CN101776492B - Distributed fiber-sensing measuring method and device - Google Patents
Distributed fiber-sensing measuring method and device Download PDFInfo
- Publication number
- CN101776492B CN101776492B CN2009101566383A CN200910156638A CN101776492B CN 101776492 B CN101776492 B CN 101776492B CN 2009101566383 A CN2009101566383 A CN 2009101566383A CN 200910156638 A CN200910156638 A CN 200910156638A CN 101776492 B CN101776492 B CN 101776492B
- Authority
- CN
- China
- Prior art keywords
- point
- section
- signal
- optic cable
- sensing
- 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.)
- Expired - Fee Related
Links
Images
Abstract
The invention relates to a distributed fiber-sensing measuring method. The method comprises the following steps: a, laying sensing fiber cable, wherein the sensing fiber cable comprises a first segment and an overlap segment, one end of the first segment is connected with a measuring host, the overlap laying area comprises a second segment and a return segment, and the sensing fiber cable senses environment parameters, and different points on the second segment and the return segment can sense the parameters in the same position of the space; and b, processing signals, wherein signals returned from the first segment are processed to obtain the outside parameters of the area in which the first segment is positioned, and signals returned from points on the second segment and the return segment corresponding to the same space point are processed to obtain the parameters of the same space point. The invention also provides a distributed fiber-sensing measuring device. The invention has advantages of reducing the fluctuation at the tail end of the sensing fiber, increasing the actual measurement length, simpleness and convenience, economy and the like.
Description
Technical field
The present invention relates to a kind of distributed fiber-sensing measuring method and device.
Background technology
OTDR (optical time domain reflectometer) be utilize light in optical fiber backscattering and the optoelectronic integration instrument of the precision made, be widely used among the maintenance, construction of lightguide cable link, can carry out the measurement of transmission attenuation, the joint decay of fiber lengths, optical fiber and localization of fault etc.Distributed optical fiber sensing system is exactly a kind of novel real-time, distributed measurement system based on the OTDR technology.Present business-like distributed optical fiber sensing system has distributed optical fiber temperature sensing system based on the Raman scattering principle, based on distribution type fiber-optic temperature strain sensor-based system of spontaneous brillouin scattering principle etc.
The basic structure of distributed optical fiber sensing system comprises measures main frame, sensing optic cable and other external unit, as fire-fighting power supply, network transmission module etc.See also Fig. 1, a kind of sensing optic cable of distributed optical fiber sensing system lays synoptic diagram, and sensing optic cable is drawn from measuring main frame, lays along the measured zone line style.Wherein, sensing optic cable is a sensing element, is again transmission medium.When extraneous parameter (temperature, strain etc.) when affacting the sensor fibre in the sensing optic cable, the light wave characteristic of transmitting in optical fiber (amplitude, phase place, frequency etc.) changes, and can calculate the size of extraneous parameter to the measurement of light wave characteristic (amplitude, phase place, frequency etc.).
For distributed optical fiber sensing system, backscatter signals is because of the fibre loss exponential damping, and the noise of system remains unchanged substantially, thus the signal to noise ratio (S/N ratio) of system with the increase of measuring distance index decreased, as shown in Figure 2.To distributed optical fiber sensing system, temperature that calculates or strain fluctuating range are directly related with system signal noise ratio, and signal to noise ratio (S/N ratio) is high more, and the temperature or the strain fluctuating range that calculate are more little.In order to realize the reliability of temperature or strain measurement, the signal to noise ratio (S/N ratio) of system is greater than a fixed value.For the signal to noise ratio (S/N ratio) that guarantees system in the scope that requires, the overall measurement length of system just is subjected to certain restriction.
Simultaneously, in the long measurement point of measuring distance, the minor fluctuations of temperature or strain also can cause the systematic survey value than great fluctuation process, system is judged by accident easily.The temperature fluctuation noise of distributed optical fiber temperature sensing system at the 2km place as certain model is 2 ℃, but the temperature fluctuation noise at the 4km place will be increased to 4 ℃, like this in the bigger measurement point of measuring distance, the minor fluctuations of temperature also can cause the warning of system, makes instrument remote monitoring ability drop.
