EP2279397A1 - Dispositif de mesure de temperature a resolution spatiale - Google Patents

Dispositif de mesure de temperature a resolution spatiale

Info

Publication number
EP2279397A1
EP2279397A1 EP09745482A EP09745482A EP2279397A1 EP 2279397 A1 EP2279397 A1 EP 2279397A1 EP 09745482 A EP09745482 A EP 09745482A EP 09745482 A EP09745482 A EP 09745482A EP 2279397 A1 EP2279397 A1 EP 2279397A1
Authority
EP
European Patent Office
Prior art keywords
polarization
optical fiber
laser light
light
light source
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Ceased
Application number
EP09745482A
Other languages
German (de)
English (en)
Inventor
Wieland Hill
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Luna Innovations Germany GmbH
Original Assignee
Lios Technology GmbH
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Lios Technology GmbH filed Critical Lios Technology GmbH
Publication of EP2279397A1 publication Critical patent/EP2279397A1/fr
Ceased legal-status Critical Current

Links

Classifications

    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01K—MEASURING TEMPERATURE; MEASURING QUANTITY OF HEAT; THERMALLY-SENSITIVE ELEMENTS NOT OTHERWISE PROVIDED FOR
    • G01K11/00—Measuring temperature based upon physical or chemical changes not covered by groups G01K3/00, G01K5/00, G01K7/00 or G01K9/00
    • G01K11/32—Measuring temperature based upon physical or chemical changes not covered by groups G01K3/00, G01K5/00, G01K7/00 or G01K9/00 using changes in transmittance, scattering or luminescence in optical fibres

