BR0309675A - Sensor a laser de fibra de alta resolução - Google Patents
Sensor a laser de fibra de alta resoluçãoInfo
- Publication number
- BR0309675A BR0309675A BR0309675-0A BR0309675A BR0309675A BR 0309675 A BR0309675 A BR 0309675A BR 0309675 A BR0309675 A BR 0309675A BR 0309675 A BR0309675 A BR 0309675A
- Authority
- BR
- Brazil
- Prior art keywords
- fiber
- laser
- sensor
- fiber laser
- optical states
- Prior art date
Links
- 239000000835 fiber Substances 0.000 title abstract 13
- 230000003287 optical effect Effects 0.000 abstract 4
- 230000008878 coupling Effects 0.000 abstract 3
- 238000010168 coupling process Methods 0.000 abstract 3
- 238000005859 coupling reaction Methods 0.000 abstract 3
- 230000035559 beat frequency Effects 0.000 abstract 1
- 238000010009 beating Methods 0.000 abstract 1
- 238000001514 detection method Methods 0.000 abstract 1
- 238000011156 evaluation Methods 0.000 abstract 1
- 230000003993 interaction Effects 0.000 abstract 1
- 238000005259 measurement Methods 0.000 abstract 1
- 230000010287 polarization Effects 0.000 abstract 1
- 238000005086 pumping Methods 0.000 abstract 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/05—Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
- H01S3/06—Construction or shape of active medium
- H01S3/063—Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
- H01S3/067—Fibre lasers
- H01S3/0675—Resonators including a grating structure, e.g. distributed Bragg reflectors [DBR] or distributed feedback [DFB] fibre lasers
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
- G01D5/00—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
- G01D5/26—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
- G01D5/32—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light
- G01D5/34—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
- G01D5/344—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells using polarisation
-
- 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
- G01L1/242—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 the material being an optical fibre
- G01L1/246—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 the material being an optical fibre using integrated gratings, e.g. Bragg gratings
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L11/00—Measuring steady or quasi-steady pressure of a fluid or a fluent solid material by means not provided for in group G01L7/00 or G01L9/00
- G01L11/02—Measuring steady or quasi-steady pressure of a fluid or a fluent solid material by means not provided for in group G01L7/00 or G01L9/00 by optical means
- G01L11/025—Measuring steady or quasi-steady pressure of a fluid or a fluent solid material by means not provided for in group G01L7/00 or G01L9/00 by optical means using a pressure-sensitive optical fibre
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L9/00—Measuring steady of quasi-steady pressure of fluid or fluent solid material by electric or magnetic pressure-sensitive elements; Transmitting or indicating the displacement of mechanical pressure-sensitive elements, used to measure the steady or quasi-steady pressure of a fluid or fluent solid material, by electric or magnetic means
- G01L9/0041—Transmitting or indicating the displacement of flexible diaphragms
- G01L9/0076—Transmitting or indicating the displacement of flexible diaphragms using photoelectric means
- G01L9/0077—Transmitting or indicating the displacement of flexible diaphragms using photoelectric means for measuring reflected light
- G01L9/0079—Transmitting or indicating the displacement of flexible diaphragms using photoelectric means for measuring reflected light with Fabry-Perot arrangements
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/05—Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
- H01S3/06—Construction or shape of active medium
- H01S3/063—Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
- H01S3/067—Fibre lasers
- H01S3/06708—Constructional details of the fibre, e.g. compositions, cross-section, shape or tapering
- H01S3/06712—Polarising fibre; Polariser
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/05—Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
- H01S3/08—Construction or shape of optical resonators or components thereof
- H01S3/08018—Mode suppression
- H01S3/08022—Longitudinal modes
- H01S3/08031—Single-mode emission
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/10—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
