Distributed and spatially averaged fiber optic temperature sensors and method using same

• US 5,499,313 A
• Filed: 09/13/1994
• Issued: 03/12/1996
• Est. Priority Date: 08/06/1982
• Status: Expired due to Fees

• Current Assignee: Marcos Y. Kleinerman
• Original Assignee: Marcos Y. Kleinerman
• Inventors: Kleinerman, Marcos Y.
• Primary Examiner(s): Healy, Brian
• Application Number:
  US08/305,252
• Time in Patent Office: 546 Days
• Field of Search: 385/12, 385/13, 385/27, 385/28, 385/29, 385/30, 385/31, 385/39, 385/38, 385/123, 385/125, 385/126, 385/127, 385/147, 385/141, 359/115, 359/124, 359/127, 250/227.11, 250/227.14, 250/227.16, 250/227.18, 250/227.22, 250/227.23, 250/458.1, 250/459.1, 372/6, 356/43, 356/44, 356/73.1, 356/300, 356/301, 356/319, 356/320, 356/432, 356/445
• US Class Current: 385/123
• CPC Class Codes: A61B 2017/00084 Temperature
• CPC Class Codes: G01D 5/35358 using backscattering to detect the measured quantity
• CPC Class Codes: G01D 5/3538 using a particular type of fiber, e.g. fibre with several cores, PANDA fiber, fiber with an elliptic core or the like
• CPC Class Codes: G01J 5/0025 Living bodies ear thermometers G01J5/0011; detecting, measuring or recording for diagnostic purposes A61B5/00
• CPC Class Codes: G01J 5/08 Optical arrangements
• CPC Class Codes: G01J 5/0818 Waveguides
• CPC Class Codes: G01J 5/0821 Optical fibres
• CPC Class Codes: G01J 5/0896 using a light source, e.g. for illuminating a surface
• CPC Class Codes: G01J 5/52 using comparison with reference sources, e.g. disappearing-filament pyrometer
• CPC Class Codes: G01J 5/602 using selective, monochromatic or bandpass filtering
• CPC Class Codes: G01K 11/32 using changes in transmittance, scattering or luminescence in optical fibres
• CPC Class Codes: G01K 11/3213 using changes in luminescence, e.g. at the distal end of the fibres
• CPC Class Codes: G01L 1/243 using means for applying force perpendicular to the fibre axis
• CPC Class Codes: G06F 2203/04109 FTIR in optical digitiser, i.e. touch detection by frustrating the total internal reflection within an optical waveguide due to changes of optical properties or deformation at the touch location
• CPC Class Codes: G06F 3/041 Digitisers, e.g. for touch screens or touch pads, characterised by the transducing means
• CPC Class Codes: G06F 3/042 by opto-electronic means
• CPC Class Codes: G06F 3/0421 by interrupting or reflecting a light beam, e.g. optical touch-screen

Abstract

Methods and devices for sensing temperature changes at a plurality of locations use a light-transmitting optical fiber system along a path including said locations, said optical fiber system having a first end and a second end and a sensing element of said locations, each sensing element being so characterized that, when exposed to the temperature changes to be sensed and transmitting interrogating light of suitable wavelength or wavelengths λ_v and an intensity P_o, it converts a fraction αP_o of the intensity of said interrogating light into a light separable from the interrogating light, at least part of the intensity of which is emitted from at least one of said two ends of the probe at wavelengths λ_f different from λ_v, where α is a temperature-dependent fraction smaller than unity, the value of which increases with increasing temperature within a temperature range, the intensity of said light of wavelengths λ_f being substantially proportional to the value of α. The system can be used to sense the temperature distribution among the different locations, or to provide the spatially averaged temperature along the optical fiber system.