For reducing the temperature fluctuation noise, improve the signal to noise ratio (S/N ratio) of system, prior art adopts following several method to solve:
1, improves incident optical power.
Can improve the intensity of signal by the optical fiber of stronger light beam being gone in the optical cable, but improve the cost that incident optical power can increase system monitoring.
2, increase Measuring Time.
Increase Measuring Time, can increase progressive mean number of times, and then improve measurement accuracy measuring-signal.But the increase of Measuring Time can influence the response speed of system.
3, increase pulse width.
The increase of pulse width can improve the energy of system's incident optical signal, and then improves signal to noise ratio (S/N ratio).But the increase of pulse width will sacrificial system spatial resolution, make monitoring produce deviation to the measurement point locus.
As seen all there is deficiency in said method.
Summary of the invention
In order to solve above-mentioned deficiency of the prior art, the invention provides a kind of fiber cable laying method of distributed optical fiber sensing system.
For achieving the above object, the present invention adopts following technical scheme:
A kind of distributed fiber-sensing measuring method may further comprise the steps:
A, lay sensing optic cable:
Sensing optic cable comprises first section and overlay segment, and an end of first section connects measures main frame;
Described overlay segment comprises second section and back-turning section;
The extraneous parameter of sensing optic cable perception, wherein, the parameter that the difference on second section, back-turning section can aware space same position place;
B, signal Processing:
Handle described first section signal that returns, obtain the extraneous parameter in first section zone of living in;
Handle with the same space and put the signal that the point on corresponding second section and the back-turning section returns, thereby obtain parameter at described the same space point place.
The processing mode of the return signal of putting on further, described second section, back-turning section is:
Described the same space point is designated as the D point, and described second section last being designated as on E point, the described back-turning section to the nearest point of D point is designated as the F point to the nearest point of D point, and described E point and F point are and the corresponding point of described D point;
The signal that described E point of signal processing unit processes and F point return, thus the corresponding extraneous parameter of D point obtained.
As preferably, utilize method of weighted mean to handle and put the signal that the point on corresponding second section and the back-turning section returns, thereby obtain parameter at described the same space point place with the same space.
Further, during signal Processing, the weighting coefficient a of the some return signal on second section is: 0.5≤a＜1; The weighting coefficient b of the some return signal on the back-turning section is: b=1-a.
As preferably, described back-turning section length is not more than half of length overall of first section and second section.
The present invention also provides a kind of distributed fiber-sensing measuring device, comprises measuring main frame and sensing optic cable, measures main frame and comprises signal processing unit, is characterized in:
Described sensing optic cable comprises first section and overlay segment, and described first a section end connects measures main frame;
Described overlay segment comprises second section and back-turning section;
Signal processing unit, be used to handle described first section signal that returns, obtain the extraneous parameter in first section zone of living in, and processing and the same space put the signal that the point on corresponding second section and the back-turning section returns, thereby obtain parameter at described the same space point place.
The processing mode of the return signal of putting on further, described second section, back-turning section is:
Described the same space point is designated as the D point, and described second section last being designated as on E point, the described back-turning section to the nearest point of D point is designated as the F point to the nearest point of D point, and described E point and F point are and the corresponding point of described D point;
The signal that described E point of signal processing unit processes and F point return, thus the corresponding extraneous parameter of D point obtained.
As preferably, signal processing unit is done weighted mean with the signal that E point and F point return, as the corresponding signal of space D point, wherein, the weighting coefficient a of second section E point return signal with the pass of the weighting coefficient b of corresponding back-turning section F point return signal is: a+b=1, and a ≠ 1.
The weighting coefficient a of described second section E point return signal is: 0.4≤a＜1.
Described back-turning section length is not more than half of first section and the second segment length sum.
The present invention compared with prior art has following beneficial effect:
1, reduces the optical cable tail end and measure fluctuation.
Sensing optic cable tail end signal attenuation maximum is turned back sensing optic cable and is laid, and by the signal weighting of latter end sensing optic cable overlapping region is average, can effectively reduce the measurement fluctuation of sensing optic cable tail end, improves measurement accuracy.
2, increase measurement length.
