Frequency-scanned optical time domain reflectometry

• US 7,859,654 B2
• Filed: 07/17/2008
• Issued: 12/28/2010
• Est. Priority Date: 07/17/2008
• Status: Active Grant

• Current Assignee: Schlumberger Technology Corporation (SLB)
• Original Assignee: Schlumberger Technology Corporation (SLB)
• Inventors: Hartog, Arthur H.
• Primary Examiner(s): Nguyen; Tu T
• Application Number:
  US12/174,712
• Publication Number:
  US 20100014071A1
• Time in Patent Office: 894 Days
• Field of Search: 356/73.1, 356/477, 356/479, 356/497, 25022711-22727, 385 12- 27, 385114-120
• US Class Current: 356/73.1
• CPC Class Codes: G01D 5/35361 using elastic backscattering to detect the measured quantity, e.g. using Rayleigh backscattering
• 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 11/3127 using multiple or wavelength variable input source

Abstract

A frequency-scanned optical time domain reflectometry technique includes launching a plurality of interrogating pulses into an optical fiber at a plurality of optical carrier frequencies. A Rayleigh backscatter signal is detected for each interrogating pulse as a function of time between the launching of the pulse and the detection of the backscatter signal. The time resolved Rayleigh backscatter signal at each optical frequency may then be examined to determine a distribution of a physical parameter along the length of the optical fiber.

Claims

1. A method of determining a physical parameter associated with an optical fiber, comprising:

launching a plurality of interrogating pulses into the optical fiber, wherein at least a first interrogating pulse has a first optical frequency and a second interrogating pulse has a second optical frequency different than the first optical frequency;

acquiring, for each of the plurality of interrogating pulses, time resolved Rayleigh backscatter signals at a plurality of locations along at least a portion of the length of the optical fiber;

comparing the time resolved Rayleigh backscatter signals from the first plurality of interrogating pulses with the time resolved Rayleigh backscatter signals from the second plurality of interrogating pulses; and

based on the comparing, determining a distribution of a first physical parameter along at least the portion of the length of the optical fiber.

2. The method as recited in claim 1, further comprising:

storing in a memory a signature of the optical fiber, the signature corresponding to time resolved Rayleigh backscatter signals as a function of optical frequency at the plurality of locations along at least the portion of the length of the optical fiber while the optical fiber is in a known physical state.

3. The method as recited in claim 2, wherein determining the distribution of the first physical parameter comprises determining a frequency shift required for the acquired time resolved Rayleigh backscatter signals to substantially align with the stored signature.

4. The method as recited in claim 1, further comprising adjusting the optical carrier frequency in a plurality of steps over a frequency range.

5. The method as recited in claim 4, wherein the steps are uniform.

6. The method as recited in claim 1, wherein the second interrogating pulse is adjacent in time to the first interrogating pulse.

7. The method as recited in claim 1, wherein the first and second interrogating pulses are launched simultaneously.

8. The method as recited in claim 1, further comprising determining a distribution of a second physical parameter along the length of the optical fiber, wherein the second physical parameter is different than the first physical parameter.

9. The method as recited in claim 8, further comprising detecting Raman scattering in response to an interrogating pulse, wherein determining the distribution of the second physical parameter is based on the detected Raman scattering.

10. The method as recited in claim 8, further comprising detecting Brillouin scattering in response to an interrogating pulse, wherein determining the distribution of the second physical parameter is based on the detected Brillouin scattering.

11. The method as recited in claim 8, wherein the optical fiber is a birefringent fiber having a first axis and a second axis, and wherein determining the distribution of the first physical parameter is based on a first plurality of time resolved Rayleigh backscatter signals produced along the first axis at a plurality of optical frequencies, and wherein determining the distribution of the second physical parameter is based on a second plurality of time resolved Rayleigh backscatter signals produced along the second axis at a plurality of optical frequencies.

12. The method as recited in claim 11, further comprising:

providing the optical fiber in a well; and

determining a flow profile of the well based on the distributions of the first and second physical parameters.