Claims

1. A method for sensing temperature changes at a plurality of locations, comprising the steps of:

(a) providing a light-transmitting optical fiber system along a path including said locations, said optical fiber system having a first end and a second end and a sensing element at each of said locations, each sensing element being so characterized that, when exposed to the temperature changes to be sensed and transmitting interrogating light of suitable wavelength or wavelengths λ

_v and an intensity P_o, it converts a fraction α

P_o of the intensity of said interrogating light into a light separable from the interrogating light, at least part of the intensity of which is emitted from the sensing element at wavelengths λ

_f different from λ

_v, where α

is a temperature-dependent fraction smaller than unity, the value of which increases with increasing temperature within a temperature range, the intensity of said light of wavelengths λ

_f being substantially proportional to the value of α

;

(b) injecting said interrogating light of intensity P_o and wavelength or wavelengths λ

_v into the optical fiber system at said first end thereof, thereby converting at each sensing element a fraction α

P_o of the intensity of said injected interrogating light into a light separable from the interrogating light, at least part of the intensity of which is emitted from each sensing element at wavelengths λ

_f different from λ

_v, the value of α

varying as a known function of temperature, said emitted light having an intensity varying with the value of α

;

(c) selectively directing a fraction of the intensity of said emitted light of wavelengths λ

_f received by said photodetector means;

(d) sensing the variations of the intensity of said emitted light of wavelengths λ

_f received by said photodetector means; and

(e) thereby sensing the temperature changes of the sensing elements from the variations of the intensity of said light of wavelengths λ

_f received by said photodetector means.

2. The method as claimed in claim 1 and using optical time domain reflectometry, wherein said interrogating light is injected into said first end of the fiber system as pulses of submicrosecond duration, said photodetector is located at or near said first end, and the intensity of said light of wavelengths λ

_f received by said photodetector is emitted by the fiber system at said first end as pulses of submicrosecond duration generated at all said sensing elements, the time of arrival at the photodetector of said emitted pulses generated at each sensing element relative to the time of injection of the interrogating light pulses identifying the location of the sensing element, the intensity of said emitted pulses being a known function of the temperature of said sensing element.

3. The method as claimed in claim 1 wherein said fiber optic system is a long continuous optical fiber doped along its length with photoluminescent material and has a core and at least one cladding, said sensing elements are spatially resolvable segments of said fiber, said interrogating light is not pulsed, and said emitted light of wavelengths λ

_f is luminescence light generated by the absorption of said fraction α

P_o of the intensity of the interrogating light by said photoluminescent material, the intensity of said light of wavelengths λ

_f received by said photodetector varying as a known function of the average temperature of the fiber system over its length.

4. The method as claimed in claim 1, additionally including the steps of:

(a) measuring the intensity of the interrogating light transmitted by the sensing elements; and

(b) comparing the intensities of said interrogating light transmitted by said sensing elements and said emitted light of wavelengths λ

_f received by said photodetector means, their ratio being an indicator of the temperatures at said locations.

5. The method as claimed in claim 3, additionally including the steps of:

(a) measuring the intensity of the interrogating light transmitted by the sensing elements; and

(b) comparing the intensities of said interrogating light transmitted by said sensing elements and said luminescence light received by said photodetector means, their ratio being an indicator of the temperatures at said locations.

6. The method as claimed in claim 1 wherein said wavelengths λ

_f are shorter than λ

_v.

7. The method as claimed in claim 1 wherein the sensing elements include a photoluminescent material and said emitted light of wavelengths λ

_f is luminescence light generated by the absorption of said fraction α

P_o of the intensity of the interrogating light by said photoluminescent material.

8. The method as claimed in claim 7 wherein said photoluminescent material is an organic fluorescent dye having a fluorescence decay time of the order of 10^-8 seconds or shorter.

9. An optical time-domain reflectometry method as claimed in claim 2 and additionally comprising the steps of:

(a) directing pulses of backscattered light of the same wavelength or wavelengths of the interrogating light from said locations to photodetector means, thus producing electrical output signals from said locations indicative of the intensity of said interrogating light at said locations; and

(b) measuring the relative intensities of said light of wavelengths λ

_f and said light of the same wavelength or wavelengths as those of the interrogating light backscattered from each of said locations, said relative intensities being indicative of the temperatures at said locations.