Definitions

  • the present invention relates to a device for spatially resolved temperature measurement according to the preamble of claim 1.
  • a device of the aforementioned type is known, for example, from EP 0 692 705 A1.
  • Fiber optic temperature measuring systems
  • DTS distributed Temperature Sensing - DTS
  • the effect of Raman scattering can be used.
  • the radiation of a narrow-band source of electromagnetic radiation eg that of a laser
  • the radiation of a narrow-band source of electromagnetic radiation is inelastic in the
  • Fiber material scattered The ratio of the intensities of the scattered radiation with shorter wavelength than the excitation (anti-Stokes scattered radiation) and the scattered radiation at longer wavelength (Stokes scattered radiation) is temperature-dependent and can be used for temperature determination.
  • Optical Frequency techniques Optical Frequency Domain Reflectometry - OFDR
  • pulse techniques Optical Time Domain Reflectometry - OTDR
  • temperature measuring systems can be used, for example, for fire monitoring in tunnels and canals, for monitoring power cables and pipelines, and in oil and gas production.
  • a DTS device In addition to the corresponding coupling optics, a DTS device generally contains the following essential optical components:
  • a laser light source A laser light source,
  • a spectral divider for coupling the light of the laser light source in the optical fiber used for the measurement and for separating the Raman scattered light components of the laser light scattered back from the optical fiber
  • a DTS device can be largely constructed as a free-form optic.
  • fiber optic structures are often used.
  • a problem of spatially resolved temperature measurement in optical fibers is the change in polarization along the fiber. This occurs especially, but not exclusively, in single-mode fibers.
  • the stimulating radiation is usually polarized. Since the Raman scattering can also be polarized, the Raman scattered light components returning from the fiber can also be polarized. Detection of Raman scattered light may be accomplished using spectral splitters, filters, and others polarization-dependent components. The result of the measurement can thus depend on the polarization.
  • the plane of polarization can be rotated or the polarization otherwise altered by effects such as stress birefringence.
  • the measurement signals depend not only in the desired manner on the local temperature, but also on the local polarization at the measuring point or the
  • the problem underlying the present invention is to provide a device of the type mentioned, with a higher temperature resolution and / or spatial resolution can be achieved.
  • the device comprises means for reducing polarization-related effects.
  • the influence of the polarization effects described can be reduced such that the temperature resolution and / or the
  • the means for reducing polarization-related effects comprise a polarization modifier which can at least partially depolarize the light of the at least one laser light source prior to coupling into the optical fiber or temporally and / or spatially change the polarization state of the light prior to the coupling.
  • the polarization modifier should influence the polarization of the laser light or possibly also of the scattered light in such a way that the polarization dependence of components such as spectral divider and
  • the desired polarization independence of detection does not necessarily require actual depolarization. Rather, it is also possible to use polarization modifiers which temporally and / or spatially change the polarization state and thus lead to an averaging of different polarization components in the detection.
  • Polarization modifier works as follows:
  • Delay distance must be greater than the coherence length so as not to get back polarized light behind the depolarizer. Since large delay lines affect spatial resolution, there may be limitations in using in high-resolution devices. For high-resolution devices other solutions come, for example using rotating optically active disks (half-wavelength plates), electroactive cells for changing the polarization or mechanically stressed optical fibers in question, which can cause a change in the polarization due to the mechanical stress due to induced birefringence.
  • a polarization modifier can be largely constructed as a free-beam optic.
  • Reduction of polarization-related effects comprise at least one filter whose properties, in particular with regard to its transmission, differ by less than 10%, in particular less than 5%, preferably less than 1%, for two or for each two mutually perpendicular polarization directions.
  • the means for reducing polarization-related effects comprise at least one spectral divider whose properties, in particular with regard to its transmission and / or its reflection, are perpendicular to one another or to each other
  • Polarization directions differ by less than 10%, in particular less than 5%, preferably less than 1%.
  • Spectral splitters and other wavelength-selective filters can be used in your
  • One way to reduce the polarization dependence of thin film filters is to use special layer designs that have very similar characteristics for both wavelengths at the wavelengths in question.
  • Another way is to use small angles of incidence.
  • the filters work polarization independent.
  • polarization effects may be sufficiently small to permit accurate measurement of the temperature with a device according to the invention.
  • Fig. 1 is a schematic view of a first embodiment of a device according to the invention
  • Fig. 2 shows an exemplary embodiment of a polarization modifier
  • FIG. 3 shows a detail of a schematic view of a second embodiment of a device according to the invention.
  • Fig. 4 is a schematic view of a third embodiment of a device according to the invention.
  • the device comprises a laser light source 2 controlled by drive means 1.
  • the light 3 of the laser light source 2 passes through a polarization modifier 4, which can depolarize the light 3 or temporally and / or spatially change the polarization state of the light 3. After passing through the polarization modifier 4, which can depolarize the light 3 or temporally and / or spatially change the polarization state of the light 3. After passing through the polarization modifier 4, which can depolarize the light 3 or temporally and / or spatially change the polarization state of the light 3.
