Electric current sensor using the faraday effect

Claim 2

A detector for electric current comprising: a material substantially transparent to light, said material having at least one characteristic direction in the absence of a magnetic field, and said material exhibiting the Faraday effect in response to a magnetic field generated by said electric current; and means for generating said light in a substantially linear polarization in a predetermined polarization direction and for injecting said light having a predetermined polarization direction into said material with an orientation with respect to said at least one characteristic direction such that a predetermined angle is established between said polarization direction and said at least one characteristic direction, said predetermined angle chosen to permit separation of a rotation of the polarization of said light by the Faraday effect from polarization effects on said light by a birefringence of said material.

Claim 3

A detector for electric current, comprising: a material substantially transparent to light, said material having at least one characteristic direction in the absence of a magnetic field, and said material exhibiting the Faraday effect in response to a magnetic field generated by said electric current; and means for generating said light in a substantially linear polarization in a predetermined polarization direction and for injecting said light having a predetermined polarization direction into said material with an orientation with respect to said at least one characteristic direction such that a non-zero angle is established between said polarization direction and said at least one characteristic direction, said non-zero angle chosen to permit separation of a rotation of the polarization of said light by the Faraday effect from other polarization effects on said light by said material.

Claim 4

A detector for electric current, comprising: a material substantially transparent to light, said material having at least one characteristic direction in the absence of a magnetic field, and said material exhibiting the Faraday effect in response to a magnetic field generated by said electric current; and means for generating said light in a substantially linear polarization in a predetermined polarization direction and for injecting said light having a predetermined polarization direction into said material with an orientation with respect to said at least one characteristic direction such that a non-zero angle is established between said polarization direction and said at least one characteristic direction, said non-zero angle chosen to permit separation of a rotation of the polarization of said light by the Faraday effect from other polarization effects on said light by said material.

Claim 5

The apparatus as in claim 2 further comprising: means for separating light emerging from said material into a first component having a first polarization and into a second component having a second polarization; means for detecting a first intensity of said first component and for detecting a second intensity of said second component; and, means, responsive to said first intensity and said second intensity, for determining a magnitude of said electric current.

Claim 6

The apparatus as in claim 1 or 2 further comprising: a first photodetector and a second photodetector to detect light after it emerges from said material, said first photodetector capable of detecting a first optical intensity having a first polarization direction at substantially 67.5 degrees to said at least one characteristic direction as said one characteristic direction appears at an exit surface of said material, and said second photodetector capable of detecting a second optical intensity having a second polarization direction at substantially 90 degrees to said first polarization direction.

Claim 7

The apparatus as in claim 1 or 2 further comprising: means for separating light emerging from said material into a first component having a first polarization to form a first emerging light beam, and into a second component having a second polarization to form a second emerging light beam; a first photodetector for detecting an intensity of said first emerging light beam; means, responsive to said first photodetector, for computing a first ratio of an AC component to a DC component of said intensity of said first emerging light beam; a second photodetector for detecting an intensity of said second emerging light beam; means, responsive to said second photodetector, for computing a second ratio of an AC component to a DC component of said intensity of said second emerging light beam; and, means for computing a quotient by dividing a function of said first ratio by a function of said second ratio.

Claim 8

The apparatus as in claim 5 wherein said means for computing a quotient, further comprises: means for producing a first average value of said first ratio; means for producing a second average value of said second ratio; and, means for computing said quotient by dividing said first average value of said first ratio, by said second average value of said second ratio.

Claim 9

The apparatus as in claim 5 further comprising: means for computing a stress birefringence of said material by using the expression βL=2*sin.sup.-1 (K1*(R-1)/(R+1)).sup.1/2 wherein said R is a symbol standing for said quotient and said K1 is a numerical constant to account for polarization leakage in a polarizer; and, means, responsive to said first ratio and responsive to said birefringence βL, for computing said electric current.

Claim 10

The apparatus in claim 7 wherein said means for computing said electric current further comprises: means, responsive to said birefringence βL, for computing a first correction factor CF(1,βL), for said first ratio; means for correcting said first ratio by said correction factor; means, responsive to said first ratio and responsive to said first correction factor, for estimating a magnitude J, of said electric current; means, responsive to said birefringence βL, for computing a spread function SF(βL); means for adjusting said correction factor using the expression ACF(J,βL)=CF(1,βL)-SF(βL)*(J/J.sub.max).sup.2 means for iterating a calculation of said quantity ACF(J,βL) until a new value differs from the last value by less than a predetermined amount; and, means, responsive to said final value of said quantity ACF(J,βL), for computing a final value of said electric current.

Claim 11

The apparatus as in claim 1, or 2 wherein said predetermined angle is between 10 degrees and 80 degrees.