10. An optical time-domain reflectometry method as claimed in claim 2 wherein said fiber optic system is a long continuous optical fiber doped along its length with photoluminescent material, said sensing elements are spatially resolvable segments of said fiber, and said light of wavelengths λ

_f is luminescence light generated by the absorption of said temperature-dependent fraction α

P_o of the intensity of the interrogating light by said photoluminescent material.

11. An optical time-domain reflectometry method as claimed in claim 10 wherein said photoluminescent material is an organic fluorescent dye having a fluorescence decay time of the order of 10^-8 seconds or shorter.

12. An optical time-domain reflectometry method as claimed in claim 10 wherein the sensing elements are made of laser material so characterized that, when excited with laser pump radiation of suitable. pre-selected wavelengths and an intensity P_o, it absorbs a fraction α

P_o of said intensity, the value of α

being smaller than unity and increasing monotonically with increasing temperature, the magnitude of α

P_o over at least part of the temperature range of operation of the method being high enough to create a concentration of the excited molecules of said laser material sufficient for stimulated light amplification of light wavelength λ

_f within a characteristic laser band of said material and different from the wavelength or wavelengths of the pump radiation, the method additionally including the step of launching at said second end of the fiber optic system a continuous beam of light of wavelength λ

_f, said light being pulse-amplified at each sensing element to an extent determined by the temperature of the element.

13. An optical time-domain reflectometry method as claimed in claim 10 wherein said fiber optic system is a long continuous optical fiber doped along its length with said laser material, said sensing elements are spatially resolvable segments of said fiber, and said laser material is a glass doped with rare earth ions chosen from the group comprising the trivalent ions of neodymium, erbium, ytterbium and holmium.

14. An optical time-domain reflectometry method as claimed in claim 10 wherein said fiber is doped along its length with an organic fluorescent dye having a fluorescence decay time of the order of 10^-8 seconds or shorter.

15. A device for sensing temperature changes at a plurality of locations, comprising

(a) a light-transmitting optical fiber system along a path including said locations, said optical fiber system having a first end and a second end and a sensing element at each of said locations, each sensing element being so characterized that, when exposed to the temperature changes to be sensed and transmitting interrogating light of suitable wavelength or wavelengths λ

_v and an intensity P_o, it converts a fraction α

P_o of the intensity of said interrogating light into a light separable from the interrogating light, at least part of the intensity of which is emitted from at least one of said two ends of the probe at wavelengths λ

_f different from λ

_v, where α

is a temperature-dependent fraction smaller than unity, the value of which increases with increasing temperature within a temperature range, the intensity of said light of wavelengths λ

_f being substantially proportional to the value of α

;

(b) a source of said interrogating light of wavelength or wavelengths λ

_v ;

(c) optical means for selectively directing a fraction of the intensity of said emitted light of wavelengths λ

_f to photodetector means; and

(d) photodetector means for measuring the intensity of said pulses of optical radiation of wavelengths λ

_f.

16. A device as claimed in claim 15 and using optical time domain reflectometry, wherein said interrogating light is injected into the optical fiber system as pulses of submicrosecond duration, said photodetector is located at or near said first end, and the intensity of said light of wavelengths λ

_f received by said photodetector is emitted by the sensing element at said first end as pulses of submicrosecond duration generated at all said sensing elements, the time of arrival at the photodetector of said emitted pulses generated at each sensing element relative to the time of injection of the interrogating light pulses identifying the location of the sensing element, the intensity of said emitted pulses being a known function of the temperature of said sensing element.

17. A device as claimed in claim 15 wherein said interrogating light is not pulsed and the intensity of said light of wavelengths λ

_f emitted by the fiber system and received by said photodetector varies as a known function of the average temperature of the fiber system over its length.

