GB2136113A - Improvements Relating to Optical Sensing Systems - Google Patents
Improvements Relating to Optical Sensing Systems Download PDFInfo
- Publication number
- GB2136113A GB2136113A GB08306135A GB8306135A GB2136113A GB 2136113 A GB2136113 A GB 2136113A GB 08306135 A GB08306135 A GB 08306135A GB 8306135 A GB8306135 A GB 8306135A GB 2136113 A GB2136113 A GB 2136113A
- Authority
- GB
- United Kingdom
- Prior art keywords
- optical fibre
- fibre
- optical
- fibre means
- along
- 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.)
- Granted
Links
- 230000003287 optical effect Effects 0.000 title claims abstract description 14
- 239000013307 optical fiber Substances 0.000 claims abstract description 49
- 239000000835 fiber Substances 0.000 claims abstract description 17
- 230000005540 biological transmission Effects 0.000 claims abstract description 3
- 230000002452 interceptive effect Effects 0.000 claims abstract description 3
- 239000000969 carrier Substances 0.000 claims description 6
- 230000001427 coherent effect Effects 0.000 claims description 5
- 230000003111 delayed effect Effects 0.000 claims description 4
- 230000001419 dependent effect Effects 0.000 claims description 3
- 238000005452 bending Methods 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000006073 displacement reaction Methods 0.000 description 1
Classifications
-
- 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
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01H—MEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
- G01H9/00—Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means
- G01H9/004—Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means using fibre optic sensors
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)
Abstract
An optical sensing system comprises an optical fibre (6) arranged to be subjected to fibre deforming forces during use of the system and laser means (1) Bragg cell (2) and sweep oscillator (3) for generating light signals frequency modulated with a saw-tooth waveform for transmission along the optical fibre (6). The fibre (6) comprises at points along its length respective discontinuities (9 to 16) from which a light signal being transmitted along the optical fibre will be partially reflected back along the fibre (6) and combined in combiner (8) with the light signal being transmitted down the fibre so that heterodyning occurs between the interfering signals. When the optical fibre (6) is deformed by impingement of acoustic waves thereon the heterodyned frequencies corresponding to the discontinuities will be frequency-modulated by the deformation of the optical fibres. Demodulation of the frequency- modulated signals provides an indication of the acoustic signal incident upon the optical fibre. Fibre 6 may be replaced by a plurality of different lengths of fibre star coupled to a main fibre and having totally reflecting free ends. Other parameters such as temperature, pressure, electrical current or voltage, may be measured if converted into a deformation of the fibre. <IMAGE>
Description
SPECIFICATION
Improvements Relating to Optical Sensing
Systems
This invention relates to optical systems for sensing strain or deformation (e.g. elongation or bending) of various members.
Although the present invention is especially concerned with hydrophones and the sensing of changes in length of an optical fibre in such hydrophones due to the impingement thereon of acoustic waves it should be understood that the invention is not limited to such application. In this connection many physical parameters can be converted by various well known means such as moving coil meters, bimetallic strips and Borden pressure gauges, into a displacement or deformation of some member which is dependent upon the particular parameter to be measured.
Such parameters as temperature, pressure, electrical current or voltage could be measured in this way.
According to the present invention there is provided an optical sensing system comprising optical fibre means arranged to be subjected to fibre deforming forces during use of the system and means for producing a coherent light signal for transmission along said optical fibre means, in which the optical fibre means comprises at points along its length respective discontinuities from which a light signal being transmitted along the optical fibre means will be partially or totally reflected back along the fibre means and combined with the light signal being transmitted down the optical fibre means so that heterodyning occurs between the interfering signals.
In carrying out the present invention the light signal transmitted down the optical fibre means is frequency-modulated with a saw-tooth waveform. Consequently, the signals reflected back along the optical fibre means from the respective discontinuities will be delayed with respect to the saw-tooth signal transmitted along the optical fibre means by different delay periods dependent upon the location of the discontinuity along the optical fibre means and thus a set of heterodyned frequencies or carriers will be produced in accordance with these delay periods.
The optical fibre means may comprise a signal optical fibre having partially-reflecting discontinuities equally spaced therealong or, alternatively, it may comprise suitably coupled different lengths of optical fibre, the fibre ends of which constitute totally-reflecting discontinuities.