  • Polarisationsver the light 3 via coupling means comprising a spectral divider 5 and, for example, a lens 6, coupled into an optical fiber 7 used for temperature measurement.
  • the lens 6 and the spectral divider 5 also serve as decoupling means and can scatter the backscattered in the optical fiber 7 parts of from the laser light source 2 generated light 3 schematically indicated evaluation 8 perform.
  • the evaluation means 8 comprise for example a spectral divider 9 for the laser wavelength and the Raman radiation and two detectors 10, 1 1 for the Stokes and the anti-Stokes scattered radiation, in front of which non-imaged filters are arranged.
  • the evaluation means 8 additionally comprise a measurement electronics 12.
  • the filters may have a structure that provides similar transmission characteristics for mutually perpendicular linear polarizations.
  • the transmission can differ by less than 1%, for example, for a Raman wavelength to be detected for two or for each two mutually perpendicular polarization directions. This minimizes the polarization-dependent influence of the filters on the temperature measurement.
  • the spatially resolved temperature measurement in the optical fiber 7 can be effected by a method which corresponds to the OFDR method as described in EP 0 692 705 A1.
  • the light 3 of the laser light source 2 can be frequency-modulated and a Fourier transformation can be carried out in the evaluation means 8.
  • a connection 34 between the drive means 1 of the laser light source 2 and the measuring electronics 12 can be seen. This connection is used to synchronize laser light source 2 and measuring electronics 12.
  • a polarization modifier 4 comprises a polarization beam splitter 13 and two Faraday mirrors 14, 15, each consisting of a mirror and a polarization rotator.
  • Polarization rotors may be a 45 ° Faraday rotator or a quarter wavelength plate.
  • the light 3 of the laser light source 2 strikes the polarization beam splitter 13 from the left in FIG. 2.
  • the light 2 should have a linear polarization 16 which is at an angle of 45 ° to the parallel and to the vertical polarization or to a vertical direction in FIG 2 is aligned.
  • a first portion 17 of the light 3 is reflected upward.
  • This first portion 17 has a polarization 18 which corresponds to a parallel polarization.
  • a second portion 19 of the light 3 is allowed to pass unimpeded by the polarization beam splitter 13.
  • This second portion 19 has a polarization 20 which corresponds to a vertical polarization.
  • the first portion 17 is reflected downward in Fig. 2, wherein its polarization is rotated by 90 ° so that it is present as a perpendicular polarization 21.
  • the second portion 19 is reflected to the left in Fig. 2, wherein its polarization is also rotated by 90 °, so that it is present as a parallel polarization 22.
  • the two parts 17, 19 are in the renewed impact on the
  • Polarization beam splitter 13 of this unites and step down in Fig. 2 from this.
  • the optical path of the first portion 17 of the polarization beam splitter 13 via the first Faraday mirror 14 back to the Polarization beam splitter 13 is shorter than the optical path of the second portion 19 of the polarization beam splitter 13 via the second Faraday mirror 15 back to the polarization beam splitter 13. This is in particular a greater distance between the polarization beam splitter 13 and the second Faraday mirror
  • the resulting optical path difference of the components 17, 19 should be greater than the coherence length of the light 3.
  • Beam splitter 13 emerging light 23 (see also Fig. 1) both a portion of vertical polarization 24 and a proportion of parallel polarization 25, which are not coherent to each other. This results in the ideal case, a depolarization of the light 23rd
  • the polarization modifier 4 shown in FIG. 2 is one of many possible examples. These and other examples of useful polarization modifiers are disclosed in US 2007/0297054.
  • FIG. 3 shows a spectral divider 26 which can be used, for example, instead of the spectral divider 5 in FIG.
  • the spectral divider 26 can be used, for example, instead of the spectral divider 5 in FIG.
  • the spectral divider 26 can be used, for example, instead of the spectral divider 5 in FIG.
  • the spectral divider 26 can be used, for example, instead of the spectral divider 5 in FIG.
  • the spectral divider 26 is tilted at an angle ⁇ of less than 10 ° with respect to the vertical 27 in FIG. As a result, the angle of incidence at which the light 3 impinges on the spectral divider 26 is smaller than 10 °.
  • the portions 28 of the light 3 scattered back from the optical fiber 6 are reflected by the spectral divider 26 at an angle 2 ⁇ and coupled into an optical fiber 29, which can supply the components to be detected 28 to the evaluation means 8. Due to the almost perpendicular incidence on the spectral divider 26, this latter functions largely independent of polarization.
  • the from Fig. 4 apparent embodiment of a device according to the invention comprises in addition to a first laser light source 2, a second laser light source 30, which is also controlled by the drive means 1.
  • the two laser light sources 2, 30 have a different polarization, in particular a mutually perpendicular linear polarization and are not coherent with each other.
  • the light 3, 31 of the laser light sources 2, 30 is brought together by a polarization coupler 32 and via the spectral divider
  • the evaluation means 8 comprise, for example, a filter
  • the filter 33 for the Raman radiation and a detector 10 for the Stokes scattered radiation is designed as a replaceable filter, so that the two channels (Stokes and anti-Stokes scattered radiation) are measured successively.
  • the evaluation means 8 additionally comprise a measurement electronics 12.
  • connection 34 between the drive means 1 of the laser light sources 2, 30 and the measuring electronics 12 can be seen. This connection is used to synchronize the laser light sources 2, 30 with the measuring electronics 12.

