Fiber-optic current sensor with polarimetric detection scheme

• US 7,692,420 B2
• Filed: 10/22/2008
• Issued: 04/06/2010
• Est. Priority Date: 04/25/2006
• Status: Expired due to Fees

• Current Assignee: ABB Power Grids Switzerland AG (Hitachi, Ltd.)
• Original Assignee: ABB Research Ltd. (ABB Limited)
• Inventors: Brandle, Hubert, Frank, Andreas, Bohnert, Klaus
• Primary Examiner(s): Nguyen; Ha Tran T
• Assistant Examiner(s): Vazquez; Arleen M
• Application Number:
  US12/256,289
• Publication Number:
  US 20090039866A1
• Time in Patent Office: 531 Days
• Field of Search: 324 96- 97, 324/753, 250/225, 356/72, 359/281, 385/12
• US Class Current: 324/96
• CPC Class Codes: G01R 15/246 based on the Faraday, i.e. linear magneto-optic, effect

Abstract

The current in a conductor is measured by exploiting the Faraday effect in a sensing fiber. The light returning from the sensing fiber is split into at least two parts, at least one of which is analyzed by a first circular analyzer for generating a first signal. A second part may e.g. be analyzed by a second circular analyzer, and a third part may be analyzed by a linear analyzer. By combining the signals obtained in this way, the current induced phase delay in the returning light can be measured efficiently and accurately.

Claims

1. A method for measuring a current comprising the steps of

sending left and right circularly polarized light waves at least once along a sensing fiber extending around said current,

passing said right and left circularly polarized light waves through an optical retarder for generating two orthogonally linearly polarized returning light waves,

sending a first part of said returning light waves to a first detector, a second part of said returning light waves to a second detector, characterized by the step of

sending a third part of said returning light waves to a third detector, wherein said first part of said returning light is passed through a first circular analyzer before impinging on said first detector, wherein said second part of said returning light waves is passed through a second circular analyzer before impinging on said second detector and having a polarization opposite to said first circular analyzer, and wherein said third part of said returning light waves is passed through a linear analyzer before impinging on said third detector,

wherein said first detector generates a signal I₊ and said second detector generates a signal I₋

and said third detector generates a signal I_L, and knowledge of the three signals I₊, I₋

, I_L allows to obtain the current even if the values for fringe visibility V and arriving optical power I₀ are not known in advance.

2. The method of claim 1, said method further comprising the step of calculating

S=(I₊−

I₋

)/(I₊+I₋

)

and the step of calculating

I_L/(I₊+I₋

).

3. The method of claim 2, wherein

S=V·

sin(Δ

φ

),

with Δ

φ

being a phase shift introduced by Faraday-effect between said circularly polarized light waves in said sensing fiber and V describing an interference fringe visibility, wherein said method comprises the step of calculating Δ

φ

from said signals I_L, I₊ and I₋

.

4. The method of claim 3, wherein the signal

S′

=I_L/(I₊+I₋

),

is used to compensate the signal S for variations in fringe visibility V.

5. The method of claim 1, further comprising the step of estimating a temperature at said retarder, or a correction factor depending on said temperature, from said signals.

6. The method of claim 5, wherein said retarder has a phase shift not equal to 90°

and/or wherein said temperature and/or said correction factor is estimated from I_L/(I₊+I₋

), where I_L is a signal generated by said third detector.

7. The method of claim 1, wherein said retarder has a phase shift equal to 90°

+ε

, with ε

being a non-zero deviation, wherein said deviation is chosen such that cos ε

·

Δ

φ

becomes independent of temperature, with Δ

φ

being a phase shift introduced between the right and left circularly polarized light waves in said fibers.

8. The method of claim 6, wherein a deviation ε

of the retarder from π

/2 is present and the signal

I_L′

=I_L/(I₊+I₋

)=(1+cos²ε

),

is calibrated so that it becomes a measure for the temperature.

9. The method of claim 8, wherein the signal I_L is determined at the zero-crossings of an alternating current.

10. The method of claim 1, wherein said first and/or second circular analyzer is comprised of a quarter wave retarder and a linear analyzer.

11. The method of claim 1, wherein said returning light waves are passed through an integrated optics device comprising at least one splitter for generating said first and said second part, and in particular at least two beam splitters.

12. The method of claim 11, wherein said integrated optics device comprises at least one integrated quarter-wave retarder cooperating with at least one external linear polarizer for forming said circular analyzer.

13. The method of claim 1, wherein said third part of said returning light waves is not passed through a linear analyzer before impinging on said third detector, and the signal I_L generated at said third detector equals I₀, which is proportional to the arriving optical power.

14. The method of claim 1, wherein for small currents

I₊=I₀(1+V·

Δ

φ

),

I₋

=I₀(1−

V·

Δ

φ

),

and for alternating currents, the ac and dc components of the signals I₊ and I₋

are extracted in a signal processor and the quotient of the ac and dc components gives a signal V·

Δ

φ

proportional to the wave form of the current and independent of variations in the light intensity.

15. The method of claim 1, wherein no ac phase modulators are present.

16. A method for measuring a current comprising the steps of

sending left and right circularly polarized light waves at least once along a sensing fiber extending around said current,

passing said right and left circularly polarized light waves through an optical retarder for generating two orthogonally linearly polarized returning light waves,

sending a first part of said returning light waves to a first detector, characterized by the step of

passing said first part of said returning light through a first circular analyzer before impinging on said first detector,

passing a further part of said returning light waves through a linear analyzer before impinging on a further detector,

wherein said first detector generates a signal I₊ or I₋

and said further detector generates a signal I_L,

and knowledge of the two signals I₊ or I₋

and I_L allows to eliminate an arriving optical power I₀ and to calculate the phase shift Δ

φ

assuming that a fringe visibility V is known or has been measured in different manner.

17. The method of claim 16 comprising the step of dividing I₊ by I_L

I₊/I_L=(1+V·

sin(Δ

φ

))/(1+V).