When the optical fibre means is deformed as by the impingement of acoustic waves thereon, the heterodyned frequencies or carriers corresponding to the discontinuities will be frequency-modulated by the deformation of the optical fibres. Demodulation of the frequencymodulated carriers provides an indication of the acoustic signal incident upon the optical fibre means and an indication of an acoustic signal incident upon a portion of optical fibre between particulardiscontinuities n and (n+1) can be obtained from the difference between demodulated signals in respect of the nth and (n+ 1 )th carriers.
By way of example the present invention will now be described with reference to the accompanying drawings in which: Figure 1 is a schematic diagram showing an optical fibre deformation detection system;
Figure 2 shows an alternative arrangement of optical fibre means to that shown in the system of
Figure 1; and,
Figure 3 shows light signal waveforms occurring in the system of Figure 1.
Referring to Figure 1 of the drawings, a laser 1 generates coherent light which is frequencymodulated in a Bragg cell 2 by the output of a sweep oscillator 3 to provide a light signal having a saw-tooth waveform as shown in Figure 3. This coherent light signal is split into two beams by a first beam splitter 4. One of these beams passes through a second beam splitter 5 into an optical fibre 6 whereas the other beam, after reflection by a mirror 7, passes into a third beam splitter 8.
The light beam of saw-tooth frequencymodulation SW (Figure 3) which is transmitted down the optical fibre 6 is partially reflected back along the optical fibre at each of a number of equally-spaced partial discontinuities 9 to 1 6 along the optical fibre. The light RF reflected back along the optical fibre 6 from the discontinuity 9 is deflected by the second beam splitter 5 into the third beam splitter 8 where it is combined with the outgoing light signal SW transmitted along the optical fibre 6. The combined outgoing signal and the reflected signal which is delayed with respect thereto by a time period "t" are heterodyned as can be seen from Figure 3 to provide the waveform HC.
Each of the other reflected signals from discontinuities 10 to 16 will be delayed by a different delay period with respect to the preceding reflection and consequently the input to a detector/receiver 1 7 will comprise a set of heterodyned signals or carriers. These carrier signals will be frequency-modulated in the event of changes in length of the optical fibre sections between discontinuities 9 to 16, suchas due to the impingement of acoustic waves thereon when the system is utilised as a hydrophone.
These frequency-moduiated carrier signals will be demodulated in the receiver/detector 1 7 to
provide a set of demodulated signals appertaining to the fibre sections. The acoustic signal incident on any of the fibre sections can be extracted by taking the difference between the demodulated signals in respect of the nthand (n+1)th portions of the optical fibre.
An alternative form of optical fibre means is shown in Figure 2 which comprises a plurality of
lengths of fibre 18 to 25 which are star-coupled to the main optical fibre 26 along which the sawtooth signal is transmitted and the free ends of which are totally reflecting.
Claims (7)
1. An optical sensing system comprising optical fibre means arranged to be subjected to fibre deforming forces during use of the system and means for producing a coherent light signal for transmission along the optical fibre means, in which the optical fibre means comprises at points along its length respective discontinuities from which a light signal being transmitted along the optical fibre means will be partially or totally reflected back along the fibre means and combined with the light signal being transmitted down the optical fibre means so that heterodyning occurs between the interfering signals and in which the combined light signals are applied to demodulation means which provides an output indicative of the acoustic or other deforming force acting on the optical fibre means.
2. An optical sensing system as claimed in claim 1, in which the light signal transmitted down the opical fibre means is frequency modulated with a saw-tooth waveform so that the signals reflected back along the optical fibre means from the respective discontinuities will be delayed with respect to the saw-tooth signal transmitted along the optical fibre means by different delay periods dependent upon the location of the discontinuity along the optical fibre means and thus a set of heterodyned frequencies or carriers will be produced in accordance with these delay periods.
3. An optical sensing system as claimed in claim 1 or claim 2, in which the optical fibre means comprises a single optical fibre having partially-reflecting discontinuities equally spaced therealong.
4. An optical sensing system as claimed in claim 1 or claim 2, in which the optical fibre means comprises suitably coupled differing lengths of optical fibre the ends of which constitute totally-reflecting discontinuities.
5. An optical sensing system as claimed in any preceding claim, in which the coherent light signal is produced by a laser which is frequencymodulated in a Bragg cell or the equivalent by the output of a sweep oscillator before being applied to the optical fibre means.
6. An optical sensing system as claimed in claim 5, in which the frequency-modulated light signal output from the Bragg cell or its equivalent is split into two beams by a first beam spiitter/combiner, one of which beams passes through a second beam splitter/combiner before being fed into the optical fibre means and the other of said beams being applied to a third splitter/combiner where it is combined with reflected light signals from the optical fibre means before being applied to demodulation means.