Claim 12

The apparatus as in claim 1 or 2 wherein said predetermined angle is 22.5 degrees.

Claim 13

The apparatus as in claim 1 or 2 wherein said material transparent to said light comprises an optical fiber.

Claim 14

The apparatus as in claim 1 or 2 wherein said material substantially transparent to said light further comprises: an optical fiber looped around a conductor carrying said electric current.

Claim 15

The apparatus as in claim 1 or 2 wherein said material transparent to said light comprises an optical fiber arranged in a coil, and a conductor carrying said electric current passes through said coil.

Claim 16

The apparatus as in claim 1 or 2 further comprising: a magnetic field concentrator to concentrate said magnetic field onto said material substantially transparent to said light.

Claim 17

The apparatus as in claim 1 or 2 wherein said material transparent to said light comprises at least one block of glass.

Claim 18

The apparatus as in claim 1 or 2 wherein said material substantially transparent to said light, further comprises: a block of glass having the shape of a rectangular parallelepiped.

Claim 19

The apparatus as in claim 1 or 2 further comprising: wherein said material transparent to said light is a block of glass; and, a magnetic field concentrator surrounding a conductor carrying said electric current, said concentrator arranged to concentrate said magnetic field generated by said electric current onto said block of glass.

Claim 20

The apparatus as in claim 1 or 2 wherein said characteristic direction is parallel to a planar side of said block of glass.

Claim 21

The apparatus as in claim 1 or 2, wherein said means for generating light comprises a light emitting diode.

Claim 22

The apparatus as in claim 1 or 2, wherein said means for generating light comprises a laser.

Claim 23

The apparatus as in claim 1 or 2, wherein said means for generating light comprises a solid state laser.

Claim 24

The apparatus as in claim 1 or 2 wherein said means for generating said light having a predetermined polarization direction, further comprises: an optical fiber having a light beam launched therein by said means for generating light; and, a polarizer having said light beam directed thereto by said optical fiber, said polarizer having a transmission direction, and said transmission direction set at substantially 22.5 degrees relative to said at least one characteristic direction.

Claim 25

An electric current detector, comprising: a material substantially transparent to light, said material having at least one characteristic direction in the absence of a magnetic field, and said material exhibiting the Faraday effect in response to a magnetic field generated by said electric current; means for generating said light in a substantially linear polarization in a predetermined polarization direction and for injecting said light having a predetermined polarization direction into said material with an orientation with respect to said at least one characteristic direction such that a predetermined angle is established between said polarization direction and said at least one characteristic direction, said predetermined angle chosen to permit separation of a rotation of the polarization of said light by the Faraday effect from polarization effects on said light by a birefringence of said material; means for separating light emerging from said material into a first component having a first polarization and into a second component having a second polarization; means for detecting a first intensity of said first component and for detecting a second intensity of said second component; and means, responsive to said first intensity and said second intensity, for determining a magnitude of said electric current.

Claim 26

An electric current detector, comprising: a material substantially transparent to light, said material having at least one characteristic direction in the absence of a magnetic field, and said material exhibiting the Faraday effect in response to a magnetic field generated by said electric current; means for generating said light in a substantially linear polarization in a predetermined polarization direction and for injecting said light having a predetermined polarization direction into said material with an orientation with respect to said at least one characteristic direction such that a predetermined angle is established between said polarization direction and said at least one characteristic direction, said predetermined angle chosen to permit separation of a rotation of the polarization of said light by the Faraday effect from polarization effects on said light by a birefringence of said material; means for separating light emerging from said material into a first component having a first polarization and into a second component having a second polarization; means for detecting a first intensity of said first component and for detecting a second intensity of said second component; and means, responsive to said first intensity and said second intensity, for determining a magnitude of said electric current.

