Method and apparatus for optically measuring a current

• US 4,564,754 A
• Filed: 03/07/1983
• Issued: 01/14/1986
• Est. Priority Date: 03/08/1982
• Status: Expired due to Term

• Current Assignee: Hitachi, Ltd.
• Original Assignee: Hitachi, Ltd.
• Inventors: Sato, Tadashi, Takahashi, Genji, Inui, Yoshiaki
• Primary Examiner(s): Corbin, John K.
• Assistant Examiner(s): Eyssallenne, R.
• Application Number:
  US06/472,834
• Time in Patent Office: 1,044 Days
• Field of Search: 250/225, 250/227, 324/96, 324/244, 356/72, 350/374, 350/375, 350/376
• US Class Current: 250/225
• CPC Class Codes: G01R 15/246 based on the Faraday, i.e. linear magneto-optic, effect

Abstract

A current is measured by making use of a rotation of polarization plane in a magnetic field, that is, a Faraday effect. A conductor under measurement is transversely inserted into a center opening of a Faraday effect glass which has at least two total reflection areas on a periphery thereof so that a light directed into the Faraday effect glass is circulated around the conductor and emitted externally. The light emitted from the Faraday effect glass is split into at least two light beams, which are converted to electric signals by photoelectric elements, and A.C. components contained in the electric signals are extracted and compared. The electric signals are corrected based on the comparison result.

The present measuring apparatus and method attain high precision current measurement in a stable manner over an extended period.

Claims

1. An optical current measuring apparatus comprising:

a conductor for conducting a current under measurement;

a Faraday effect glass disposed to link perpendicularly to said conductor and having at least two total reflection areas at corners thereof;

a light source for directing a light to a light input section of said Faraday effect glass;

a polarizer for linearly polarizing the light from said light source and directing the linearly polarized light to said Faraday effect glass;

said linearly polarized light being reflected at said total reflection areas of said Faraday effect glass such that said linearly polarized light circulates around said conductor as linearly polarized light and emits from a light output section of said Faraday glass as linearly polarized light, whereby said current is measured based on a Faraday rotation angle of the light by a magnetic field created by said current flowing in said conductor;

said total reflection areas of said Faraday effect glass being configured for enabling said linearly polarized light reflected thereat to circulate and be emitted from said Faraday effect glass as linearly polarized light;

said Faraday effect glass being planar and having an opening through which said conductor extends;

an analyzer disposed to face said light output section of said Faraday effect glass for splitting the light from said light output section into two light beams;

a pair of condenser lenses disposed to condense said two light beams from said analyzer;

a pair of optical fibers disposed to face said condenser lenses;

a pair of light detectors arranged to receive lights transmitted through said optical fibers; and

an arithmetic unit for calculating said Faraday rotation angle based on outputs from said light detectors.

2. An optical current measuring apparatus according to claim 1 wherein each of said total reflection areas includes two closely arranged reflection planes.

3. An optical current measuring apparatus according to claim 1 wherein said total reflection areas of said Faraday effect glass extend over an entire periphery of the planar glass, and a single prism is disposed to interrupt both said light input section and said light output section.

4. An optical current measuring apparatus according to claim 1 wherein said total reflection areas of said Faraday effect glass extend over an entire periphery of the planar glass, and separate prisms are disposed at said light input section and said light output section, respectively.

5. An optical current measuring apparatus comprising:

a conductor for conducting a current under measurement;

a Faraday effect glass disposed to link perpendicularly to said conductor and having at least two total reflection areas at corners thereof;

a light source for directing a light to a light input section of said Faraday effect glass;

a polarizer for linearly polarizing the light from said light source and directing the linearly polarized light to said Faraday effect glass;

said linearly polarized light being reflected at said total reflection areas of said Faraday effect glass such that said linearly polarized light circulates around said conductor and emits from a light output section of said Faraday effect glass, whereby said current is measured based on a Faraday rotation angle of the light by a magnetic field created by said current flowing in said conductor;

said Faraday effect glass being planar and having an opening through which said conductor extends;

each of said total reflection areas at the corners of said Faraday effect glass having two closely arranged reflection planes;

an analyzer disposed to face said light output section of said Faraday effect glass for splitting the light from said light output section into two light beams;

a pair of condenser lenses disposed to condense said two light beams from said analyzer;

a pair of optical fibers disposed to face said condenser lenses;

a pair of light detectors arranged to receive lights transmitted through said optical fibers; and

an arithmetic unit for calculating said Faraday rotation angle based on outputs from said light detectors.