- H01S3/105—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling the mutual position or the reflecting properties of the reflectors of the cavity, e.g. by controlling the cavity length
- H01S3/1053—Control by pressure or deformation
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Optics & Photonics (AREA)
- Optical Transform (AREA)
- Photometry And Measurement Of Optical Pulse Characteristics (AREA)
- Length Measuring Devices By Optical Means (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
"SENSOR A LASER DE FIBRA DE ALTA RESOLUçãO". A presente invenção refere-se a um sensor a laser de fibra de alta resolução para medir uma quantidade a ser medida (M), que tem uma fonte de luz de bombeamento (2), um laser de fibra (1) e uma unidade de detecção/ avaliação (3). O laser de fibra (1) tem: um primeiro refletor de extremidade birrefringente (11) e um segundo refletor de extremidade (12), uma fibra de amplificação de laser (13), uma fibra sensora (14) e um meio para acoplamento de modo (15). A fibra de amplificação de laser (13), a fibra sensora (14) e o meio para acoplamento de modo (15) são dispostos entre o refletores de extremidade (11, 12). No laser de fibra (1), luz é capaz de se propagar em dois estados óticos (x,y; LP<39>~ 01~,LP<39>~ 11~), que são ortogonais um ao outro devido a sua polarização e/ou sua estrutura de espaço transversal. Os estados óticos ortogonais (x,y; LP<39>~ 01~,LP<39>~ 11~) podem ser acoplados um ao outro pelo meio para acoplamento de modo (15). No laser de fibra (1) um número de modos longitudinais (LM^ x^~ p~, LM^ x^~ p+1~..., LM^ y^~ q~, LM^ y^~ q+1~..., LM^ 01^~ p~, LM^ 01^~ p+1~..., LM^ 11^~ q~, LM^ 11^~ q+1~...) são capazes de oscilar em cada um dos dois estados óticos (x,y; LP<39>~ 01~,LP<39>~ 11~). Na fibra sensora (14) uma mudança na birrefringência para os dois estados óticos ortogonais (x,y; LP<39>~ 01~,LP<39>~ 11~) pode ser obtida pela interação da quantidade a ser medida (M) com a fibra sensora (14). A mudança na birrefringência resulta em uma mudança nas freq³ências de batimento na emissão do laser. Devido ao fato de que o primeiro refletor de extremidade (11) é dessintonizado com relação ao segundo refletor de extremidade (12), é possível detectar sinais de batimento individuais do modo de polarização em lugar de um sinal de batimento que consiste em um número de sinais de PMB degenerados e é, portanto, ampliado. Uma alta resolução de sensor é obtida.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP02405353A EP1359394A1 (de) | 2002-04-30 | 2002-04-30 | Hochauflösender Faserlaser-Sensor |
PCT/CH2003/000277 WO2003093770A1 (de) | 2002-04-30 | 2003-04-29 | Hochauflösender faserlaser-sensor |
Publications (2)
Publication Number | Publication Date |
---|---|
BR0309675A true BR0309675A (pt) | 2005-02-15 |
BRPI0309675B1 BRPI0309675B1 (pt) | 2016-11-29 |
Family
ID=28799767
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
BRPI0309675A BRPI0309675B1 (pt) | 2002-04-30 | 2003-04-29 | sensor a laser de fibra de alta resolução |
Country Status (6)
Country | Link |
---|---|
US (1) | US7251023B2 (pt) |
EP (2) | EP1359394A1 (pt) |
AU (1) | AU2003218858A1 (pt) |
BR (1) | BRPI0309675B1 (pt) |
NO (1) | NO20045125L (pt) |
WO (1) | WO2003093770A1 (pt) |
Families Citing this family (17)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE102004037519B4 (de) * | 2004-07-30 | 2008-12-18 | Universität Kassel | Sensor-Vorrichtung und Verfahren zur Ermittlung einer physikalischen Größe |
GB0500277D0 (en) * | 2005-01-07 | 2005-02-16 | Southampton Photonics Ltd | Apparatus for propagating optical radiation |
KR100640006B1 (ko) * | 2005-10-14 | 2006-11-01 | 한국전자통신연구원 | 광학적 클럭 신호 추출 장치 및 방법 |
JPWO2007066747A1 (ja) * | 2005-12-09 | 2009-05-21 | パナソニック株式会社 | ファイバーレーザ |
FR2929000B1 (fr) * | 2008-03-18 | 2010-04-09 | Thales Sa | Capteur a fibre optique auto-reference et reseau de capteurs associe |
WO2010054262A1 (en) * | 2008-11-07 | 2010-05-14 | The Government Of The United States Of America, As Represented By The Secretary Of The Navy | Measurement of fiber twist by polarization tracking |
EP2646862B1 (en) * | 2010-12-02 | 2020-09-23 | Ofs Fitel Llc | Dfb fiber laser bend sensor and optical heterodyne microphone |
DE102012214441B4 (de) * | 2012-08-14 | 2020-08-06 | Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. | Messverfahren |
EP3036502A4 (en) * | 2013-08-23 | 2017-03-15 | FOCE Technology International B.V. | Single mode fiber bragg grating pressure sensor |
