Fabry-perot optical sensing device for measuring a physical parameter

• US 5,202,939 A
• Filed: 07/21/1992
• Issued: 04/13/1993
• Est. Priority Date: 07/21/1992
• Status: Expired due to Term

• Current Assignee: Institut national d'optique, Ministere Des Transports
• Original Assignee: Her Majesty The Queen In Right of Canada As Represented By The Minister of National Defence, Institut national d'optique
• Inventors: Belleville, Claude, Duplain, Gaetan
• Primary Examiner(s): Lee, John D.
• Assistant Examiner(s): PALMER, PHAN T H
• Application Number:
  US07/915,645
• Time in Patent Office: 266 Days
• Field of Search: 385/12, 385/27, 385/13, 385/18, 250/227.27, 356/345, 356/349
• US Class Current: 385/12
• CPC Class Codes: G01B 11/18 using photoelastic elements
• CPC Class Codes: G01D 5/266 by interferometric means G01D5/353 takes precedence
• CPC Class Codes: G02B 6/29359 Cavity formed by light guide ends, e.g. fibre Fabry Pérot [FFP]
• CPC Class Codes: G02B 6/3854 Ferrules characterised by materials
• CPC Class Codes: G02B 6/3855 characterised by the method of anchoring or fixing the fibre within the ferrule G02B6/3854 takes precedence
• CPC Class Codes: G02B 6/3863 fabricated by using polishing techniques grinding of the fibre ends B24B19/226
• CPC Class Codes: G02B 6/4215 the intermediate optical elements being wavelength selective optical elements, e.g. variable wavelength optical modules or wavelength lockers G02B6/4246 takes precedence

Abstract

The optical sensing device and the method thereof are for measuring a physical parameter. The device is to be connected to a light source which generates a multiple frequency light signal having predetermined spectral characteristics. The device comprises a Fabry-Perot interferometer through which the light signal is passed, an optical focusing device for focusing at least a portion of the light signal outgoing from the Fabry-Perot interferometer, and a Fizeau interferometer through which the focused light signal is passed. The Fabry-Perot interferometer includes two semi-reflecting mirrors substantially parallel to one another and spaced by a given distance so as to define a Fabry-Perot cavity having transmittance or reflectance properties which are affected by the physical parameter and which cause the spectral properties of the light signal to vary in response to the physical parameter. The Fabry-Perot interferometer is provided with at least one multimode optical fiber for transmitting the light signal into the Fabry-Perot cavity and for collecting the portion of the light signal outgoing thereof. The Fizeau interferometer includes an optical wedge forming a wedge-profiled Fizeau cavity from which exits a spatially-spread light signal indicative of the transmittance or reflectance properties of the Fabry-Perot interferometer. The physical parameter can be determined by means of the spatially-spread light signal.

Claims

1. An optical sensing device for measuring a physical parameter, to be connected to a light source for generating a multiple frequency light signal having predetermined spectral characteristics, said device comprising:

a) a Fabry-Perot interferometer through which the light signal is passed, said Fabry-Perot interferometer including two semi-reflective mirrors substantially parallel to one another and spaced by a given distance so as to define a Fabry-Perot cavity having transmittance or reflectance properties which are affected by said physical parameter and which cause said spectral properties of the light signal to vary in response to said physical parameter, said Fabry-Perot interferometer being provided with at least one multimode optical fiber for transmitting the light signal into said Fabry-Perot cavity and for collecting at least a portion of the light signal outgoing thereof;

b) optical focusing means for focusing said at least a portion of the light signal; and

c) a Fizeau interferometer through which said focused light signal is passed, said Fizeau interferometer including optical wedge means forming a wedge-profiled Fizeau cavity from which exits a spatially-spread light signal indicative of said transmittance or reflectance properties of said Fabry-Perot interferometer;

whereby said physical parameter can be determined by means of said spatially-spread light signal.

2. An optical sensing device according to claim 1, further comprising photodetecting means positioned for receiving said spatially-spread light signal, for generating a set of discrete electrical signals representing said spatially-spread light signal.