18. A device as claimed in claim 17 wherein said wherein said fiber optic system is a long continuous optical fiber and said sensing elements are spatially resolvable segments of said fiber.

19. A device as claimed in claim 18 wherein said wherein said optical fiber is doped along its length with photoluminescent material and said emitted light of wavelengths λ

_f is luminescence light generated by the absorption of said fraction α

P_o of the intensity of the interrogating light by said photoluminescent material.

20. A device as claimed in claim 19 wherein said photoluminescent material is a glass doped with rare earth ions chosen from the group comprising the trivalent ions of neodymium, erbium, ytterbium and holmium.

21. A device as claimed in claim 20 and additionally including:

(a) means for measuring the intensity of the interrogating light transmitted by said optical fiber; and

(b) means for comparing the intensities of said interrogating light transmitted by said sensing elements and said emitted light of wavelengths λ

_f received by said photodetector means, their ratio being an indicator of the average temperature of the fiber over its length.

22. An optical time domain reflectometry device as claimed in claim 16 wherein said wavelengths λ

_f are shorter than λ

_v.

23. An optical time domain reflectometry device as claimed in claim 16 wherein the sensing elements include a photoluminescent material and said emitted light of wavelengths λ

_f is luminescence light generated by the absorption of said fraction α

P_o of the intensity of the interrogating light by said photoluminescent material.

24. An optical time domain reflectometry device as claimed in claim 23 wherein said photoluminescent material is an organic fluorescent dye having a fluorescence decay time of the order of 10^-8 seconds or shorter.

25. An optical time domain reflectometry device as claimed in claim 16 and additionally comprising:

(a) means for directing pulses of backscattered light of the same wavelength or wavelengths of the interrogating light from said locations to photodetector means, thus producing electrical output signals from said locations indicative of the intensity of said interrogating light at said locations; and

(b) photodetection means for measuring the relative intensities of said light of wavelengths λ

_f and said light of the same wavelength or wavelengths as those of the interrogating light backscattered from each of said locations, said relative intensities being indicative of the temperatures at said locations.

26. An optical time domain reflectometry device as claimed in claim 16 wherein said fiber optic system is a long continuous optical fiber and said sensing elements are spatially resolvable segments of said fiber.

27. An optical time domain reflectometry device as claimed in claim 26 and adapted to sense force at a plurality of locations in addition to temperature, wherein said fiber has a clear first core and a second core comprised of photoluminescent material, said second core having an index of refraction not lower than that of the first core, said second core and said first core being disposed within a clear cladding having an index of refraction lower than that of the first core, the fiber being so characterized that, when transmitting pulses of interrogating light along the clear core, a lateral mechanical force acting on the fiber causes the deflection of a force-dependent fraction of the intensity of the interrogating light from the clear core to the second core, and the generation therein of pulses of luminescence light the time of arrival of which at the photodetector, relative to the time of injection of the interrogating light pulses, identifying the location of the sensing element, the intensity of said emitted pulses being a known function of the temperature of said sensing element.

28. An optical time domain reflectometry device as claimed in claim 26 wherein said wavelengths λ

_f are shorter than λ

_v.

29. An optical time domain reflectometry device as claimed in claim 16 wherein said sensing elements are doped with laser material so characterized that, when excited with laser pump radiation of said wavelength or wavelengths λ

_v and an intensity P_o, it absorbs a fraction α

P_o of said intensity, the value of α

being smaller than unity and increasing monotonically with increasing temperature, the magnitude of α

P_o over at least part of the temperature range of operation of the method being high enough to create a concentration of the excited molecules of said laser material sufficient for stimulated light amplification of light of wavelength λ

_f within a characteristic laser band of said material and different from the wavelength or wavelengths of the pump radiation, having an optical absorption band at wavelengths including the wavelength or wavelengths of the interrogating radiation, and wherein said interrogating optical radiation has an intensity sufficiently high to produce a population inversion of the laser material and amplification of optical radiation of wavelength λ

_f within a laser band of said material at said locations, the magnitude of said population inversion and the amplification gain being a indicative of the temperatures at said locations, the apparatus additionally comprising;

(a) source means for launching a continuous beam of optical radiation of wavelength λ

_f at the second end of said fiber system, to propagate in a direction counter to the direction of propagation of the interrogating radiation; and

(b) means for measuring the amplification gain of said continuous beam of optical radiation of wavelengths λ

_f at said locations.

