metrological assessment of distributed temperature sensing techniques · · 2016-10-24sensing...
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Laboratoire commun de métrologie LNE-Cnam
G. Failleau , O. Beaumont, R. Razouk, F. Martinot, B. Courthial,J. Bertrand, S. Delepine-Lesoille, S. Plumeri, B. Hay
Metrological Assessment of
Distributed Temperature
Sensing Techniques
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Introduction
2G. Failleau, 12th of October 2016
Management of the nuclear wastes repository sites
Management of the nuclear power plants, and hydrolics dams and dikes
Thermal instrumentation and metrology, development of new calibration capabilities
Distributed Temperature Sensing
Partnership LNE – EDF - Andra
http://www.decommissioning-emrp.eu /
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Outlines
3G. Failleau, 12th of October 2016
I. Fundamentals on Distributed Temperature Sensing by Raman Scattering
II. Development of testing facilities suitable to DTS devices
III. Assessment of a few metrological performances
IV. Conclusions and outcomes
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Distributed Temperature Sensing
4G. Failleau, 12th of October 2016
Raman ScatteringV
irtua
l en
erg
y le
ve
ls
En
erg
y leve
l
Vib
ratio
nn
al s
tate
sIn
tensity
� Inelastic collision (Excitating photon Vs. Crystal lattice)
� Energetic transition between two vibrationnal state s of the lattice
� Emission of a Stokes radiation : most probable case (i.e Bose-Einstein distribution)
� Emission of an Anti-Stokes radiation : less probable, depending of the temperature
The ratio of Stokes & Anti-Stokes intensities is dependant with the temperature
2
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5G. Failleau, 12th of October 2016
Distributed Temperature SensingApplication to the optical fibres
Acrylate coating (dia. 250 µm)
Core (dia. 50 µm)
Cladding (dia. 125 µm)
� Technologies based on the Optical Time Domain Reflectometry (OTDR)
� The optical fibre is the sensitive element
� Multimode optical fibres used as sensors (Telecom. standard)
� Fibres interrogated by nano-second pulsed laser (typically 1064 nm)
� Continuous measurement along the whole length of the optical fibre
� Absolute spatial resolution (sampling resolution) of 1 m
� Measurement range : 0 – 30 km
� Typical operating range : -5 – 90 °C (depending of the optical fibre intrinsic properties)
Tem
pera
ture
Distance
Measured temperature profile
Pulsed laser source
Detection
Laser pulse (pump)
Backscattered light
Sampling resolution
Signal processingDisplay / Data file
InterrogatorSensing optical fibre
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6G. Failleau, 12th of October 2016
Distributed Temperature Sensing
Temperature monitoring by conventionnal thermometer s
� A few hundreds/thousands sensors by structure� ~100 € - 200 € per sensor
Underground nuclear waste repository sites
Dikes
Dams
But also… Tunnels, gas & oil pipelines, etc…
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7G. Failleau, 12th of October 2016
Distributed Temperature Sensing
Temperature monitoring by optical fibres
� A few hundreds/thousands measurements over the fibre length� ~0,20 € / m
Underground nuclear waste repository sites
Dikes
Dams
But also… Tunnels, gas & oil pipelines, etc…
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Expected sources of error
8G. Failleau, 12th of October 2016
Interrogator
Temperature Mechanical constraints
Ionizing radiations
Source
Detection
Temperature
Humidity and chemical pollutions
The interrogator and the optical fibre are influenced by the environmental conditions :
� Changes of the optical fibre properties (attenuation factor, refractive index variations ,…)
� Influence of the temperature on the interrogator optics and internal reference
� Mechanical constraints on the fibre (curvature radius…)
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Achievements
DTS devices commercially available but lack of stan dardization
9G. Failleau, 12th of October 2016
� To identify relevant metrological characteristics to be evaluated
� To develop experimental facilities suitable to DTS devices
� To define experimental methods and protocol for testing the DTS devices
� To provide a benchmark on DTS devices for the users
Finaly, to propose new standards devoted to the DTS methods
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Outlines
10G. Failleau, 12th of October 2016
I. Fundamentals on Distributed Temperature Sensing by Raman Scattering
II. Development of testing facilities suitable to DTS devices
III. Assessment of a few metrological performances
IV. Conclusions and outcomes
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Calibration facilities
11G. Failleau, 12th of October 2016
� Implementation of a reference optical fibre (length of 5, 10, 15, or 20 km)