3. An optical sensing device according to claim 2, further comprising at least a second Fabry-Perot interferometer similar in structure to the first Fabry-Perot interferometer, each of said Fabry-Perot interferometers being optically coupled in parallel between said light source and said optical focusing means, wherein said focusing means are arranged to produce at least a second focused light signal derived from said at least a second Fabry-Perot interferometer and distinct from the first focused light signal, and wherein said Fizeau interferometer is arranged to produce at least a second spatially-spread light signal derived from said at least a second focused light signal and distinct from the first spatially-spread light signals, said photodetecting means being a two-dimensional photodiode array generating at least a second set of discrete electrical signals representing said at least a second spatially-spread light signal, whereby at least another physical parameter can be measured by means of said at least a second Fabry-Perot interferometer, each of said spatially-spread light signals exhibiting respectively information on the physical parameter in respect with the corresponding one of said Fabry-Perot interferometers.

4. An optical sensing device according to claim 1, further comprising a microcapillary having a longitudinal bore in which said mirrors of the Fabry-Perot interferometer are mounted, said at least one optical fiber having a tip connected to a corresponding one of said mirrors, a portion extending outside said bore, and a weld with the microcapillary, whereby said microcapillary can be bonded to a body whose deformation is to be measured, in order that the distance between said mirrors changes as a result of an elongation of the microcapillary, thereby varying the transmittance or reflectance properties of said Fabry-Perot cavity.

5. An optical sensing device according to claim 4, wherein said at least one optical fiber is a pair of multimode optical fibers, each of the tips of said optical fibers having a surface cleaved or polished at right angle and coated with the corresponding one of said mirrors.

6. An optical sensing device according to claim 4, wherein said Fabry-Perot interferometer is further provided with a thin wire made of a same material as said body, said thin wire having a tip connected to the other one of said mirrors, a portion extending therefrom in said bore, and a weld with said microcapillary, said other one of the mirrors being made of a light absorbing material for absorbing a portion of the light signal, each of the tips of said at least one optical fiber and said thin wire having a surface cleaved or polished at right angle and coated with the corresponding one of said mirrors, whereby a thermal expansion of said body is compensated by a similar thermal expansion of a portion of said thin wire within said bore.

7. An optical sensing device according to claim 5, wherein one of said optical fibers is optically coupled with said light source, and the other of said optical fibers is optically coupled to said optical focusing means.

8. An optical sensing device according to claim 4, further comprising an optical coupler for coupling the light signal into said at least one optical fiber and for coupling said at least a portion of the light signal transmitted by said at least one optical fiber into said optical focusing means, said optical coupler being optically coupled between said at least one optical fiber, said optical focusing means and said light source.

9. An optical sensing device according to claim 4, in combination with said light source, wherein said microcapillary is in quartz or stainless steel, the mirrors of said Fabry-Perot interferometer are 30% semi-reflective thin layers mirrors, said at least one optical fiber has a numerical aperture below or equal to 0,2, said focusing means are a cylindrical lens, said optical wedge means are two flat glass plates at an angle to one another, said light source is a quartz-halogen lamp or a broadband light emitting diode, and said photodetecting means are a linear photodiode array.

10. An optical sensing device according to claim 5, wherein said mirrors of the Fabry-Perot interferometer are layers of dielectric material laid all around the tips of said optical fibers, said dielectric material having a temperature melting point higher than a temperature melting point of said microcapillary and said optical fibers, the welds of said optical fibers being precisely located where said thin layers terminate over the tips of said optical fibers, whereby a gage length defined between said welds can be precisely determined.

11. An optical sensing device according to claim 1, further comprising at least a second Fabry-Perot interferometer similar in structure to the first Fabry-Perot interferometer and connected thereto in series, a first one of said Fabry-Perot interferometers being optically coupled to said light source, and a last one of said Fabry-Perot interferometer being optically coupled to said optical focusing means, whereby at least another physical parameter can be measured by means of said at least a second Fabry-Perot interferometer, said spatially-spread light signal simultaneously exhibiting information on the physical parameters in respect with each of said Fabry-Perot interferometers.

12. An optical sensing device according to claim 11, wherein said wedge means have a stepped-profiled surface for providing to said Fizeau cavity distinct ranges of cavity length, whereby crosstalk interferences in said spatially-spread light signal are suppressed.