30. An optical time domain reflectometry device as claimed in claim 29 wherein said fiber optic system is a long continuous optical fiber doped along its length with said laser material and said sensing elements are spatially resolvable segments of said fiber.

31. A device as claimed in claim 30 wherein said laser material is a glass doped with rare earth ions chosen from the group comprising the trivalent ions of neodymium, erbium, ytterbium and holmium.

32. A device as claimed in claim 30 and adapted to sense force at a plurality of locations in addition to temperature, wherein said fiber has a clear first core and a second core comprised of photoluminescent material, said second core having an index of refraction not lower than that of the first core, said second core and said first core being disposed within a clear cladding having an index of refraction lower than that of the first core.

33. An optical time domain reflectometry arrangement for sensing physical variables at a plurality of sensing points, including

(a) an optical fiber having a first end and a second end and a glass core having a cross-sectional area perpendicular to the fiber length smaller than about 10^-5 cm² and comprised of laser material having an index of refraction n_b, said core being disposed within a first cladding having an index of refraction n_a lower than n_b, said first cladding being surrounded by a second cladding having an index of refraction n_c lower than n_b, with substantially no space between said first cladding and said second cladding,

wherein the cross-sectional area of said first cladding taken substantially transverse to the axial extent of the optical fiber has a first path across said area which passes substantially through the geometric center thereof whose length is substantially different from the length of a second path across said area which passes substantially through the geometric center thereof, said second path being substantially perpendicular to said first path, the length of said first path being not more than a few micrometers longer than the dimension of the core along a path parallel to said first path, the length of said second path being at least several times longer than the length of said first path,

said fiber being disposed along a length including said plurality of sensing points and being additionally so characterized that, when optical pump radiation of suitable intensity and wavelengths λ

_s is injected into the cross-sectional area of said first cladding at said first end of the fiber and propagates along the length of the fiber, most of the energy of said pump radiation is absorbed by the laser material of said core at said sensing points, thereby generating a population inversion and luminescence radiation having wavelengths λ

_f different from the wavelengths of said pump radiation, the magnitude of the population inversion at each sensing point being a know function of the magnitude of the physical parameter;

the arrangement additionally including

(b) means for generating and launching said optical pump radiation into the cross-sectional area of said first cladding at said one end of the fiber, said pump radiation being in the form of pulses of submicrosecond duration and an intensity sufficiently high to generate a population inversion within the fiber core at said sensing points,

(c) means for injecting radiation of said wavelengths λ

_f into said fiber core at said second fiber end, said radiation of said wavelengths λ

_f being pulse-amplified at said sensing points as it propagates along the fiber in the direction opposite to that of the pump radiation, the magnitude of the amplification at a sensing point being a known function of the magnitude of the population inversion and, hence, of the magnitude of the physical parameter at that point;

(d) fiber optic means for directing a fraction of the intensity of said converted radiation of wavelengths λ

_f amplified at said sensing points along the fiber to photodetector means; and

(e) photodetector means for measuring the intensities of said amplified radiation of wavelengths λ

_f at said sensing points.

34. A device as claimed in claim 33 wherein said physical parameter is temperature and the amplification factor at each of said sensing points varies as a known function of temperature.

35. A device as claimed in claim 33 wherein said laser material is a glass doped with rare earth ions chosen from the group comprising the trivalent ions of neodymium, erbium, ytterbium and holmium.