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Physical Sciences Inc. 20 New England Business Center Andover, MA 01810
Physical
Sciences Inc.
Laser-Based Standoff Methane Sensors for
Enhancing Coal Miner Safety
Mickey Frish1, Clinton Smith1, Richard Wainner1 ,
James Rutherford2, Steve Chancey2, Paul Wehnert2
1Physical Sciences Inc., 20 New England Business Center, Andover MA
2Heath Consultants 9030 Monroe Rd., Houston TX
Pittcon 2015
New Orleans, LA
March 8, 2015
VG15-020
This material is based upon work supported by The Centers for Disease Control and Prevention. Any opinions, findings and conclusions
or recommendations expressed in this material are those of the author(s) and do not necessarily reflect the views of the CDC.
Physical Sciences Inc.
Overview
 Motivation
– Enhance miner safety by supplementing current methane measurement
practices with remote methane detection
 Technology: Backscatter Laser Sensor
– Hand-held sensor locates areas of increased methane
• Demonstrated in research and working mines.
• Standoff range up to > 150 ft.
• Measures path integrated concentration.
– Sensor pair maps methane concentrations via tomography
• Map actual concentration.
• Demonstrated in coal mine face simulation lab.
 Summary
VG15-020-1
Physical Sciences Inc.
 During mining operations, methane emanates from the sidewalls and
ceilings.
– Can create pockets that are explosion or breathing hazards
 Point sensors utilized for methane measurement might not detect
pockets trapped in areas that are difficult to access
 Remote methane detection can provide additional knowledge
regarding the location, volume and extent of methane pockets,
enhancing miner safety.
Benefit of Remote Methane Detection
VG15-020-2
Physical Sciences Inc.
VG15-020
Technology Platform:
The Remote Methane Leak Detector (RMLD)
 Like a flashlight, laser beam
Illuminates a surface up to
150 feet distant
 Senses target gas between
surveyor and illuminated surface
 >3000 in use for natural gas (CH4) distribution pipeline leak surveying
– leak sensitivity comparable to commonly-used flame ionization detectors
 Being adopted for CO2 pipeline monitoring at sequestration sites
-3
Physical Sciences Inc.
Handheld Use Scenarios
VG15-020
 Portable tool warns before entering a hazardous area
− Including through doors and windows
 Searches for methane pockets in inaccessible areas such
as high roof
 Manually scans mine face for abnormally high methane
-4
Physical Sciences Inc.
Tests in Research Coal Mine
 Hung a transparent 1 m2 Tedlar bag against a representative coal
mine wall
– Filled w/ 2.1% methane, nominal 12.5 cm path  ~2600 ppm-m.
– Directed laser beam at selected wall areas around and through the bag at
ranges of 50 ft., 75 ft., 100 ft., and 150 ft.
– Achieved acceptable laser return signal and detected the increased
methane from all ranges
– Established good return signals for different wall compositions
 Performed a controlled detection test using 2.1% methane released
from pressurized cylinder
VG15-020-5
Physical Sciences Inc.
Targeting a Representative Coal Mine Wall
1) Brown
stone
2) Grey
stone
3) Brown/grey
stone
4) 2.1%
methane
bag
5) coal
8) coal
7) coal6)
Brown
stone
 Laser beam was directed at each of the 8 locations
 Surface of coal mine face was wet
 Measurements made from distance of 50, 75, 100, 150 ft.
 Backscatter signal strengths are sufficient to detect methane from
distances > 200 ft.
1) 2)
3)
4)
5)
6) 7)
8)
VG15-020-6
Physical Sciences Inc.
Detected Methane from Remote Distance
 2.1% methane concentration in bag against mine wall
– Bag thickness (i.e., methane path) is ~5 inches
 Able to detect the methane at all distances measured
 2.1% methane pocket (5” deep) detectable from >200 ft.
– Power law extrapolation based on return signal
VG15-020
4000
3500
3000
2500
2000
1500
1000
500
0
50 70 90 110 130 150
Distance From Wall (ft.)
0
10
20
30
40
50
60
70
80
90
2
1
r
1f at Methane Bag Vs. DistancePath Integrated Concentration of
Methane Bag Vs. Distance
50 70 90 110 130 150
Distance From Wall (ft.) L-3129
-7
Physical Sciences Inc.
Rock Types Have Little Impact on Signals
 Aimed RMLD away from the methane bag
 Brown stone, grey stone, and coal all return similar laser power
– Path integrated concentration increases with distance due to ambient methane
• Positions #5, #6, #8 exhibit anomalies at 150 ft. range due to laser beam sampling
only a portion of the methane bag
– Beam diameter @ 150’ is ~75 cm
VG15-020
1200
1000
800
600
400
200
0
50 90 110 130 150
Distance From Wall (ft.)
70 50 90 110 130 150
Distance From Wall (ft.)
70
0
20
40
60
80
100
120
140
160
Methane Concentration for Different Surfaces Vs. Distance
L-3130
1. Brown stone 2. Grey stone 3. Brown/grey stone 5. Coal
6. Brown stone 7. Coal 8. Coal
-8
Physical Sciences Inc.