7. An optical sensing system substantially as hereinbefore described with reference to the accompanying drawings.
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB08306135A GB2136113B (en) | 1983-03-05 | 1983-03-05 | Improvements relating to optical sensing systems |
AU25092/84A AU564486B2 (en) | 1983-03-05 | 1984-02-27 | Optical sensing system |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB08306135A GB2136113B (en) | 1983-03-05 | 1983-03-05 | Improvements relating to optical sensing systems |
Publications (2)
Publication Number | Publication Date |
---|---|
GB2136113A true GB2136113A (en) | 1984-09-12 |
GB2136113B GB2136113B (en) | 1986-08-06 |
Family
ID=10539071
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB08306135A Expired GB2136113B (en) | 1983-03-05 | 1983-03-05 | Improvements relating to optical sensing systems |
Country Status (2)
Country | Link |
---|---|
AU (1) | AU564486B2 (en) |
GB (1) | GB2136113B (en) |
Cited By (19)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2562741A1 (en) * | 1984-04-05 | 1985-10-11 | Exxon Production Research Co | FIBER OPTIC DATA COLLECTION SYSTEM |
EP0178814A2 (en) * | 1984-09-29 | 1986-04-23 | Plessey Overseas Limited | Optical sensing systems |
EP0216565A2 (en) * | 1985-09-10 | 1987-04-01 | Gec-Marconi Limited | Improvements relating to optical devices |
GB2182223A (en) * | 1985-10-23 | 1987-05-07 | Stc Plc | Optical fibre reflectometer |
JPS62111212A (en) * | 1985-09-10 | 1987-05-22 | ジーイーシー ― マルコニ リミテッド | Optical device |
US4708471A (en) * | 1985-02-27 | 1987-11-24 | U.S. Philips Corporation | Optical time-domain reflectometer using heterodyne reception |
GB2192984A (en) * | 1986-07-25 | 1988-01-27 | Plessey Co Plc | Optical sensing arrangement |
GB2199135A (en) * | 1986-12-10 | 1988-06-29 | Plessey Co Plc | Optical sensing arrangements |
FR2610465A1 (en) * | 1987-02-02 | 1988-08-05 | Photonetics | FIBER OPTIC SENSING DEVICE INVOLVING PROPER OPERATION |
GB2202046A (en) * | 1987-03-11 | 1988-09-14 | Plessey Co Plc | Optical fibre sensor arrangement |
GB2215055A (en) * | 1988-02-20 | 1989-09-13 | Stc Plc | Vibratory optical fibre sensor |
EP0404242A1 (en) * | 1989-06-23 | 1990-12-27 | AGIP S.p.A. | Method and device based on fibre-optic interferometer sensors, for analyzing the dynamic deformation of a structure or its components |
GB2238112A (en) * | 1986-11-11 | 1991-05-22 | British Aerospace | Measurement of distortion |
US5038618A (en) * | 1986-11-11 | 1991-08-13 | British Aerospace Public Limited Company | Measurement of distortion |
EP0464346A1 (en) * | 1990-06-12 | 1992-01-08 | Strabag Ag | Device to determine linear deformations of a medium along a measuring line |
US5187362A (en) * | 1988-12-06 | 1993-02-16 | British Telecommunications Public Limited Company | Loss detection in a branched optical fiber |
DE4132113A1 (en) * | 1991-09-26 | 1993-04-01 | Siemens Ag | Strain measurement pick=up for weighing appts. - operates on interferometer principle, and amplifies change in optical guide length by multiple reflections of beam |
US5227624A (en) * | 1990-12-06 | 1993-07-13 | Gec-Marconi Limited | Optical sensing systems with plural wavelengths and wavelength sensitive sensors |
CN106092305A (en) * | 2016-08-25 | 2016-11-09 | 上海交通大学 | Distributed optical fiber sensing system and vibration detection localization method thereof |
-
1983
- 1983-03-05 GB GB08306135A patent/GB2136113B/en not_active Expired
-
1984
- 1984-02-27 AU AU25092/84A patent/AU564486B2/en not_active Ceased
Cited By (29)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2562741A1 (en) * | 1984-04-05 | 1985-10-11 | Exxon Production Research Co | FIBER OPTIC DATA COLLECTION SYSTEM |
