WO2011076503A1 - Interféromètre et dispositif capteur de pression doté d'un tel interféromètre - Google Patents
Interféromètre et dispositif capteur de pression doté d'un tel interféromètre Download PDFInfo
- Publication number
- WO2011076503A1 WO2011076503A1 PCT/EP2010/067935 EP2010067935W WO2011076503A1 WO 2011076503 A1 WO2011076503 A1 WO 2011076503A1 EP 2010067935 W EP2010067935 W EP 2010067935W WO 2011076503 A1 WO2011076503 A1 WO 2011076503A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- reflector body
- interferometer
- light
- reflection
- reflection surface
- Prior art date
Links
- 230000002452 interceptive effect Effects 0.000 claims abstract description 4
- 230000003287 optical effect Effects 0.000 claims abstract 4
- 230000001419 dependent effect Effects 0.000 claims description 10
- 238000011156 evaluation Methods 0.000 claims description 10
- 230000005021 gait Effects 0.000 claims description 7
- 230000010355 oscillation Effects 0.000 claims description 4
- 230000001427 coherent effect Effects 0.000 claims description 3
- 238000012544 monitoring process Methods 0.000 claims description 2
- 239000013307 optical fiber Substances 0.000 description 3
- 238000005259 measurement Methods 0.000 description 2
- 230000000284 resting effect Effects 0.000 description 1
- 230000001953 sensory effect Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B9/00—Measuring instruments characterised by the use of optical techniques
- G01B9/02—Interferometers
- G01B9/02015—Interferometers characterised by the beam path configuration
- G01B9/02027—Two or more interferometric channels or interferometers
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B9/00—Measuring instruments characterised by the use of optical techniques
- G01B9/02—Interferometers
- G01B9/02015—Interferometers characterised by the beam path configuration
- G01B9/02023—Indirect probing of object, e.g. via influence on cavity or fibre
-
- 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
- G01K11/3206—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 at discrete locations in the fibre, e.g. using Bragg scattering
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01K—MEASURING TEMPERATURE; MEASURING QUANTITY OF HEAT; THERMALLY-SENSITIVE ELEMENTS NOT OTHERWISE PROVIDED FOR
- G01K5/00—Measuring temperature based on the expansion or contraction of a material
- G01K5/48—Measuring temperature based on the expansion or contraction of a material the material being a solid
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L1/00—Measuring force or stress, in general
- G01L1/24—Measuring force or stress, in general by measuring variations of optical properties of material when it is stressed, e.g. by photoelastic stress analysis using infrared, visible light, ultraviolet
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B2290/00—Aspects of interferometers not specifically covered by any group under G01B9/02
- G01B2290/25—Fabry-Perot in interferometer, e.g. etalon, cavity
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B2290/00—Aspects of interferometers not specifically covered by any group under G01B9/02
- G01B2290/45—Multiple detectors for detecting interferometer signals
Definitions
- the present invention relates to an interferometer, in particular a white light interferometer, and a pressure sensor arrangement with such an interferometer.
- a pressure sensor arrangement with a white light interferometer comprises a light source, at least one pressure sensor with a
- Sensor interferometer which has a pressure-dependent path difference over a range of value of gear differences
- evaluation interferometer which the path difference of
- Sensor interferometer over the range of values of the sensor interferometer simulates, wherein the light source, the sensor interferometer and the Ausenseinterferometer are coupled together via optical fibers.
- the sensor interferometers are usually Fabry-Perot interferometers, while the evaluation interferometers may comprise, for example, Michelson interferometers, Fabry-Perot interferometers or Fizeau interferometers.
- Evaluation interferometer are to evaluate, so it is possible to
- An evaluation interferometer for such a measurement arrangement must cover the entire value range of the possible path differences of all
- irradiated, collimated white light comprises a first
- Reflector body with at least two juxtaposed, parallel reflection surfaces, which are used to produce a
- the stroke for example, at least one basic course difference, preferably at least the 1, 5 times, and more preferably at least twice, a path difference due to the offset between the first and second
- Reflection surface of the first reflector body is.
- the interferometer comprises at least two light-sensitive detectors, wherein the detectors are respectively assigned to exactly one of the reflection surfaces.
- the movement of the first reflector body and / or the second reflector body comprises an oscillation around a rest position.
- a determination of the position of the oscillating reflector body to determine the current takes place
- the interferometer further comprises a capacitive transducer with a first, fixed electrode and a second electrode whose position relative to the first electrode depends on the position of the moving reflector body, wherein the
- Capacitance of the capacitive transducer takes place.
- the interferometer comprises a Michelson interferometer.
- the interferometer comprises a drive for moving at least one reflector body.
- the drive may in particular be a piezo drive, an electrostatic drive or a magnetic drive.
- the interferometer further comprises a control unit for controlling the path differences between the light reflected at the reflection surfaces of the first reflector body and the light reflected at the reflection surface of the second reflector body by controlling the movement of at least one reflector body, the control unit being designed at least in one
- Reflection on a first reflection surface of the first reflector body with to be able to compare a determined corresponding retardation due to a reflection on a second reflection surface of the first reflector body.
- Gap difference is greater than the baseline difference due to the offset between two reflective surfaces, then the interferometer can a retardation by reflections at different
- control unit is designed to set the stroke of the continuous change in the path differences to no more than one basic course difference in a measuring mode.