In order to realize the reliability of temperature or strain measurement, the signal to noise ratio (S/N ratio) of system is greater than a fixed value.For the signal to noise ratio (S/N ratio) that guarantees system in the scope that requires, the overall measurement length of system just is subjected to certain restriction.And the mode that adopts the latter end optical cable to turn back and lay can effectively improve the signal to noise ratio (S/N ratio) of sensing optic cable tail end, thereby increase total measurement length.
3, easy, economical.
Reduce the measurement fluctuation of system by the turn back mode of laying of sensing optic cable, easy, economical, do not increase systematic survey main frame cost, the not response time of sacrificial system and spatial resolution yet.
Description of drawings
Fig. 1 lays synoptic diagram for sensing optic cable in the background technology;
Fig. 2 is the relation of signal to noise ratio (S/N ratio) and measuring distance in the optical fiber sensing system;
Fig. 3 lays synoptic diagram for sensing optic cable among the embodiment;
The temperature curve of Fig. 4 for utilizing the present invention and prior art to record respectively among the embodiment 1;
The temperature curve of Fig. 5 for utilizing the present invention and prior art to record respectively among the embodiment 2;
The strain curve of Fig. 6 for utilizing the present invention and prior art to record respectively among the embodiment 3;
The temperature curve of Fig. 7 for utilizing the present invention and prior art to record respectively among the embodiment 4;
The strain curve of Fig. 8 for utilizing the present invention and prior art to record respectively among the embodiment 5;
The strain curve of Fig. 9 for utilizing the present invention and prior art to record respectively among the embodiment 6.
Embodiment
Embodiment 1
See also Fig. 3, a kind of distributed fiber Raman scattering temperature sensing measurement mechanism comprises and measures main frame and sensing optic cable; Measure main frame and comprise signal processing unit;
Measure main frame and comprise light source, signal processing unit, optical fibre wavelength-division multiplex system and photoelectricity reception and amplification module etc.
Sensing optic cable comprises two parts: first section and overlay segment, first section length are 5000m; The sensing optic cable of overlay segment is turned back at the B point, forms second section AB and back-turning section BC, and second section AB and back-turning section BC press close to mutually; Wherein, the length of AB section and BC section is 500m;
The space a bit is designated as the D point in the overlay segment, second section of corresponding sensing optic cable and back-turning section each a bit, be designated as E point and F point respectively, second section upward the E point to D order nearest, on the back-turning section F point to D order nearest; Determine with second section of the corresponding sensing optic cable of space D point on the E process of ordering be prior art, and with the corresponding sensing optic cable back-turning section of D point on the F point with turn back that a B order apart from BF and E point and a B that turns back order identical apart from BE, then the position that F is ordered can be determined in the position of ordering by the E point and a B that turns back;
The signal that signal processing unit can return E point and F point is done weighted mean, as the size of the corresponding signal of space D point; Wherein, the weighting coefficient a and the b of AB section E point and BC section F point return signal are 0.5.
Present embodiment also provides a kind of distributed fiber Raman scattering temperature sensing measuring method, sees also Fig. 3, may further comprise the steps:
A, lay sensing optic cable
The long sensing optic cable of 6000m is drawn from measuring main frame O point, lays along measured zone, forms first section OA, and a section the length is 5000m; Sensing optic cable continues to lay, and turns back at a B point of turning back, and back-turning section BC and second section AB press close to mutually, forms overlay segment, so that back-turning section BC and second section AB can respond same ambient temperature field simultaneously; Wherein, the length of AB section and BC section is 500m; Fibre loss factor alpha=0.9dB/km;
In sensing optic cable the B point igniting of turning back, signal processing unit draws B point locus of living in by the analysis to the sensing optic cable return signal;
B, signal Processing:
To first section OA Signal Processing of sensing optic cable:
Signal processing unit is handled the signal that first section OA returns, and obtains the size of ambient temperature in the OA section measured zone; This signal processing is the state of the art, does not repeat them here;
To sensing optic cable overlay segment Signal Processing:
As the space in the overlay segment zone of living in a bit, be designated as the D point, second section of corresponding sensing optic cable and back-turning section each a bit, be designated as E point and F point respectively, on second section the E point to D order nearest, on the back-turning section F point to D order nearest; Wherein, E point, F point are identical with the distance that B is ordered; By the locus that B is ordered, determine the position that E point and F are ordered;
Determine with second section of the corresponding sensing optic cable of space D point on the E process of ordering be prior art, and with the corresponding sensing optic cable back-turning section of D point on the F point with turn back that a B order apart from BF and E point and a B that turns back order identical apart from BE, then the position that F is ordered can be determined in the position of ordering by the E point and a B that turns back;
Signal processing unit is done weighted mean with the signal that the AB section E point on the sensing optic cable and BC section F point return, and as the size of the corresponding outer signals of space D point, the weight coefficient of present embodiment E point and F point return signal is 0.5; By the processing of signal processing unit, obtain the size of the corresponding ambient temperature of space D point;
The value of the outer signals that space D point is corresponding is handled, and obtains corresponding ambient temperature, and this signal processing is the state of the art, does not repeat them here;
In like manner, can obtain the temperature of space each point correspondence in the sensing optic cable overlay segment zone of living in.