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Temperature Or Quantity Of Heat (AREA)
  • Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)

Abstract

Dispositif de mesure de température à résolution spatiale, comprenant une fibre optique (6) pour la mesure de température à résolution spatiale et au moins une source de lumière laser (2), dont la lumière (3, 23) peut être injectée dans la fibre optique (6), les fractions de la lumière (3, 23) rétrodiffusées dans la fibre optique (6) pouvant être extraites de la fibre optique (6) et évaluées. Le dispositif comprend en outre des moyens destinés à réduire les effets dus à la polarisation, moyens qui pourront comprendre, par exemple, un variateur de polarisation (4), lequel peut dépolariser, au moins partiellement, la lumière (3).
EP09745482A 2008-05-15 2009-03-14 Dispositif de mesure de temperature a resolution spatiale Ceased EP2279397A1 (fr)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
DE200810023777 DE102008023777B4 (de) 2008-05-15 2008-05-15 Vorrichtung zur ortsaufgelösten Temperaturmessung
PCT/EP2009/001879 WO2009138148A1 (fr) 2008-05-15 2009-03-14 Dispositif de mesure de température à résolution spatiale

Publications (1)

Publication Number Publication Date
EP2279397A1 true EP2279397A1 (fr) 2011-02-02

Family

ID=40718879

Family Applications (1)

Application Number Title Priority Date Filing Date
EP09745482A Ceased EP2279397A1 (fr) 2008-05-15 2009-03-14 Dispositif de mesure de temperature a resolution spatiale

Country Status (5)

Country Link
US (1) US8807832B2 (fr)
EP (1) EP2279397A1 (fr)
CN (1) CN102027346B (fr)
DE (1) DE102008023777B4 (fr)
WO (1) WO2009138148A1 (fr)

Families Citing this family (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB0612868D0 (en) * 2006-06-29 2006-08-09 Schlumberger Holdings Fiber optic temperature monitoring sensor for use on sub-sea pipelines to predict hydrate formation
CN114563030A (zh) * 2009-05-27 2022-05-31 希里克萨有限公司 光学感测的方法及装置
DE102009047990A1 (de) * 2009-10-01 2011-04-07 Lios Technology Gmbh Vorrichtung und Verfahren zur ortsaufgelösten Temperaturmessung
CN102680138B (zh) * 2012-06-07 2014-06-25 北京航空航天大学 一种双向四通道耦合的分布式光纤拉曼测温系统
CN103292928B (zh) * 2013-05-31 2016-12-28 威海北洋电气集团股份有限公司 高分辨率分布式光纤温度传感器和测温装置及使用方法
CN106323470B (zh) * 2016-08-04 2019-01-15 北京华泰诺安探测技术有限公司 使用空间输出激光器的偏振调制拉曼探头及光谱探测方法
CN108872154B (zh) * 2018-05-25 2021-01-01 中国科学院上海光学精密机械研究所 无包层光纤空间角分辨激光散射损耗的测量装置和方法
CN108709661B (zh) * 2018-07-26 2020-05-19 苏州光格设备有限公司 用于分布式光纤测温系统的数据处理方法及装置

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US20080018903A1 (en) * 2006-06-05 2008-01-24 Xiaoyi Bao Distributed Brillouin sensor system based on DFB lasers using offset locking

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Also Published As

Publication number Publication date
US8807832B2 (en) 2014-08-19
CN102027346A (zh) 2011-04-20
DE102008023777B4 (de) 2011-08-25
US20110058590A1 (en) 2011-03-10
CN102027346B (zh) 2014-05-21
WO2009138148A1 (fr) 2009-11-19
DE102008023777A1 (de) 2009-11-26

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