Optical sensor and method of use

• US 9,140,582 B2
• Filed: 05/27/2010
• Issued: 09/22/2015
• Est. Priority Date: 05/27/2009
• Status: Active Grant

• Current Assignee: Silixa Limited
• Original Assignee: Silixa Limited
• Inventors: Farhadiroushan, Mahmoud, Parker, Tom Richard, Shatalin, Sergey
• Primary Examiner(s): Geisel, Kara E
• Assistant Examiner(s): BOLOGNA, DOMINIC JOSEPH
• Application Number:
  US13/322,448
• Publication Number:
  US 20120162639A1
• Time in Patent Office: 1,944 Days
• Field of Search: 356/73.1, 356477-495
• US Class Current: 1/1
• CPC Class Codes: E21B 47/002 by visual inspection
• CPC Class Codes: E21B 47/0025 generating an image of the borehole wall using down-hole measurements, e.g. acoustic or electric
• CPC Class Codes: E21B 47/107 using acoustic means
• CPC Class Codes: G01D 5/35303 using a reference fibre, e.g. interferometric devices
• CPC Class Codes: G01D 5/35306 using an interferometer arrangement
• CPC Class Codes: G01D 5/35325 using interferometer with two arms in reflection, e.g. Mickelson interferometer
• CPC Class Codes: G01D 5/35335 Aspects of emitters or receivers used by an interferometer in an optical fibre sensor arrangement using multiple sensor devices using multiplexing techniques G01D5/35383
• CPC Class Codes: G01D 5/35358 using backscattering to detect the measured quantity
• CPC Class Codes: G01D 5/35364 using inelastic backscattering to detect the measured quantity, e.g. using Brillouin or Raman backscattering
• CPC Class Codes: G01D 5/35377 Means for amplifying or modifying the measured quantity
• CPC Class Codes: G01D 5/35383 using multiple sensor devices using multiplexing techniques
• CPC Class Codes: G01F 1/66 by measuring frequency, phase shift or propagation time of electromagnetic or other waves, e.g. using ultrasonic flowmeters
• CPC Class Codes: G01F 1/661 using light
• CPC Class Codes: G01F 1/662 Constructional details
• CPC Class Codes: G01F 1/666 by detecting noise and sounds generated by the flowing fluid
• CPC Class Codes: G01F 1/667 Arrangements of transducers for ultrasonic flowmeters; Circuits for operating ultrasonic flowmeters
• CPC Class Codes: G01H 9/004 using fibre optic sensors light guides per se G02B6/00, acousto-optical devices specially adapted for gating or modulating in optical wave guides G02F1/125
• CPC Class Codes: G01M 11/085 the optical fiber being on or near the surface of the DUT
• CPC Class Codes: G01M 11/331 by using interferometer
• CPC Class Codes: G01M 3/24 using infrasonic, sonic, or ultrasonic vibrations
• CPC Class Codes: G01M 5/0058 : of elongated objects, e.g. pipes, masts, towers or railways
• CPC Class Codes: G01M 5/0066 : by exciting or detecting vibration or acceleration vibration testing of structures G01M7/00
• CPC Class Codes: G01M 5/0091 : by using electromagnetic excitation or detection
• CPC Class Codes: G01V 1/226 : Optoseismic systems
• CPC Class Codes: G01V 1/40 : specially adapted for well-logging

Abstract

An interferometer apparatus for an optical fiber system and method of use is described. The interferometer comprises an optical coupler and optical fibers which define first and second optical paths. Light propagating in the first and second optical paths is reflected back to the optical coupler to generate an interference signal. First, second and third interference signal components are directed towards respective first, second and third photodetectors. The third photodetector is connected to the coupler via a non-reciprocal optical device and is configured to measure the intensity of the third interference signal component directed back towards the input fiber. Methods of use in applications to monitoring acoustic perturbations and a calibration method are described.