6. A optical current measuring apparatus according to claim 5 wherein said total reflection areas of said Faraday effect glass extend over an entire periphery of the planar glass, and a single prism is disposed to interrupt both said light incident section and said light output section.

7. An optical current measuring apparatus for measuring a current flowing through a conductor by detecting a Faraday rotation angle, said apparatus comprising:

a Faraday effect glass having an opening through which said conductor is passed thereby to inter-link said Faraday effect glass with a current flow in said conductor, said Faraday effect glass having three total internal reflection portions disposed in a light path, said light path looping around a periphery of said conductor;

a light source emitting said light into said light path in said Faraday effect glass;

a polarizer disposed between said light source and said Faraday effect glass for linearly polarizing the light from said light source, said linearly polarized light being passed through said light path for reflection at said total internal reflection portions of said Faraday effect glass and then for exciting from said Faraday effect glass;

an analyzer for splitting said polarized light excited from said Faraday effect glass into two light beams;

a pair of optical fibers in which said two light beams converged by said condenser lenses are guided therealong;

a pair of light detectors for detecting said two light beams guided by said optical fibers; and

means for calculating said Faraday rotation angle on the basis of the detected two light beams so that said current flowing through said conductor is determined according to said Faraday rotation angle,

wherein each of said total internal reflection portions is formed by adjoining two total internal reflection planes, incident planes of the light at each of said total internal reflection planes being perpendicular to each other and said light being total internally reflected at each of said total internal reflection planes so that said light reflected by said total internal reflection portions is maintained as linearly polarized light.

8. An optical current measuring apparatus according to claim 7, wherein said Faraday effect glass has a prism disposed in said light path so that the light emitted from said light source enters into said Faraday effect glass via said prism and the total internally reflected light exits through said prism.

9. An optical current measuring apparatus according to claim 7, wherein said light detectors are photo-electric devices transforming the light guided by said optical fibers into electric signals, and said calculating means includes a pair of amplifiers for amplifying said electric signals, a pair of signal extraction means for extracting A.C. components from said amplified electric signals, comparator means for comparing said A.C. components from said signal extraction means, and signal correction means for correcting said amplified electric signals in accordance with an output of said comparator means so that an error in the Faraday rotation angle due to environmental condition variation in said light path is compensated.

10. An optical current measuring apparatus according to claim 9, wherein said Faraday effect glass has a prism disposed in said light path so that the light emitted from said light source enters into said Faraday effect glass via said prism and the total internally reflected light exits through said prism.

11. An optical current measuring apparatus according to claim 9, wherein each of said signal extraction means is a band-pass filter.

12. An optical current measuring apparatus according to claim 7, wherein said light detectors are photo-electric devices transforming the light guided by said optical fibers into electric signals, and said calculating means includes a pair of amplifiers for amplifying said electric signals, a pair of A/D converters for analog to digital converting said amplified electric signals, and a digital signal processing unit for extracting A.C. components from said converted amplified electric signals and for calculating said current on the basis of said converted amplified electric signals in digital form and said A.C. components in digital form thereby to output said calculated current in digital form.

13. An optical current measuring apparatus according to claim 12, wherein said Faraday effect glass has a prism disposed in said light path so that the light emitted from said light source enters into said Faraday effect glass via said prism and the total internally reflected light exits through said prism.

14. An optical current measuring apparatus according to claim 7, wherein said apparatus includes further combination of said Faraday effect glass, said light source, said polarizer, said analyzer said pair of condenser lenses, said pair of optical fibers, said pair of light detectors, and said calculating means, said Faraday effect glasses in the respective combinations having different characteristics of magnetic field versus Faraday rotation angle so that said Faraday effect glasses share measuring ranges of the current, and said apparatus further includes signal selection means for selecting a higher one of the Faraday rotation angles calculated in said calculating means of the respective combinations.

15. An optical current measuring apparatus according to claim 14, wherein one of said Faraday effect glasses of the respective combinations is made of a lead glass and another of said Faraday effect glasses is made of a silica glass.

16. An optical current measuring apparatus according to claim 14, wherein each Faraday effect glass has a prism disposed in said light path so that the light emitted from said light source enters into said Faraday effect glass via said prism and the total internally reflected light exits through said prism.