Claim 27

An electric current detector, comprising: a material substantially transparent to light, said material having at least one characteristic direction in the absence of a magnetic field, and said material exhibiting the Faraday effect in response to a magnetic field generated by said electric current; means for generating said light in a substantially linear polarization in a predetermined polarization direction and for injecting said light having a predetermined polarization direction into said material with an orientation with respect to said at least one characteristic direction such that a predetermined angle of substantially 22.5 degrees is established between said polarization direction and said at least one characteristic direction; means for separating light emerging from said material into a first component having a first polarization to form a first emerging light beam, and into a second component having a second polarization to form a second emerging light beam; a first photodetector for detecting an intensity of said first emerging light beam; means, responsive to said first photodetector, for computing a first ratio of an AC component to a DC component of said intensity of said first emerging light beam; a second photodetector for detecting an intensity of said second emerging light beam; means, responsive to said second photodetector, for computing a second ratio of an AC component to a DC component of said intensity of said second emerging light beam; means for producing a first average value of said first ratio; means for producing a second average value of said second ratio; means for computing said quotient by dividing said first average value of said ratio, by said second average value of said second ratio; means for computing a stress birefringence of said material by using the expression βL=2*sin.sup.-1 (K1*(R-1)/(R+1)).sup.1/2 wherein said R is a symbol standing for said quotient and said K1 is a numerical constant to account for polarization leakage in a polarizer; means, responsive to said birefringence βL, for computing a first correction factor CF(1,βL), for said first ratio; means for correcting said first ratio by said correction factor; means, responsive to said first ratio and responsive to said first correction factor, for estimating a magnitude, J, of said electric current; means, responsive to said birefringence βL, for computing a spread function SF(βL); means for adjusting said correction factor using the expression ACF(J,βL)=(CF(1,βL)-SF(βL)*(J/J.sub.max).sup.2 means for iterating a calculation of said quantity ACF(J,βL) until a new value differs from a last value by less than a predetermined amount; and, means, responsive to said past value of said quantity ACF(J,β), for computing a final value of said electric current.

Claim 28

An electric current detector, comprising: a material substantially transparent to light, said material having at least one characteristic direction in the absence of a magnetic field, and said material exhibiting the Faraday effect in response to a magnetic field generated by said electric current; means for generating said light in a substantially linear polarization in a predetermined polarization direction and for injecting said light having a predetermined polarization direction into said material with an orientation with respect to said at least one characteristic direction such that a predetermined angle of substantially 22.5 degrees is established between said polarization direction and said at least one characteristic direction; means for separating light emerging from said material into a first component having a first polarization to form a first emerging light beam, and into a second component having a second polarization to form a second emerging light beam; a first photodetector for detecting an intensity of said first emerging light beam; means, responsive to said first photodetector, for computing a first ratio of an AC component to a DC component of said intensity of said first emerging light beam; a second photodetector for detecting an intensity of said second emerging light beam; means, responsive to said second photodetector, for computing a second ratio of an AC component to a DC component of said intensity of said second emerging light beam; means for producing a first average value of said first ratio; means for producing a second average value of said second ratio; means for computing said quotient by dividing said first average value of said ratio, by said second average value of said second ratio; means for computing a stress birefringence of said material by using the expression βL=2*sin.sup.-1 (K1*(R-1)/(R+1)).sup.1/2 wherein said R is a symbol standing for said quotient and said K1 is a numerical constant to account for polarization leakage in a polarizer; means, responsive to said birefringence βL, for computing a first correction factor CF(1,βL), for said first ratio; means for correcting said first ratio by said correction factor; means, responsive to said first ratio and responsive to said first correction factor, for estimating a magnitude, J, of said electric current; means, responsive to said birefringence βL, for computing a spread function SF(βL); means for adjusting said correction factor using the expression ACF(J,βL)=(CF(1,βL)-SF(βL)*(J/J.sub.max).sup.2 means for iterating a calculation of said quantity ACF(J,βL) until a new value differs from a last value by less than a predetermined amount; and, means, responsive to said past value of said quantity ACF(J,β), for computing a final value of said electric current.

Claim 33

An electric current detector, comprising: a material substantially transparent to light, said material having at least one characteristic direction in the absence of a magnetic field and said material exhibiting the Faraday effect in response to a magnetic field generated by said electric current; means for generating said light in a substantially linear polarization in a predetermined polarization direction and for injecting said light having a predetermined polarization direction into said material with an orientation with respect to said at least one characteristic direction such that a predetermined angle of substantially 22.5 degrees is established between said polarization direction and said at least one characteristic direction; and a processor including: means for separating light emerging from said material into a first component and into a second component; means, responsive to said first component and said second component, for determining a stress birefringence of said material; means, responsive to said stress birefringence, for producing a correction factor; and means, responsive to said correction factor for determining a magnitude of said electric current.

Claim 34

An electric current detector, comprising: a material substantially transparent to light, said material having at least one characteristic direction in the absence of a magnetic field and said material exhibiting the Faraday effect in response to a magnetic field generated by said electric current; means for generating said light in a substantially linear polarization in a predetermined polarization direction and for injecting said light having a predetermined polarization direction into said material with an orientation with respect to said at least one characteristic direction such that a predetermined angle of substantially 22.5 degrees is established between said polarization direction and said at least one characteristic direction; and a processor including: means for separating light emerging from said material into a first component and into a second component; means, responsive to said first component and said second component, for determining a stress birefringence of said material; means, responsive to said stress birefringence, for producing a correction factor; and means, responsive to said correction factor for determining a magnitude of said electric current.

Claim 37

The method as in claim 28 wherein said chosen non-zero angle is substantially 22.5 degrees.