US9341532B2 (en) * | 2014-03-24 | 2016-05-17 | General Electric Company | Systems and methods for distributed pressure sensing |
CN106773014A (zh) * | 2016-12-12 | 2017-05-31 | 南京大学 | 一种提高光纤液压传感器灵敏度的复合双腔结构 |
WO2019205028A1 (zh) * | 2018-04-25 | 2019-10-31 | 深圳大学 | 一种光纤激光压力传感器及其压力测量方法 |
WO2020264056A1 (en) * | 2019-06-24 | 2020-12-30 | Nlight, Inc. | Functionally homogenized intensity distribution for additive manufacturing or other industrial laser processing applications |
US11761828B2 (en) * | 2020-04-14 | 2023-09-19 | Ultra Communications, Inc. | Single wavelength fiber grating sensing with spatial location |
IT202000032027A1 (it) * | 2020-12-23 | 2022-06-23 | Brembo Spa | Metodo e sistema per interrogare un sensore fibre bragg grating birifrangente, impiegante rilevazione ottica eterodina |
CN113049014B (zh) * | 2021-03-10 | 2022-04-15 | 太原理工大学 | 一种基于泵浦光扫频的时频复用botda系统及传感方法 |
US11656140B1 (en) | 2022-04-25 | 2023-05-23 | The Government Of The United States Of America, As Represented By The Secretary Of The Navy | Coated fiber optic pressure sensor with improved acceleration response |
Family Cites Families (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5513913A (en) | 1993-01-29 | 1996-05-07 | United Technologies Corporation | Active multipoint fiber laser sensor |
KR960015900B1 (ko) | 1993-04-22 | 1996-11-23 | 국방과학연구소 | 광섬유 레이저를 이용한 물리량 측정장치 |
NO302441B1 (no) * | 1995-03-20 | 1998-03-02 | Optoplan As | Fiberoptisk endepumpet fiber-laser |
GB2323441B (en) * | 1997-03-22 | 2001-02-14 | British Aerospace | Apparatus for sensing temperature and/or strain in an object |
US6801686B2 (en) * | 1997-06-06 | 2004-10-05 | Novera Optics, Inc. | Methods and apparatus for measuring the power spectrum of optical signals |
US6640027B2 (en) * | 1997-06-06 | 2003-10-28 | Novera Optics, Inc. | Gain flattening tunable filter |
DE19807891A1 (de) * | 1998-02-25 | 1999-08-26 | Abb Research Ltd | Faserlaser-Drucksensor |
US6188712B1 (en) * | 1998-11-04 | 2001-02-13 | Optigain, Inc. | Asymmetrical distributed feedback fiber laser |
US6246048B1 (en) * | 1999-05-18 | 2001-06-12 | Schlumberger Technology Corporation | Methods and apparatus for mechanically enhancing the sensitivity of longitudinally loaded fiber optic sensors |
NO321724B1 (no) * | 1999-06-15 | 2006-06-26 | Optoplan As | Framgangsmate og anordning for malinger av de ortogonalt polariserte Bragg-bolgelengdene fra fiber-Bragg-gitter |
US6532321B1 (en) * | 2000-02-16 | 2003-03-11 | Adc Telecommunications, Inc. | Fiber optic isolator for use with multiple-wavelength optical signals |
-
2002
- 2002-04-30 EP EP02405353A patent/EP1359394A1/de not_active Withdrawn
-
2003
- 2003-04-29 EP EP03714605A patent/EP1499859A1/de not_active Withdrawn
- 2003-04-29 WO PCT/CH2003/000277 patent/WO2003093770A1/de not_active Application Discontinuation
- 2003-04-29 US US10/512,574 patent/US7251023B2/en not_active Expired - Fee Related
- 2003-04-29 AU AU2003218858A patent/AU2003218858A1/en not_active Abandoned
- 2003-04-29 BR BRPI0309675A patent/BRPI0309675B1/pt not_active IP Right Cessation
-
2004
- 2004-11-24 NO NO20045125A patent/NO20045125L/no not_active Application Discontinuation
Also Published As
Publication number | Publication date |
---|---|
US7251023B2 (en) | 2007-07-31 |
BRPI0309675B1 (pt) | 2016-11-29 |
EP1499859A1 (de) | 2005-01-26 |
WO2003093770A1 (de) | 2003-11-13 |
EP1359394A1 (de) | 2003-11-05 |
NO20045125L (no) | 2005-01-28 |
US20060013534A1 (en) | 2006-01-19 |
AU2003218858A1 (en) | 2003-11-17 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
B25A | Requested transfer of rights approved |
Owner name: ABB OFFSHORE SYSTEMS LTD. (GB) Free format text: TRANSFERIDO DE: ABB RESEARCH LTD. |
|
B25D | Requested change of name of applicant approved |
Owner name: VETCO GRAY CONTROLS LIMITED (GB) Free format text: ALTERADO DE: ABB OFFSHORE SYSTEMS LTD. |
|
B25A | Requested transfer of rights approved |
Owner name: GE OIL AND GAS UK LIMITED (GB) |
|
B09A | Decision: intention to grant [chapter 9.1 patent gazette] | ||
B16A | Patent or certificate of addition of invention granted [chapter 16.1 patent gazette] |
Free format text: PRAZO DE VALIDADE: 10 (DEZ) ANOS CONTADOS A PARTIR DE 29/11/2016, OBSERVADAS AS CONDICOES LEGAIS. |
|
B21F | Lapse acc. art. 78, item iv - on non-payment of the annual fees in time | ||
B24J | Lapse because of non-payment of annual fees (definitively: art 78 iv lpi, resolution 113/2013 art. 12) |