of a d.c. magnetic field to said magnetostrictive material causes a corresponding change in optical path length within the respective fibre portion; wherein the first portion of the first optical fibre is spaced apart from the first portion of the second optical fibre in a first direction; wherein the first portion of the first optical fibre is spaced apart from the second portion of the second optical fibre in a second direction, which first and second directions are orthogonal; the first and second portions of the second optical fibre each being disposed within respective solenoid means to which respective a.c. signals are applied such that respective bias fields oscillating at first and second differing frequencies are provided thereat; the first portion of the first optical fibre being provided with solenoid means so as to provide thereat two bias fields, one oscillating at said first frequency and the other oscillating at said second frequency, the bias fields of the first portion of said first optical fibre and the second portion of said second optical fibre being aligned with the second direction, and the bias fields of the first portion of said first optical fibre and the first portion of said second optical fibre being parallel; and wherein in use each said fibre portion has an output including a component at the or each respective a.c. frequency which is proportional to the d.c. magnetic field thereat and from which the magnitude of the two orthogonal magnetic gradients can be determined, the first portions of the first and second optical fibres responding to one of said two orthogonal magnetic gradients and the first portion of the first optical fibre and the second portion of the second optical fibre responding to the other of said two orthogonal magnetic gradients, and including means for coupling a light source to input ends of the first and second optical fibres and means for detecting light from output ends thereof, detected signals at the first frequency being related to the magnetic gradient in the second direction, and wherein the a.c. signals comprise digitally generated sine waves.

References Cited (Backward Citations)

US4587487A Cited
US4591786A Cited

USPTO Annuity & Maintenance Windows

Annuity Stage Window Opens Payment Deadline Surcharge Period Until Estimated Fee Status
3.5 Years (Year 4) 1990-05-11 1990-11-10 1991-05-12 $2000.00 Window Closed / Lapsed
7.5 Years (Year 8) 1994-05-11 1994-11-10 1995-05-12 $3760.00 Window Closed / Lapsed
11.5 Years (Year 12) 1998-05-11 1998-11-10 1999-05-12 $7700.00 Window Closed / Lapsed

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