Controlled 2.1% Methane Release:
Search for Source
Search wall area away
from source
Search wall area away
from source
Methane Pocket
Concentration increases
near methane source
 Manually scanned from 50 ft. range
 Methane pocket created by release from bottle was readily detected
Methane released in back corner
VG15-020-9
Physical Sciences Inc.
Dual-Sensor Tomography
 Operator scans two tripod-mounted laser beams across the mine face
– Employs two sensors on rotational stages to make in-plane horizontal scans over the region of
interest.
– Pathlength retrieval with rangefinders.
 Log signals to rugged laptop for software processing
 A Graphical User Interface computer displays methane spatial concentration
VG15-020-10
Physical Sciences Inc.
Tomography: Coal Mine Face Simulation Lab Tests
• Performed tomographic scans with varying
flow rates and leak sources (2.1% methane)
− 20 ft. distance from wall
− Single source (0.5 L/min)
− Single source (>2 L/min)
− Three sources (> 2 L/min)
• 2.1% methane flow at 2 L/min is equivalent
to 0.08 scfh pure methane
− Less than a pilot light
X2X1
X=RMLD + laser rangefinder
mounted on tripod (~4ft. High)
40ft.roomdepth
16.5 ft. room width
Control cables
Simulated coal face with leak(s)
single source
Three sources
X1
X2
leak sources
VG15-020-11
Physical Sciences Inc.
Tomographic Scan of Single Leak Source – 20 ft. away
Single source high flow (>2L/min.)Single source low flow (0.5 L/min.)
 Leak source is located in the middle of the face; Background methane is less than 15 ppmv
– Methane collects near far wall (conforms with historical observation)
 Tomographic low flow peak is ~25 ppmv; high flow peak is ~60 ppmv
– Note: These values are 2-3 orders-of-magnitude below concentrations of concern at coal
mine faces
 Electrochemical sensors deployed for comparison
– Detected high flow (~2% methane) when placed at leak source
• Could not detect methane several inches from leak source
– Could not detect low (0.5L/min.) flow
VG15-020-12
Physical Sciences Inc.
Three sources high flow (sources near scan plane)
Tomographic Scan of Three Leak Sources – 20 ft. away
X2X1
X=RMLD + laser rangefinder
mounted on tripod (~4ft. High)
40ft.roomdepth
16.5 ft. room width
Control cables
Simulated coal face with leak(s)
Three sources
 2.1% methane; Flow rate > 2 L/min.
 Peak of 0.01% (100 ppm) detected from stronger (upstream) source
– All three sources are distinguishable
VG15-020-13
Physical Sciences Inc.
Coal Mine Face Simulation Lab Tests – 40 ft. away
X2X1
X=RMLD + laser rangefinder
mounted on tripod (~4ft. High)
40ft.roomdepth
16.5 ft. room width
Control cables
 2.1% methane flow rate of > 2 L/min.
 Peak of 0.08% (800 ppm) detected from stronger
(upstream) source
 Two sources are distinguishable
Three sources high flow (sources near scan plane)
VG15-020-14
Physical Sciences Inc.
Summary
1. Successful remote methane detection inside an experimental mine
– Single laser backscatter sensor readily identified areas of increased
methane from distances > 150 ft.
– Successfully located the source of a controlled 2.1% methane release from a
distance of 50 ft.
• Tests were done against wet coal faces and a fresh coal mine face
2. Tomographic scans located and quantified methane near
simulated mine faces from distances of 20 ft. to 40 ft.
– Identified releases of 2.1% methane at 0.5 L/min and 2 L/min
– Sensitivity > 100x better than concentrations of concern in mines
– New application for backscatter TDLAS laser sensor systems.
VG15-020-15
Physical Sciences Inc.
Acknowledgments
VG15-020
Research funded by CDC/NIOSH Contract #200-2011-40565
and Heath Consultants Inc.
-16
Physical Sciences Inc.
Questions?
VG15-020-17
Physical Sciences Inc.
Machine Mounted Mapping Tool Scenario
VG15-020
 Automated tool installed on mining machine that continuously
maps methane concentrations at mine face
-18
Physical Sciences Inc.
VG15-020
Absorption Spectroscopy Fundamentals
• Gas molecules absorb light at
specific colors (“absorption lines”)
Beer-Lambert law
Iν = Iνo exp [S(T) g( - o) N]
where:
 = optical frequency (= c/l)
o = line center frequency
g() = lineshape function
 = path length
N = absorbing species number density
S(T) = temperature dependent linestrength
Iνo = unattenuated laser intensity
I = laser intensity with absorption
DI = change in intensity (= I0-I)
c = speed of light
l = wavelength of light
Absorbance = - ℓn (I /Io)
≈ DI/I0 ( with small DI)
CH4 Spectrum
Mid-IR fundamental
Near-IR overtone
200x linestrength advantage is
the mid-IR appeal
(when deployed judiciously)
-19

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Laser-Based Standoff Methane Sensors for Enhancing Coal Miner Safety

  • 1. Physical Sciences Inc. 20 New England Business Center Andover, MA 01810 Physical Sciences Inc. Laser-Based Standoff Methane Sensors for Enhancing Coal Miner Safety Mickey Frish1, Clinton Smith1, Richard Wainner1 , James Rutherford2, Steve Chancey2, Paul Wehnert2 1Physical Sciences Inc., 20 New England Business Center, Andover MA 2Heath Consultants 9030 Monroe Rd., Houston TX Pittcon 2015 New Orleans, LA March 8, 2015 VG15-020 This material is based upon work supported by The Centers for Disease Control and Prevention. Any opinions, findings and conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect the views of the CDC.