Claims

1. An interferometer apparatus for an optical fibre system, the apparatus comprising:

an optical coupler having an input port and first and second ports coupled to optical fibres which define first and second optical paths;

first and second Faraday rotator mirrors arranged respectively at the ends of the first and second optical paths to reflect light propagating in the first and second optical paths back to the optical coupler to generate an interference signal;

wherein the optical coupler is configured to direct first and second interference signal components of the interference signal respectively to first and second detector ports, and is configured to direct a third interference signal component of the interference signal towards the input port, and the apparatus comprises means for introducing a phase shift between the first, second and third interference signal components;

first and second photodetectors connected to first and second detector ports of the optical coupler and configured to measure an intensity of the first and second interference signal components at respective phase shifts;

a third photodetector connected to a non-reciprocal optical device and configured to measure the intensity of the third interference signal component directed back towards the input port;

an incoherent light source configured to propagate light in the interferometer apparatus; and

calibration circuitry configured to;

determine an electrical offset for each of the photodetectors from the outputs of the photodetectors in a first condition, in which no light is input to the input port and the incoherent light source is switched off so that no light propagates in the interferometer apparatus; and

determine at least one of a photodetector offset, a relative photodetector gain, and a coupling ratio of the first and second optical paths from the outputs of the photodetectors in a second condition, in which the incoherent light source is switched on such that light propagates in the interferometer apparatus.

2. The interferometer apparatus as claimed in claim 1, wherein the means for introducing a phase shill between the first, second and third interference signal components is the optical coupler.

3. The interferometer apparatus as claimed in claim 1, wherein the optical coupler is m×

m optical coupler, where m≧

3.

4. The interferometer apparatus as claimed in claim 1, wherein the non-reciprocal optical device is an optical circulator.

5. The interferometer apparatus as claimed in claim 1, wherein a third output port of the optical coupler is connected to a fourth photodetector.

6. The interferometer apparatus as claimed in claim 1, wherein a third output port of the optical coupler is coupled to an optical fibre defining a third optical path, and the apparatus comprises a third reflector arranged in the third optical path to reflect light propagating in the third optical path back to the optical coupler to generate an interference signal.

7. The apparatus of claim 1, further comprising a bandpass filter arranged to filter the light from the incoherent light source, such that the light propagating in the interferometer apparatus has a bandwidth around the frequency of the light propagating in the first and second optical paths.

8. The apparatus as claimed in claim 1, wherein the light input to the interferometer apparatus has a coherence length shorter than the length of the first and second optical paths of the interferometer apparatus such that substantially no interference signal is detected.

9. The apparatus as claimed in claim 1, further comprising:

an optical amplifier configured to receive transmitted, reflected or backscattered light propagating in the first and second optical paths and output an amplified light signal;

wherein an Amplified Spontaneous Emission (ASE) of the optical amplifier is the incoherent light source.

10. The apparatus as claimed in claim 9, wherein the calibration circuitry operates at least whilst the interferometer apparatus is in a third condition, in which the optical amplifier receives an input light signal from the light some and outputs an amplified light signal.

11. The apparatus as claimed in claim 10, wherein the calibration circuitry operates between optical signal pulses.

12. An Interferometer system comprising a first interferometer apparatus as claimed in claim 1, and a second interferometer apparatus as claimed in claim 1, wherein a third output port of the optical coupler of the first interferometer apparatus is coupled to an input of the second interferometer apparatus.

13. The interferometer system as claimed in claim 12 comprising multiple interferometer apparatuses, wherein respective output ports of a subset of the interferometer apparatuses are utilised as inputs for sequential interferometer apparatuses.

14. The interferometer system as claimed in claim 13 wherein the interferometer apparatuses are cascaded in series and/or in a star configuration.

15. The interferometer system as claimed in claim 14 wherein different interferometer apparatuses have different optical path length differences.

16. An optical fibre system for monitoring an optical signal, the system comprising:

a light source;

an optical fibre deployed in an environment to be monitored and coupled to the light source;

an interferometer apparatus as claimed in claim 1 and configured to receive backscattered or reflected light from the optical fibre;

data capturing means for gathering data output from the photodetectors of the interferometer apparatus.