Utilize the temperature of said method measured zone OB section, the result who obtains utilizes result that prior art obtains shown in the last figure of Fig. 4 shown in Fig. 4 figure below.
As can be seen, in the measuring distance of preceding 5000m, present embodiment and of the prior art to record the result close substantially; But in the measuring distance between 5000m～5500m, the wave noise that present embodiment records temperature is significantly less than prior art.
As seen, be feasible by the latter end sensing optic cable temperature fluctuation noise that the method for laying reduces the sensing optic cable tail end of turning back.
The sensing optic cable latter end is turned back and is laid, and has reduced the temperature fluctuation amplitude of sensing optic cable tail end, thereby reduces the rate of false alarm of system, improves the reliability of system.
A kind of distributed fiber Raman scattering temperature sensing measurement mechanism, as different from Example 1:
Signal processing unit is respectively 0.9 and 0.1 to the weighting coefficient a and the b of AB section E point and BC section F point return signal when carrying out signal Processing.
Present embodiment also provides a kind of distributed fiber Raman scattering temperature sensing measuring method, and different with embodiment 1 is:
Signal processing unit is respectively 0.9 and 0.1 to the weighting coefficient a and the b of AB section E point and BC section F point return signal when carrying out signal Processing.
Utilize said method that the temperature of a certain moment measured zone OB section is measured, the result who obtains utilizes result that classic method obtains shown in the last figure of Fig. 5 shown in Fig. 5 figure below.
As can be seen, in the measuring distance of preceding 5000m, present embodiment and of the prior art to record the result close substantially; But in the measuring distance between 5000m～5500m, the wave noise that present embodiment records temperature is significantly less than prior art.
As seen, be feasible by the latter end sensing optic cable temperature fluctuation noise that the method for laying reduces the sensing optic cable tail end of turning back.
The sensing optic cable latter end is turned back and is laid, and has reduced the temperature fluctuation amplitude of sensing optic cable tail end, thereby reduces the rate of false alarm of system, improves the reliability of system.
Embodiment 3
A kind of distributed Brillouin scattering strain sensing measurement mechanism, as different from Example 1:
First section length of sensing optic cable is 18000m, and second section length with back-turning section is 2000m;
Measure main frame and be used to measure strain;
Second section weighting coefficient a and b with back-turning section respective point return signal is respectively 0.7 and 0.3.