� Interrogator and optical fibre thermally decoupled (thermal enclosures)
� Thermal conditions rigorously controlled (trueness, stability, temperature homogeneity)
� Mechanical constraints controlled ( « constraint free » optical fibre wound )
� Temperature stability within 0,02 °C
� Temperature homogeneity within 0,1 °C
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0 1 2
Tem
pé
ratu
e,
°C
Temps, hTime, h
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12G. Failleau, 12th of October 2016
Calibration facilities
� Implementation of a reference optical fibre free from any mechanical constraint
� Operating range : ~ 0°C up to 90 °C
� Temperature stability within 0.05 °C over 5 hours, thermal homogeneity within 0.2 °C over 23 m
Horizontal furnace with 25 m of length
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5 15 25 35 45 55
Tem
pera
ture
, °C
Time, h
static PRT
mobile PRT
0.01 C
Thermal stability at 23 °C
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Outlines
13G. Failleau, 12th of October 2016
I. Fundamentals on Distributed Temperature Sensing by Raman Scattering
II. Development of testing facilities suitable to DTS devices
III. Assessment of metrological performances
IV. Conclusions and outcomes
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14G. Failleau, 12th of October 2016
Metrological characteristics
� Spatial resolutionThe shortest length of optical fibre which has to be immersed into a thermally homogenousenvironment for measuring the true temperature value.Depending of the sampling interval, optical pulse width .
� Spatial dispersionThe lowest temperature gradient which can be measured over a length of optical fibre corresponding to 10 times the spatial resolution.Depending of the optical pulse broadening (chromatic & intermodal dispersions), signal-to-noise ratio, spatial resolution, integration time.
� Temporal dispersionRepeatability of the temperature measurement one one given point of the optical fibre over 10 successive measuring cycles over time.Depending of the optical pulse broadening, signal-to-noise ratio , spatial resolution.
� Trueness errorComparison of the temperature measured by the DTS-Raman to the temperature measured by a Standard Platinum Resistance thermometer (SPRT)Depending of the interrogator temperature, optical fibre temperature.
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15G. Failleau, 12th of October 2016
Benchmark on Raman-DTS devices
Device A Device B
� Quantifying the metrological characteristics of DTS -Raman devices
� Proposing a relevant comparison to the end-users
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°C)
Position (m)
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Similar temperature traces obtained at 23 °C, but…
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16G. Failleau, 12th of October 2016
Benchmark on Raman-DTS devices
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23 °C 40 °C
60 °C
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40 °C 60 °C
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Device A Device B
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40 °C 60 °C
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23 °C (initial) 3 °C
23 °C 40 °C
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17G. Failleau, 12th of October 2016
Device A Device B
Benchmark on Raman-DTS devices
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dis
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°C)
Position (m)
23 °C (initial) 3 °C
23 °C 40 °C
60 °C
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tep
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)
Optical fibre length immersed at 0 °C (m)
Sampling 1 m - Resolution 1 m
Sampling 0.5m - Resolution 1 m
Sampling 0.5 m - Resolution 2 m
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Sampling 1 m
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reso
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nt
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Outlines
18G. Failleau, 12th of October 2016
I. Fundamentals on Distributed Temperature Sensing by Raman Scattering
II. Development of testing facilities suitable to DTS devices
III. Assessment of metrological performances
IV. Conclusions and outcomes
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Conclusions & outcomes
19G. Failleau, 12th of October 2016
� Development of calibration facilities suitable with DTS
� Metrological characteristics identified
� Influence factors identified
� Development of a characterization protocol suitable to DTS
� Benchmark on DTS devices to be performed
� Toward a normalized frame (procedures to be proposed to IEC)
Our goal is to ensure the metrological traceability to the measurements performed by DTS
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20G. Failleau, 12th of October 2016
Thank you for your attention
… Any question(s) ?