EP0178814A2 (en) * | 1984-09-29 | 1986-04-23 | Plessey Overseas Limited | Optical sensing systems |
EP0178814A3 (en) * | 1984-09-29 | 1986-08-06 | Plessey Overseas Limited | Optical sensing systems |
US4708471A (en) * | 1985-02-27 | 1987-11-24 | U.S. Philips Corporation | Optical time-domain reflectometer using heterodyne reception |
EP0216565A3 (en) * | 1985-09-10 | 1989-08-16 | Plessey Overseas Limited | Improvements relating to optical devices |
EP0216565A2 (en) * | 1985-09-10 | 1987-04-01 | Gec-Marconi Limited | Improvements relating to optical devices |
JPS62111212A (en) * | 1985-09-10 | 1987-05-22 | ジーイーシー ― マルコニ リミテッド | Optical device |
GB2182223A (en) * | 1985-10-23 | 1987-05-07 | Stc Plc | Optical fibre reflectometer |
GB2192984A (en) * | 1986-07-25 | 1988-01-27 | Plessey Co Plc | Optical sensing arrangement |
GB2192984B (en) * | 1986-07-25 | 1990-07-18 | Plessey Co Plc | Optical sensing arrangements |
GB2238112B (en) * | 1986-11-11 | 1991-10-09 | British Aerospace | Measurement of distortion |
GB2238112A (en) * | 1986-11-11 | 1991-05-22 | British Aerospace | Measurement of distortion |
US5038618A (en) * | 1986-11-11 | 1991-08-13 | British Aerospace Public Limited Company | Measurement of distortion |
GB2199135A (en) * | 1986-12-10 | 1988-06-29 | Plessey Co Plc | Optical sensing arrangements |
GB2199135B (en) * | 1986-12-10 | 1990-11-07 | Plessey Co Plc | Improvements relating to optical sensing arrangements |
EP0278820A2 (en) * | 1987-02-02 | 1988-08-17 | Photonetics | Fibre-optical detection apparatus involving proper-functioning control |
EP0278820A3 (en) * | 1987-02-02 | 1988-08-31 | Photonetics | Fibre-optical detection apparatus involving proper-functioning control |
FR2610465A1 (en) * | 1987-02-02 | 1988-08-05 | Photonetics | FIBER OPTIC SENSING DEVICE INVOLVING PROPER OPERATION |
GB2202046A (en) * | 1987-03-11 | 1988-09-14 | Plessey Co Plc | Optical fibre sensor arrangement |
US4891512A (en) * | 1988-02-20 | 1990-01-02 | Stc Plc | Thermo-optic differential expansion fiber sensor |
GB2215055A (en) * | 1988-02-20 | 1989-09-13 | Stc Plc | Vibratory optical fibre sensor |
GB2215055B (en) * | 1988-02-20 | 1992-04-01 | Stc Plc | Optical fibre sensor |
US5187362A (en) * | 1988-12-06 | 1993-02-16 | British Telecommunications Public Limited Company | Loss detection in a branched optical fiber |
EP0404242A1 (en) * | 1989-06-23 | 1990-12-27 | AGIP S.p.A. | Method and device based on fibre-optic interferometer sensors, for analyzing the dynamic deformation of a structure or its components |
EP0464346A1 (en) * | 1990-06-12 | 1992-01-08 | Strabag Ag | Device to determine linear deformations of a medium along a measuring line |
US5227624A (en) * | 1990-12-06 | 1993-07-13 | Gec-Marconi Limited | Optical sensing systems with plural wavelengths and wavelength sensitive sensors |
DE4132113A1 (en) * | 1991-09-26 | 1993-04-01 | Siemens Ag | Strain measurement pick=up for weighing appts. - operates on interferometer principle, and amplifies change in optical guide length by multiple reflections of beam |
CN106092305A (en) * | 2016-08-25 | 2016-11-09 | 上海交通大学 | Distributed optical fiber sensing system and vibration detection localization method thereof |
CN106092305B (en) * | 2016-08-25 | 2022-02-18 | 上海交通大学 | Distributed optical fiber sensing system and vibration detection positioning method thereof |
Also Published As
Publication number | Publication date |
---|---|
AU564486B2 (en) | 1987-08-13 |
AU2509284A (en) | 1984-09-06 |
GB2136113B (en) | 1986-08-06 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
732 | Registration of transactions, instruments or events in the register (sect. 32/1977) | ||
PCNP | Patent ceased through non-payment of renewal fee |
Effective date: 19940305 |