Present embodiment also provides a kind of distribution type fiber-optic Brillouin scattering strain sensing measuring method, sees also Fig. 3, may further comprise the steps:
A, for this distributive fiber optic strain sensing device, fibre loss factor alpha=0.2dB/km;
The 2000m of sensing optic cable latter end adopts the twin-core single-mode fiber, adopts optical fiber splicer that twin-core fiber is welded together at optical fiber connector B point;
The above-mentioned sensing optic cable that has latter end 2000m twin-core single-mode fiber is drawn from measuring main frame O, lay along measured zone, form first section OA and overlay segment, wherein the length of first section OA is 18000m; Overlay segment comprises second section AB and back-turning section BC, and the length of AB section and BC section is 2000m, and connects at the B point, so that the signal of BC section can pass through AB section return measurement main frame; The use of twin-core single-mode fiber has guaranteed that AB section and BC section optical fiber closely presses close to, and can respond to same extraneous strain field simultaneously;
Exert pressure at a sensing optic cable B point of turning back, signal processing unit is analyzed by the signal that sensing optic cable is returned, and draws B point locus of living in;
B, signal Processing:
To first section OA Signal Processing of sensing optic cable:
Signal processing unit is handled the signal that first section OA of sensing optic cable returns, and obtains the strain of OA section regional each point of living in; This signal processing is the state of the art, does not repeat them here;
Processing to sensing optic cable overlay segment return signal:
As the space in the overlay segment zone of living in a bit, be designated as the D point, second section of corresponding sensing optic cable and back-turning section each a bit, be designated as E point and F point respectively, on second section the E point to D order nearest, on the back-turning section F point to D order nearest; Wherein, E point, F point are identical with the distance that B is ordered; By the locus that B is ordered, determine the position that E point and F are ordered;
Determine with second section of the corresponding sensing optic cable of space D point on the E process of ordering be prior art, and with the corresponding sensing optic cable back-turning section of D point on the F point with turn back that a B order apart from BF and E point and a B that turns back order identical apart from BE, then the position that F is ordered can be determined in the position of ordering by the E point and a B that turns back;
The signal that sensing optic cable AB section E point and BC section F point return is done weighted mean, and as the size of the corresponding outer signals of space D point, the weight coefficient a and the b of present embodiment E point and F point return signal are respectively 0.7 and 0.3; By the processing of signal processing unit, obtain the size of the corresponding extraneous strain of D point;
The value of the outer signals that space D point is corresponding is handled, and obtains corresponding extraneous strain, and this signal processing is the common practise of this area, does not repeat them here;
In like manner, obtain the strain of each point correspondence in the sensing optic cable overlay segment zone of living in.
Utilize result that this method records shown in Fig. 6 figure below, utilize result that classic method records shown in the last figure of Fig. 6.
As can be seen, in the measuring distance before 18000m, this method and prior art are close substantially; But in the measuring distance between 18000m～20000m, the wave noise of the strain that this method records is significantly less than prior art.
As seen, be feasible by the latter end sensing optic cable strain wave moving noise that the method for laying reduces the sensing optic cable tail end of turning back.
The sensing optic cable latter end is turned back and is laid, and has reduced the strain fluctuating range of sensing optic cable tail end, thereby reduces the rate of false alarm of system, improves the reliability of system.
Embodiment 4
A kind of distributed fiber Raman scattering temperature sensing measurement mechanism, as different from Example 1: the length that sensing optic cable is first section is 4000m, second section length with back-turning section is 1000m;
Signal processing unit is respectively 0.8 and 0.2 to the weighting coefficient a and the b of AB section E point and BC section F point return signal when carrying out signal Processing.
Present embodiment also provides a kind of distributed fiber Raman scattering temperature sensing measuring method, as different from Example 1:
In step a, the sensing optic cable of 6000m is drawn from measuring main frame O point, lays along measured zone, and the length of first section OA section of sensing optic cable is 4000m; Sensing optic cable continues to lay, and turns back at a B point of turning back, and wherein, the length of AB section and BC section is 1000m;
In step b, signal processing unit is respectively 0.8 and 0.2 to the weighting coefficient a and the b of AB section E point and BC section F point return signal when carrying out signal Processing.
Utilize said method that the temperature of a certain moment measured zone OB section is measured, the result who obtains utilizes the classic method sensing optic cable not have to turn back the result who obtains when laying shown in the last figure of Fig. 7 shown in Fig. 7 figure below.
As can be seen, in the measuring distance before 4000m, the latter end sensing optic cable does not have to turn back and lays and have the temperature measurement result that obtains when laying of turning back close substantially; But in the measuring distance between 4000m～5000m, the turn back temperature fluctuation noise of the measurement result that obtains under the laying state of sensing optic cable is significantly less than and does not have the temperature fluctuation noise of turning back when laying.
