Bragg grating temperature/strain fiber sensor having combination interferometer/spectrometer output arrangement

• US 6,137,565 A
• Filed: 05/06/1999
• Issued: 10/24/2000
• Est. Priority Date: 05/15/1998
• Status: Expired due to Fees

• Current Assignee: Institut Fuer Physikalische Hochtechnologie E.V., Jenoptik AG
• Original Assignee: Jenoptik AG
• Inventors: Belke, Siegfried, Goerlich, Steffen, Ecke, Wolfgang
• Primary Examiner(s): Turner, Samuel A.
• Application Number:
  US09/306,533
• Time in Patent Office: 537 Days
• Field of Search: 356/32, 356/35.5, 356/345, 356/346, 250/227.19, 250/227.27, 385/12, 385/14
• US Class Current: 356/35.5
• CPC Class Codes: G01D 5/35316 using a Bragg gratings
• 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: G01J 5/60 using determination of colour temperature
• CPC Class Codes: G01K 11/3206 at discrete locations in the fibre, e.g. using Bragg scattering

Abstract

An arrangement for simultaneous optical determination of temperature and strain fluctuations in an optical fiber for precisely determining the changes in environmental influences and/or fiber loads is disclosed. The arrangement performs two different measurement tasks of the absolute measurement of a stationary quantity, such as temperature and the relative, high-resolution measurement of quickly varying quantities of fluctuation processes with comparable accuracy in a single optical The arrangement which is achieved using a spectrometer with an imaging, spectrally dispersive element, a first input light bundle being arranged with reference to the dispersive element such that the light spectrally dispersed at the dispersive element is projected onto a first linear receiver The arrangement, and an additional second input light bundle is directed onto the dispersive element in the spectrometer, whose spectrally dispersed light falls onto a second linear receiver The arrangement, parallel to the first one, the two input light bundles are fed light from a broadband light source which has been reflected by at least two optical fiber gratings with different mean wavelengths, and an interferometer The arrangement with phase modulation and different arm lengths is present at least in the light path of the second input light bundle upstream of the spectral dispersion by means of the dispersive element, whose evaluation is performed via the second receiver. The arrangement by means of phase modulation modules with reference to relative changes in the Bragg wavelengths, while a CCD evaluation module for determining the absolute Bragg wavelengths of the optical fiber gratings is arranged downstream of the first receiver The arrangement.

Claims

1. An arrangement for optically determining an absolute physical state variable in an optical fiber with the aid of an optical spectral analyzer for determining different Bragg wavelengths of fiber gratings which have different mean wavelengths and at which the light traversing the optical fiber is reflected, as well as means for calculating the absolute physical quantity from the determined Bragg wavelengths, comprising:

an optical spectral analyzer in the form of a spectrometer having an imaging, spectrally dispersive element;

a first linear receiver arrangement;

a first input light bundle being arranged with reference to said dispersive element such that the light spectrally dispersed at said dispersive element is projected onto said first linear receiver arrangement;

a second linear receiver arrangement;

an additional second input light bundle being directed onto said dispersive element in said spectrometer, whose spectrally dispersed light falls onto said second linear receiver arrangement, parallel to the first one;

a broadband light source;

said two input light bundles being fed light from said broadband light source which has been reflected by at least two optical fiber gratings with different mean wavelengths;

an interferometer arrangement with phase modulation and different arm lengths being present at least in the light path of the second input light bundle upstream of the spectral dispersion by said dispersive element;

said interferometer arrangement having an evaluation section which is arranged downstream of said second receiver arrangement assigned to said input light bundle;

a signal processing module for determining the absolute Bragg wavelengths of the optical fiber gratings and for calculating a physical variable dependent thereon being connected downstream of said first receiver arrangement; and

phase demodulation modules arranged downstream of said second receiver arrangement being provided for evaluating interferometer signals for determining relative changes in the Bragg wavelengths of the optical fiber gratings, and for calculating the relative changes in a physical quantity.

2. The arrangement according to claim 1, wherein, for a selected measurement, task determination of the temperature is provided as the absolute physical quantity, and determination of strain fluctuations in the optical fiber is provided as the variable relative quantity.