17. The optical fibre system as claimed in claim 16, further comprising data processing apparatus for processing the data output from the photodetectors to derive an acoustic signal.

18. The optical fibre system as claimed in claim 16, wherein the environment to be monitored is subterranean, a wellbore, or comprises a pipeline.

19. The optical fibre system as claimed in claim 16, wherein the optical fibre is deployed linearly.

20. The optical fibre system as claimed in claim 16, wherein the optical fibre is deployed at least partially in a planar arrangement to provide directional sensing.

21. The optical fibre system as claimed in claim 16, wherein the optical fibre is deployed in a multidimensional array.

22. The optical fibre system as claimed in claim 16, wherein at least a part of the optical fibre is arranged on a surface area in a continuous path without crossing over another part of the fibre.

23. A method of monitoring acoustic perturbations, the method comprising:

providing a light source, an optical fibre deployed in an environment to be monitored and coupled to the light source, and an interferometer configured to receive a pulsed optical signal from the optical fibre, the interferometer comprising at least two optical paths having Faraday rotator mirrors at the ends thereof and at least three photodetectors;

receiving, in the interferometer, backscattered light from the optical fibre, and generating an interference signal in dependence thereon;

introducing a phase shift between first, second, and third interference signal components of the interference signal, and directing the first, second, and third interference signal components to first, second, and third photodetectors respectively;

measuring the intensity of the first, second, and third interference signal components at respective phase shills to provide first intensity data, second intensity data, and third intensity data;

processing the first, second, and third intensity data to determine an optical phase angle of the optical signal to thereby provide optical phase angle data and optical phase angle modulation data and;

identifying acoustic perturbations to which the optical fibre has been exposed from the optical phase angle modulation data;

determining a normalisation factor for at least one of a photodetector offset, a relative photodetector gain, and a coupling ratio of the interferometer optical paths, by inputting light from an incoherent light source to the interferometer and measuring the outputs of the photodetectors;

wherein the determining further comprises;

determining the electrical photodetector offset for each of the photodetectors from the outputs of the photodetectors in a first condition, in which transmitted, reflected or backscattered light propagating through the optical fibre is decoupled from the interferometer and the incoherent light source is switched off so that no light is input to the interferometer; and

determining at least one of the photodetector offset, the relative photodetector gain, and the coupling ratio of the interferometer optical paths from the outputs of the photodetectors in a second condition, in which transmitted, reflected or backscattered light propagating through the optical fibre is decoupled from the interferometer and the incoherent light source is switched on to input light to the interferometer.

24. The method as claimed in claim 23, comprising selecting a spatial resolution interval at which optical phase angle data is desired, and oversampling the outputs of the photodetectors to provide multiple optical phase angle data over the spatial resolution interval.

25. The method as claimed in claim 23, comprising:

providing an optical amplifier configured to receive transmitted, reflected or backscattered light propagating through the fibre and output an amplified light signal to the interferometer; and

utilising the Amplified Spontaneous Emission of the optical amplifier (ASE) as the incoherent light source.

26. The method as claimed in claim 23 comprising:

operating the interferometer in a third condition, in which the optical amplifier receives an input light signal from the light source and outputs an amplified light signal to the interferometer; and

correcting for offsets and normalising the signals detected at the photodetectors using the determined normalisation factor.

27. The method as claimed in claim 23, further comprising;

filtering the light from the incoherent light source using a bandpass titter, such that the light input to the interferometer has a bandwidth around the frequency of light transmitted, reflected or backscattered light propagating through the fibre.

28. The method as claimed in claim 23, wherein the light input to the interferometer has a coherence length shorter than the length of the interferometer optical paths such that substantially no interference signal is detected.

29. The method as claimed, in claim 26, further comprising:

correcting for offsets and normalising the signals detected at the photodetectors between optical signal pulses.