Embodiment 5
A kind of distributed fiber Raman scattering temperature sensing measurement mechanism, as different from Example 1: the length that sensing optic cable is first section is 3000m, second section length with back-turning section is 1500m;
Signal processing unit is respectively 0.6 and 0.4 to the weighting coefficient a and the b of AB section E point and BC section F point return signal when carrying out signal Processing.
Present embodiment also provides a kind of distributed fiber Raman scattering temperature sensing measuring method, as different from Example 1:
In step a, the sensing optic cable of 6000m is drawn from measuring main frame O point, lays along measured zone, and the length of first section OA section of sensing optic cable is 3000m; Sensing optic cable continues to lay, and turns back at a B point of turning back, and wherein, the length of AB section and BC section is 1500m;
In step b, signal processing unit is respectively 0.6 and 0.4 to the weighting coefficient a and the b of AB section E point and BC section F point return signal when carrying out signal Processing.
Utilize said method that the temperature of a certain moment measured zone OB section is measured, the result who obtains utilizes the classic method sensing optic cable not have to turn back the result who obtains when laying shown in the last figure of Fig. 8 shown in Fig. 8 figure below.
As can be seen, in the measuring distance before 3000m, the latter end sensing optic cable does not have to turn back and lays and have the temperature measurement result that obtains when laying of turning back close substantially; But in the measuring distance between 3000m～4500m, the turn back temperature fluctuation noise of the measurement result that obtains under the laying state of sensing optic cable is significantly less than and does not have the temperature fluctuation noise of turning back when laying.
Embodiment 6
A kind of distributed fiber Raman scattering temperature sensing measurement mechanism, as different from Example 5: signal processing unit all is functions of measuring distance z to the weighting coefficient a and the b of AB section E point and BC section F point return signal when carrying out signal Processing, be a=0.7*exp (0.0002* (z-3000)), b=1-a, wherein, the span of z is [3000,4500].
Present embodiment also provides a kind of distributed fiber Raman scattering temperature sensing measuring method, and different with embodiment 5 is:
In step b, signal processing unit all is functions of measuring distance z to the weighting coefficient a and the b of AB section E point and BC section F point return signal when carrying out signal Processing, present embodiment a is exponential taper function: a=0.7*exp (0.0002* (z-3000)), wherein, the span of z is [3000,4500], b=1-a.Then, through calculating, the span of a is: [0.52,0.7], the span of b is: [0.3,0.48]
Utilize said method that the temperature of a certain moment measured zone OB section is measured, the result who obtains utilizes the classic method sensing optic cable not have to turn back the result who obtains when laying shown in the last figure of Fig. 9 shown in Fig. 9 figure below.
As can be seen, in the measuring distance before 3000m, the latter end sensing optic cable does not have to turn back and lays and have the temperature measurement result that obtains when laying of turning back close substantially; But in the measuring distance between 3000m～4500m, the turn back temperature fluctuation noise of the measurement result that obtains under the laying state of sensing optic cable is significantly less than and does not have the temperature fluctuation noise of turning back when laying.
Signal processing unit both can be constant to the weighting coefficient of second section AB section E point and back-turning section BC section F point return signal when carrying out signal Processing, also can be variable, all can reduce tail end temperature fluctuation noise.
Above-mentioned embodiment should not be construed as limiting the scope of the invention.Key of the present invention is: the overlay segment that sensing optic cable comprises first section, is made up of second section and back-turning section, handle with the same space and put the signal that the point on corresponding second section and the back-turning section returns, thereby obtaining the parameter at described the same space point place, then is prior art for the processing of first section return signal.Under the situation that does not break away from spirit of the present invention, any type of change that the present invention is made all should fall within protection scope of the present invention.
Claims (10)
1. distributed fiber-sensing measuring method may further comprise the steps:
A, lay sensing optic cable:
Sensing optic cable comprises first section and overlay segment, and an end of first section connects measures main frame;
Described overlay segment comprises second section and back-turning section;
The extraneous parameter of sensing optic cable perception, wherein, the parameter that the difference on second section, back-turning section can aware space same position place;
B, signal Processing:
Handle described first section signal that returns, obtain the extraneous parameter in first section zone of living in;
Handle with the same space and put the signal that the point on corresponding second section and the back-turning section returns, thereby obtain parameter at described the same space point place.