- the sensor arrangement according to the invention comprises a light source, in particular coherent white light; at least two
- an evaluation interferometer comprising an interferometer according to any one of the preceding claims, an optical fiber array comprising the light source, the sensor interferometer and the Ausreteinterferometer coupled together, and a
- Collimator arrangement for collimating the light from the light guide assembly into the Ausenseinterferometer.
- the sensory interferometers have pressure-dependent path differences or temperature-dependent
- FIG. 1 shows a schematic illustration of an exemplary embodiment of a sensor arrangement according to the invention.
- the sensor arrangement in Figure 1 is in particular a
- Pressure sensor arrangement with a light source, in particular coherent white light, via an optical fiber assembly 4 to four
- the evaluation interferometer comprises a first reflector body 16 with four reflection surfaces 16a, 16b, 16c, 16d offset from one another by the fundamental differences of the sensor interferometers 6a, 6b, 6c, 6d and a second reflector body having a reference reflection surface 14.
- a beam splitter 12 which is at an angle of 45 ° ° to the incident light and the reflection surfaces 14, 16a, 16b, 16c, 16d, this leads Light the reflector bodies 14, 16 and allows the interfering superposition of the reflected light.
- the interferometer further comprises a detector arrangement 18, with four detectors 18a, 18b, 18c, 18d, each one of the reflection surfaces 16a, 16b, 16c, 16d of the first
- Reflector body 16 are assigned to receive light from this reflection surface.
- the interferometer 1 further comprises a control and evaluation unit 20 which controls, for example, an electrostatic drive 22 for the second reflector body and receives position signals from the drive, wherein via the drive 22, the path differences between the at the reflection surfaces 16 a, 16 b, 16 c, 16 d of the first
- Reflector body reflected light and the at the
- Reference reflection surface 14 of the second reflector body reflected light can be varied continuously.
- the detected signals of the detector arrangement 18 are supplied to the control and evaluation unit 20.
- the path difference of the sensor interferometer and therefrom the respective pressure can be determined.
- the stroke for continuously varying the path differences by moving the second reflector body can be checked by determining the same path difference by reflection after determining a reference path difference based on the reflection at a first reflection surface and after adding or subtracting a fundamental difference in movement of the second reflector body must be reproducible at a reflection surface offset by the Referenzgangunter Kunststoff. Deviations may give rise to a readjustment of the stroke and / or to an error message.
Abstract
L'invention concerne un interféromètre pour générer des différences de chemin dans de la lumière blanche injectée et collimatée, qui comprend un premier corps réflecteur (16) doté d'au moins deux surfaces de réflexion (16a, 16b, 16c, 16d) juxtaposées et parallèles, lesquelles sont décalées l'une par rapport à l'autre en direction de la normale des surfaces de réflexion afin de générer une différence de chemin de base, un second corps réflecteur (14) doté d'au moins une surface de réflexion de référence, la lumière réfléchie sur les surfaces de réflexion (16a, 16b, 16c, 16d) du premier corps réflecteur (16) étant superposée au moins en partie par interférence à la lumière réfléchie sur le second corps réflecteur (14), la différence de chemin respective entre la lumière réfléchie sur les surfaces de réflexion (16a, 16b, 16c, 16d) du premier corps réflecteur (16) et la lumière réfléchie sur la surface de réflexion du second corps réflecteur pouvant être modifiée de façon continue par le déplacement du premier corps réflecteur dans le sens de la normale des surfaces de réflexion et/ou par le déplacement du second corps réflecteur dans le sens de la normale de la surface de réflexion de référence.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE102009055230.8 | 2009-12-23 | ||
DE102009055230 | 2009-12-23 |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2011076503A1 true WO2011076503A1 (fr) | 2011-06-30 |
Family
ID=43567511
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/EP2010/067935 WO2011076503A1 (fr) | 2009-12-23 | 2010-11-22 | Interféromètre et dispositif capteur de pression doté d'un tel interféromètre |
Country Status (1)
Country | Link |
---|---|
WO (1) | WO2011076503A1 (fr) |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE1937355A1 (de) * | 1968-07-26 | 1970-01-29 | Abramson Nils Hugo Leopold | Laengenmessung mit einem Laser-Interferometer |
WO1990009557A1 (fr) * | 1989-02-18 | 1990-08-23 | Cambridge Consultants Limited | Interferometrie |
US5202939A (en) | 1992-07-21 | 1993-04-13 | Institut National D'optique | Fabry-perot optical sensing device for measuring a physical parameter |
US6057911A (en) * | 1997-11-17 | 2000-05-02 | Northrop Grumman Corporation | Fiber optic fabry-perot sensor for measuring absolute strain |
US20020163643A1 (en) * | 2001-05-04 | 2002-11-07 | Li Chian Chiu | Optical interference apparatus and method |
-
2010
- 2010-11-22 WO PCT/EP2010/067935 patent/WO2011076503A1/fr active Application Filing
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE1937355A1 (de) * | 1968-07-26 | 1970-01-29 | Abramson Nils Hugo Leopold | Laengenmessung mit einem Laser-Interferometer |
WO1990009557A1 (fr) * | 1989-02-18 | 1990-08-23 | Cambridge Consultants Limited | Interferometrie |
US5202939A (en) | 1992-07-21 | 1993-04-13 | Institut National D'optique | Fabry-perot optical sensing device for measuring a physical parameter |
US6057911A (en) * | 1997-11-17 | 2000-05-02 | Northrop Grumman Corporation | Fiber optic fabry-perot sensor for measuring absolute strain |
US20020163643A1 (en) * | 2001-05-04 | 2002-11-07 | Li Chian Chiu | Optical interference apparatus and method |
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