Fluid analysis system based on integrated computing element technology and fiber Bragg grating radiometry

Patent metadata

Field	Value
Publication number	US-10801865-B2
Application number	US-201616068089-A
Country	US
Kind code	B2
Filing date	Feb 2, 2016
Priority date	Feb 2, 2016
Publication date	Oct 13, 2020
Grant date	Oct 13, 2020

Abstract

A device for fluid analysis including an integrated computational element (ICE), a sample cell that optically interacts the ICE with a sample to generate a computation light associated with a characteristic of the sample, and a fiber sensor that receives the computation light and converts the computation light into a heat, is provided. The fiber sensor is coupled with a detector through an optical link, and is configured to return a portion of probe light through the optical link to the detector based on the heat converted. A method for using the device for performing fluid analysis is provided. A system for fluid analysis including at least one device as above is also provided.

First claim

The invention claimed is:

1. A device, comprising:
an integrated computational element (ICE);
a sample cell that optically interacts the ICE with a sample to generate computation light associated with a characteristic of the sample; and
a fiber sensor that receives the computation light and converts the computation light into heat, the fiber sensor being communicably coupled with a detector through an optical link and configured to return a portion of probe light through the optical link to the detector according to the heat converted.

2. The device of claim 1 , wherein an intensity of the computation light is proportional to the characteristic of the sample.

3. The device of claim 1 , wherein the probe light is selected from one of a plurality of telecommunications wavelength bands.

4. The device of claim 1 , wherein the ICE includes a plurality of alternating layers of two materials having different indices of refraction, each of the layers of material having a selected thickness so that an intensity of the computation light is proportional to the characteristic of the sample.

5. The device of claim 1 , wherein the fiber sensor includes a fiber Bragg grating (FBG) that returns the portion of the probe light, and wherein the FBG includes a core that is thermally coupled to a sensitive coating that absorbs the computation light.

6. The device of claim 5 , wherein the FBG is a first FBG and the fiber sensor includes a second FBG configured to return a second portion of the probe light based on an environmental condition of the fiber sensor.

7. The device of claim 5 , wherein the sensitive coating absorbs the computation light and transmits the heat to the core.

8. The device of claim 5 , wherein the sensitive coating comprises a material that is an absorber in a near infrared (NIR) spectral domain.

9. The device of claim 5 , wherein the returned portion of the probe light has a center wavelength related to the heat received by the sensitive coating.

10. The device of claim 1 , wherein the ICE provides a modified light from an illumination source and the modified light optically interacts with the sample in the sample cell to generate the computation light.

11. The device of claim 1 , wherein the ICE provides the computation light from the optical interaction of an illumination source with the sample in the sample cell.

12. A system, comprising:
a probe light source that generates and emits a probe light;
a detector;
an optical link to transmit the probe light; and
an optical computing device, comprising:
an integrated computational element (ICE);
a sample cell that optically interacts the ICE with a sample to generate computation light associated with a characteristic of the sample; and
a fiber sensor that converts the computation light into heat, the fiber sensor being communicably coupled to the detector through the optical link and configured to return a portion of the probe light through the optical link to the detector according to the heat converted.

13. The system of claim 12 , wherein the probe light source generates the probe light in a wavelength range included in at least one of a plurality of telecommunication bands.

14. The system of claim 12 , wherein the probe light source is one of a continuous laser, a pulsed laser, a tunable laser, and a broadband light source.

15. The system of claim 12 , further comprising a plurality of optical computing devices distributed in a network communicably coupled with each other via the optical link.

16. The system of claim 12 , wherein the fiber sensor comprises a sensitized fiber Bragg grating (FBG) that is thermally coupled with a sensitive coating that absorbs and converts the computation light into the heat.

17. A method, comprising:
providing probe light to an optical waveguide communicably coupled to an optical link;
optically interacting illumination light with an integrated computational element and a sample to generate computation light associated with a characteristic of a sample;
converting the computation light to heat generated by a coating disposed in a fiber sensor located along the optical link;
reflecting, in the fiber sensor, a portion of the probe light according to the heat generated by the coating; and
determining a value for the characteristic of the sample based on the reflected portion of the probe light.

18. The method of claim 17 , further comprising reflecting a second portion of the probe light at a wavelength according to an environmental condition of the fiber sensor.

19. The method of claim 17 , further comprising determining a wavelength shift of the reflected portion of the probe light, wherein determining the value for the characteristic of the sample includes finding the value for the characteristic of the sample in a table associating the wavelength shift of the reflected portion of the probe light with the value of the characteristic of the sample.

20. The method of claim 17 , wherein determining the value for the characteristic of the sample based on the reflected portion comprises comparing a wavelength shift of the reflected portion in the presence of the illumination light with the wavelength shift of the reflected portion in the absence of the illumination light.

21. The method of claim 17 , further comprising modifying a wellbore operation based on the value for the characteristic of the sample.

22. The method of claim 17 , further comprising modifying a fluid flow parameter based on the value for the characteristic of the sample.

23. The method of claim 17 , wherein reflecting in the fiber sensor a portion of the probe light comprises reflecting a portion of the probe light from a long period grating formed along the optical link.

24. The method of claim 17 , wherein reflecting in the fiber sensor a portion of the probe light comprises reflecting a portion of the probe light from an extrinsic Fabry-Pérot interferometer optically coupled to the optical link.

25. The method of claim 17 , wherein determining a value for the characteristic of the sample comprises measuring a change in a property of the reflected portion of the probe light selected from the group consisting of a power, a phase, and a state of polarization.

Assignees

• Halliburton Energy Services Inc

Inventors

• Leblanc Michel Joseph
• Perkins David L
• Lan Xinwei

Classifications

• G01N21/31

  Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry {(G01N21/72 takes precedence)} · CPC title

• G01D5/35316 Primary

  using a Bragg gratings · CPC title

• G02B2006/12138

  Sensor · CPC title

• E21B49/08

  Obtaining fluid samples or testing fluids, in boreholes or wells · CPC title

• G02B6/02076

  Refractive index modulation gratings, e.g. Bragg gratings · CPC title