2. method according to claim 1 is characterized in that: the processing mode of the return signal of putting on described second section, back-turning section is:
Described the same space point is designated as the D point, and described second section last being designated as on E point, the described back-turning section to the nearest point of D point is designated as the F point to the nearest point of D point, and described E point and F point are and the corresponding point of described D point;
The signal that described E point of signal processing unit processes and F point return, thus the corresponding extraneous parameter of D point obtained.
3. method according to claim 2, it is characterized in that: signal processing unit is done weighted mean with the signal that E point and F point return, as the corresponding signal of space D point, wherein, the weighting coefficient a of E point return signal with the pass of the weighting coefficient b of corresponding F point return signal is: a+b=1, and a ≠ 1.
4. method according to claim 3 is characterized in that: the weighting coefficient a of described second section E point return signal is: 0.4≤a＜1.
5. method according to claim 1 and 2 is characterized in that: described back-turning section length is not more than half of first section and the second segment length sum.
6. a distributed fiber-sensing measuring device comprises and measures main frame and sensing optic cable, wherein, measures main frame and comprises signal processing unit, it is characterized in that:
Described sensing optic cable comprises first section and overlay segment, and described first a section end connects measures main frame;
Described overlay segment comprises second section and back-turning section;
Signal processing unit, be used to handle described first section signal that returns, obtain the extraneous parameter in first section zone of living in, and processing and the same space put the signal that the point on corresponding second section and the back-turning section returns, thereby obtain parameter at described the same space point place.
7. measurement mechanism according to claim 6 is characterized in that: the processing mode of the return signal of putting on described second section, back-turning section is:
Described the same space point is designated as the D point, and described second section last being designated as on E point, the described back-turning section to the nearest point of D point is designated as the F point to the nearest point of D point, and described E point and F point are and the corresponding point of described D point;
The signal that described E point of signal processing unit processes and F point return, thus the corresponding extraneous parameter of D point obtained.
8. device according to claim 7, it is characterized in that: signal processing unit is done weighted mean with the signal that E point and F point return, as the corresponding signal of space D point, wherein, the weighting coefficient a of second section E point return signal with the pass of the weighting coefficient b of corresponding back-turning section F point return signal is: a+b=1, and a ≠ 1.
9. device according to claim 8 is characterized in that: the weighting coefficient a of described second section E point return signal is: 0.4≤a＜1.
10. according to claim 6 or 7 described devices, it is characterized in that: described back-turning section length is not more than half of first section and the second segment length sum.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN2009101566383A CN101776492B (en) | 2009-12-29 | 2009-12-29 | Distributed fiber-sensing measuring method and device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN2009101566383A CN101776492B (en) | 2009-12-29 | 2009-12-29 | Distributed fiber-sensing measuring method and device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN101776492A CN101776492A (en) | 2010-07-14 |
| CN101776492B true CN101776492B (en) | 2011-11-16 |
Family
ID=42513009
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN2009101566383A Expired - Fee Related CN101776492B (en) | 2009-12-29 | 2009-12-29 | Distributed fiber-sensing measuring method and device |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN101776492B (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101957244B (en) * | 2010-09-27 | 2013-04-10 | 苏州光格设备有限公司 | Distributed optical fiber sensing system with high space resolving power |
| CN103346620A (en) * | 2013-07-22 | 2013-10-09 | 国家电网公司 | Cable temperature monitoring system based on distribution type optical fiber temperature detection sensor |
Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6079875A (en) * | 1997-09-04 | 2000-06-27 | Alcatel | Apparatus for measuring the temperature of an object with a temperature sensor and method of making the temperature sensor |
| CN101109660A (en) * | 2007-08-03 | 2008-01-23 | 聚光科技（杭州）有限公司 | Temperature measurement system for high temperature liquid |
| CN201297967Y (en) * | 2008-11-26 | 2009-08-26 | 上海华魏自动化设备有限公司 | Loop detection type distributed optical fiber temperature sensor |
| US7603009B2 (en) * | 2003-07-03 | 2009-10-13 | Schlumberger Technology Corporation | Double-ended distributed temperature sensing systems |
-
2009
- 2009-12-29 CN CN2009101566383A patent/CN101776492B/en not_active Expired - Fee Related
Patent Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6079875A (en) * | 1997-09-04 | 2000-06-27 | Alcatel | Apparatus for measuring the temperature of an object with a temperature sensor and method of making the temperature sensor |
| US7603009B2 (en) * | 2003-07-03 | 2009-10-13 | Schlumberger Technology Corporation | Double-ended distributed temperature sensing systems |
| CN101109660A (en) * | 2007-08-03 | 2008-01-23 | 聚光科技（杭州）有限公司 | Temperature measurement system for high temperature liquid |
| CN201297967Y (en) * | 2008-11-26 | 2009-08-26 | 上海华魏自动化设备有限公司 | Loop detection type distributed optical fiber temperature sensor |
Also Published As
| Publication number | Publication date |
|---|---|
| CN101776492A (en) | 2010-07-14 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN106595776B (en) | A kind of more physical quantity sensor-based systems of distribution type fiber-optic and method | |
| CN102636217B (en) | Sensing device based on joint detection of Brillouin optical time domain analysis and Mach-Zehnder interference | |
| CN103591971B (en) | A kind of localization method of fiber grating | |
| CN102506912A (en) | Optical fiber distributed disturbance sensor | |
| CN103439766B (en) | A kind of space division multiplexing method of multi-core fiber | |
| US8734011B2 (en) | Distributed optical fiber temperature sensor based on optical fiber delay | |
| CN109595470B (en) | Distributed pipeline detection method | |
| CN102147236A (en) | Fully distributed optical fiber strain and vibration sensing method and sensor | |
| CN102829807A (en) | BOTDA (Brillouin Optical Time Domain Analyzer) and POTDR (Polarization Optical Time Domain Reflectometer) combined distributed type optical fiber sensing system | |
| KR102292226B1 (en) | Fiber-optic acoustic sensor module apparatus and system using coherent optical time-domain reflectormeter method | |
| KR20090120032A (en) | Fire data detector using optical fiber | |
| KR101465788B1 (en) | optical sening system having dual core | |
| CN102393220A (en) | SMS (single mode-multimode-single mode) optical fiber structural duplexing sensor | |
| JP2013185922A (en) | Optical fiber vibration sensor | |
| CN101701844B (en) | Optical fiber vibration sensing system and using method thereof based on double Mach-Zehnder interferometers | |
| CN101776492B (en) | Distributed fiber-sensing measuring method and device | |
| CN204680159U (en) | Optical fiber distributed type reservoir dam monitoring system | |
| CN201521291U (en) | Underground distributed temperature sensor | |
| CN201688927U (en) | Distributed optical fiber sensor measurement device | |
| CN102735272A (en) | Barrier-searchable Brillouin optical time domain analyzer | |
| CN104655193B (en) | Brillouin optical coherent reflectometer based on noise modulation | |
| CN202267497U (en) | Multiplexing sensor with SMS (single-mode, multi-mode and single-mode) fiber structures | |
| CN206959867U (en) | A kind of optical signal collection system based on Rayleigh scattering | |
| CN102353339A (en) | Optical time domain reflection (OTDR)-fiber Bragg grating (FBG) structure damage detection system having single-fiber single-ended structure | |
| CN201540180U (en) | Novel pressure sensing system |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| C06 | Publication | ||
| PB01 | Publication | ||
| C10 | Entry into substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| C14 | Grant of patent or utility model | ||
| GR01 | Patent grant | ||
| C41 | Transfer of patent application or patent right or utility model | ||
| TR01 | Transfer of patent right |
Effective date of registration: 20160120 Address after: 310052, No. 1, No. 351, Changhe Road, Changhe Road, Changhe Road, Hangzhou, Zhejiang, Binjiang District, 5 Patentee after: Hangzhou Anyuan Technology Co., Ltd. Address before: Hangzhou City, Zhejiang province Binjiang District 310052 shore road 760 Patentee before: Focused Photonics (Hangzhou) Inc. |
|
| CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20111116 Termination date: 20181229 |
|
| CF01 | Termination of patent right due to non-payment of annual fee |