13. The method as recited in claim 12, wherein the first physical parameter is pressure and the second physical parameter is temperature.

14. The method as recited in claim 1, wherein acquiring the time resolved Rayleigh backscatter signals comprises coherently detecting the Rayleigh backscattered produced by the optical fiber in response to the first and second interrogating pulses.

15. A system, comprising:

an optical fiber;

an optical source to output an optical pulse at each of a plurality of optical frequencies for launching into the optical fiber; and

a detection and acquisition system coupled to the optical fiber and configured to;

detect Rayleigh backscatter corresponding to each launched optical pulse as a function of time;

based on the detected Rayleigh backscatter, acquire a time resolved coherent Rayleigh spectra (TRCRS) measurement corresponding to each of the optical frequencies;

save at least one of the time resolved coherent Rayleigh spectra (TRCRS) measurements as a baseline;

compare the time resolved Rayleigh coherent spectra (TRCRS) corresponding to given optical frequencies to the baseline; and

determine a distribution of a physical parameter along a length of the fiber based on the TRCRS measurement comparison at each of the plurality of optical frequencies.

16. The system as recited in claim 15, further comprising a memory to store a signature of the optical fiber, the signature corresponding to Rayleigh backscatter along the length of the optical fiber as a function of optical frequency while the optical fiber is in a known state.

17. The system as recited in claim 16, wherein the detection and acquisition system is configured to determine the physical parameter based on a comparison between the stored signature and the TRCRS measurement at each of the optical frequencies.

18. The system as recited in claim 15, wherein the detection and acquisition system is configured to coherently detect the Rayleigh backscatter.

19. The system as recited in claim 18, wherein the optical source is configured to output the optical pulse at each of the plurality of optical frequencies for launching simultaneously into the optical fiber.

20. The system as recited in claim 15, wherein the detection and acquisition system is configured to detect a phase and an intensity of the Rayleigh backscatter.

21. The system as recited in claim 15, wherein the optical fiber is a birefringent fiber having a plurality of axes, and wherein the detection and acquisition system is configured to detect the Rayleigh backscatter produced along each of the axes.

22. The system as recited in claim 21, wherein the optical fiber is disposed in a well, and wherein the detection and acquisition system is further configured to determine a distribution of a first physical parameter based on the detected Rayleigh backscatter produced along a first axis of the birefringent fiber and a distribution of a second physical parameter based on the detected Rayleigh backscatter produced along a second axis of the birefringent fiber.

23. The system as recited in claim 22, wherein the first physical parameter is pressure, and the second physical parameter is temperature.

24. The system as recited in claim 23, wherein the detection and acquisition system is further configured to determine a flow profile of the well based on the distribution of the first and second physical parameters.

25. A method of determining a physical parameter associated with an optical fiber, comprising:

providing a signature of the optical fiber, the signature corresponding to time resolved coherent Rayleigh spectra measurements taken along at least a portion of the optical fiber at a plurality of optical frequencies;

launching a plurality of interrogating pulses into the optical fiber, wherein at least a first interrogating pulse has a first optical frequency and a second interrogating pulse has a second optical frequency different than the first optical frequency;

acquiring, for each of the plurality of interrogating pulses, time resolved Rayleigh backscatter spectra at a plurality of locations along at least a portion of the length of the optical fiber;

comparing the acquired time resolved Rayleigh backscatter spectra to the signature; and

based on the comparing, determining a distribution of a physical parameter along at least the portion of the length of the optical fiber.

26. The method as recited in claim 25, further comprising coherently detecting Rayleigh backscatter produced by the optical fiber in response to each of the interrogating pulses.

27. The method as recited in claim 26, wherein the plurality of interrogating pulses are launched into the optical fiber simultaneously.

28. The method as recited in claim 26, wherein the plurality of interrogating pulses are launched into the optical fiber sequentially.

29. The method as recited in claim 25, wherein each launched interrogating pulse is adjacent in time to the previously launched interrogating pulse.

30. The system as recited in claim 25, further comprising:

providing the optical fiber in a well; and

determining a flow profile of the well based on the distribution of the physical parameter.