3. The arrangement according to claim 1, wherein the optical fiber gratings are arranged inside the optical fiber which function as a measuring point.

4. The arrangement according to claim 1, wherein the imaging dispersive element is a prism.

5. The arrangement according to claim 1, wherein the imaging dispersive element is an imaging reflection grating.

6. The arrangement according to claim 1, wherein a Mach-Zehnder interferometer with two outputs is present as interferometer arrangement, the first and the second input light bundles of the spectrometer being formed in each case by one of the outputs of the Mach-Zehnder interferometer.

7. The arrangement according to claim 1, wherein the interferometer arrangement is a Michelson interferometer which is arranged in the light path of the second input light bundle downstream of a splitting of the light from the optical fiber onto the input light bundles of the interferometer.

8. The arrangement according to claim 1, wherein the interferometer arrangement is a Michelson interferometer whose conventional output is applied via a splitter to the second input light bundle of the spectrometer, and whose existing light path is branched outside the interferometer arms in order to be fed as first input light bundle to the spectrometer.

9. The arrangement according to claim 1, wherein the interferometer arrangement is a Michelson interferometer whose light path branches in a two-fold fashion at the input of the Michelson interferometer, a first splitter being present to create a direct light path to the first input light bundle of the spectrometer, and a second light path to a second splitter, which is provided for the purpose of splitting the second light path into two interferometer arms as well as, after reflection of the light in the interferometer arms, of combining an outcoupling onto a third light path to the second input light bundle of the spectrometer.

10. The arrangement according to claim 1, wherein the interferometer arrangement is a set-up using free-beam optics as mirror elements, a mechanical displacing unit being provided as phase modulator for periodically changing the optical path length of an interferometer arm by a mirror displacement.

11. The arrangement according to claim 10, wherein the free-beam optical system is constructed as a Mach-Zehnder interferometer and is integrated in the spectrometer, and the outputs of the Mach-Zehnder interferometer constitute the input light bundles.

12. The arrangement according to claim 1, wherein the interferometer arrangement is constructed from optical fibers and fiber couplers as optical splitters.

13. The arrangement according to claim 12, wherein the optical fibers are monomode fibers.

14. The arrangement according to claim 1, wherein the interferometer arrangement contains an optical phase modulator at least in one interferometer arm.

15. The arrangement according to claim 14, wherein an electro-optical modulator is used as phase modulator.

16. The arrangement according to claim 15, wherein the phase modulator can be driven by two-frequency sine-wave modulation and can be evaluated on a common multiple of the two modulation frequencies.

17. The arrangement according to claim 14, wherein one phase modulator each is arranged in the two interferometer arms, the phase modulators being piezoelectric fiber stretchers for implementing a symmetric basic set up of the interferometer arms, and one phase modulator is driven in push-pull fashion relative to the other phase modulator.

18. The arrangement according to claim 1, wherein the first receiver arrangement is a CCD row.

19. The arrangement according to claim 1, wherein the second receiver arrangement is adapted in number, position and width of the light entrance surfaces of its elements to the reflections of the different optical fiber gratings, account additionally being taken in this case of the expected fluctuation widths, dependent on the measured quantity, of the wavelengths of the fiber grating reflections.

20. The arrangement according to claim 19, wherein the second receiver arrangement is a photodiode array with a specifically produced distribution and size of the light-sensitive elements.

21. The arrangement according to claim 19, wherein the second receiver arrangement is a photodiode array with a regular distribution and size of the light-sensitive elements, only specific elements being used to evaluate the fiber grating reflections.

22. The arrangement according to claim 19, wherein optical fibers for launching the fiber grating reflections onto the second receiver arrangement are present for the purpose of adaptation to the conditions of the fiber grating reflections, optical fibers being adapted with their diameters and spacings to the number, position and magnitude of the fiber grating reflections, and the light entrance surfaces of the fibers being arranged in the receiver plane prescribed by the imaging reflection gratings, and their light exit surfaces being directed onto an arbitrarily positioned linear photodiode array.

23. The arrangement according to claim 22, wherein the second receiver row is a row with regularly arranged elements.

24. The arrangement according to claim 23, wherein the second receiver row is a regular photodiode row.