13. An optical sensing device according to claim 1, further comprising at least a second Fabry-Perot interferometer similar in structure to the first Fabry-Perot interferometer, and an optical coupler for coupling the light signal into each of said Fabry-Perot interferometers and for coupling the portion of the light signal outgoing from each of said Fabry-Perot interferometers into said optical focusing means, sad optical coupler being optically coupled to each of said Fabry-Perot interferometers, to said light source and to said optical focusing means, whereby at least another physical parameter can be measured by means of said at least a second Fabry-Perot interferometer, said spatially-spread light signal simultaneously, exhibiting information on the physical parameters in respect with each of said Fabry-Perot interferometers.

14. An optical sensing device according to claim 1, in combination with said light source, further comprising at least a second light source and at least a second Fabry-Perot interferometer respectively similar in structure to the first light source and the first Fabry-Perot interferometer, each of said Fabry-Perot interferometers being optically coupled between the corresponding one of said light sources and said optical focusing means, whereby at least another physical parameter can be measured by means of said at least a second Fabry-Perot interferometer, only one of said light sources operating at a time such that said spatially-spread light signal only exhibits information on the physical parameter in respect with the one of said Fabry-Perot interferometers connected to said only one of the light sources.

15. An optical sensing device according to claim 1, further comprising optical collimating means for collimating said at least a portion of the light signal, said optical collimating means being optically coupled between said Fabry-Perot interferometer and said optical focusing means.

16. An optical sensing device according to claim 1, wherein said optical wedge means are formed by a thin layer of dielectric material laid down on a flat glass plate, said thin layer having a variable width so as to form said wedge-profiled Fizeau cavity.

17. An optical sensing device according to claim 1, wherein said Fabry-Perot interferometer is further provided with means for filling a space between said mirrors of the Fabry-Perot interferometer with a liquid having a refractive index which exhibits a variation as a function of said parameter, said distance between the mirrors being fixed.

18. An optical sensing device according to claim 1, wherein said Fabry-Perot interferometer includes a translucent crystal having a refractive index that exhibits a variation as a function of temperature, and opposite flat surfaces respectively forming said mirrors of the Fabry-Perot interferometer, said distance between the mirrors being fixed, whereby said temperature can be measured.

19. An optical sensing device according to claim 1, wherein said Fabry-Perot interferometer includes a translucent crystal having a refractive index that exhibits a variation as a function of temperature, and opposite flat surfaces on which said mirrors of the Fabry-Perot interferometer are respectively laid down, said distance between the mirrors being fixed, whereby said temperature can be measured.

20. An optical sensing method for measuring a physical parameter, comprising steps of:

a) generating a multiple frequency light signal having predetermined spectral characteristics;

b) passing the light signal in a Fabry-Perot interferometer including two semi-reflective mirrors substantially parallel to one another and spaced by a given distance so as to define a Fabry-Perot cavity having transmittance or reflectance properties which are affected by said physical parameter and which cause said spectral properties of the light signal to vary in response to said physical parameter, the light signal being transmitted into said Fabry-Perot cavity with at least one multimode optical fiber, and at least a portion of the light signal outgoing from said Fabry-Perot cavity being collected with said at least one optical fiber;

c) focusing said at least a portion of the light signal; and

d) passing the focused light signal through a Fizeau interferometer for converting the focused light signal into a spatially-spread light signal indicative of said transmittance or reflectance properties of said Fabry-Perot interferometer;

whereby said physical parameter can be determined by means of said spatially-spread light signal.

21. An optical sensing method according to claim 20, further comprising a step of converting said spatially-spread light signal into a set of discrete electrical signals representing said spatially-spread light signal.

22. An optical sensing method according to claim 20, wherein the light signal is also passed through at least a second Fabry-Perot interferometer in step b), whereby at least a second physical parameter can be measured and determined by means of said spatially-spread light signal

23. An optical sensing method according to claim 20, wherein the light signal is also passed through at least a second Fabry-Perot interferometer in step b), the portions of the light signal outgoing each of said Fabry-Perot interferometers are distinctly focused in step c) and converted in step d) so as to produce at least a second spatially-spread light signal, whereby at least a second physical parameter can be measured and determined by means of said at least a spatially-spread light signal.

24. An optical sensing method according to claim 20, further comprising a step of focusing at least a portion of the light signal before said step c).