  • 2. Physical Sciences Inc. Overview  Motivation – Enhance miner safety by supplementing current methane measurement practices with remote methane detection  Technology: Backscatter Laser Sensor – Hand-held sensor locates areas of increased methane • Demonstrated in research and working mines. • Standoff range up to > 150 ft. • Measures path integrated concentration. – Sensor pair maps methane concentrations via tomography • Map actual concentration. • Demonstrated in coal mine face simulation lab.  Summary VG15-020-1
  • 3. Physical Sciences Inc.  During mining operations, methane emanates from the sidewalls and ceilings. – Can create pockets that are explosion or breathing hazards  Point sensors utilized for methane measurement might not detect pockets trapped in areas that are difficult to access  Remote methane detection can provide additional knowledge regarding the location, volume and extent of methane pockets, enhancing miner safety. Benefit of Remote Methane Detection VG15-020-2
  • 4. Physical Sciences Inc. VG15-020 Technology Platform: The Remote Methane Leak Detector (RMLD)  Like a flashlight, laser beam Illuminates a surface up to 150 feet distant  Senses target gas between surveyor and illuminated surface  >3000 in use for natural gas (CH4) distribution pipeline leak surveying – leak sensitivity comparable to commonly-used flame ionization detectors  Being adopted for CO2 pipeline monitoring at sequestration sites -3
  • 5. Physical Sciences Inc. Handheld Use Scenarios VG15-020  Portable tool warns before entering a hazardous area − Including through doors and windows  Searches for methane pockets in inaccessible areas such as high roof  Manually scans mine face for abnormally high methane -4
  • 6. Physical Sciences Inc. Tests in Research Coal Mine  Hung a transparent 1 m2 Tedlar bag against a representative coal mine wall – Filled w/ 2.1% methane, nominal 12.5 cm path  ~2600 ppm-m. – Directed laser beam at selected wall areas around and through the bag at ranges of 50 ft., 75 ft., 100 ft., and 150 ft. – Achieved acceptable laser return signal and detected the increased methane from all ranges – Established good return signals for different wall compositions  Performed a controlled detection test using 2.1% methane released from pressurized cylinder VG15-020-5
  • 7. Physical Sciences Inc. Targeting a Representative Coal Mine Wall 1) Brown stone 2) Grey stone 3) Brown/grey stone 4) 2.1% methane bag 5) coal 8) coal 7) coal6) Brown stone  Laser beam was directed at each of the 8 locations  Surface of coal mine face was wet  Measurements made from distance of 50, 75, 100, 150 ft.  Backscatter signal strengths are sufficient to detect methane from distances > 200 ft. 1) 2) 3) 4) 5) 6) 7) 8) VG15-020-6
  • 8. Physical Sciences Inc. Detected Methane from Remote Distance  2.1% methane concentration in bag against mine wall – Bag thickness (i.e., methane path) is ~5 inches  Able to detect the methane at all distances measured  2.1% methane pocket (5” deep) detectable from >200 ft. – Power law extrapolation based on return signal VG15-020 4000 3500 3000 2500 2000 1500 1000 500 0 50 70 90 110 130 150 Distance From Wall (ft.) 0 10 20 30 40 50 60 70 80 90 2 1 r 1f at Methane Bag Vs. DistancePath Integrated Concentration of Methane Bag Vs. Distance 50 70 90 110 130 150 Distance From Wall (ft.) L-3129 -7
  • 9. Physical Sciences Inc. Rock Types Have Little Impact on Signals  Aimed RMLD away from the methane bag  Brown stone, grey stone, and coal all return similar laser power – Path integrated concentration increases with distance due to ambient methane • Positions #5, #6, #8 exhibit anomalies at 150 ft. range due to laser beam sampling only a portion of the methane bag – Beam diameter @ 150’ is ~75 cm VG15-020 1200 1000 800 600 400 200 0 50 90 110 130 150 Distance From Wall (ft.) 70 50 90 110 130 150 Distance From Wall (ft.) 70 0 20 40 60 80 100 120 140 160 Methane Concentration for Different Surfaces Vs. Distance L-3130 1. Brown stone 2. Grey stone 3. Brown/grey stone 5. Coal 6. Brown stone 7. Coal 8. Coal -8
  • 10. Physical Sciences Inc. Controlled 2.1% Methane Release: Search for Source Search wall area away from source Search wall area away from source Methane Pocket Concentration increases near methane source  Manually scanned from 50 ft. range  Methane pocket created by release from bottle was readily detected Methane released in back corner VG15-020-9
  • 11. Physical Sciences Inc. Dual-Sensor Tomography  Operator scans two tripod-mounted laser beams across the mine face – Employs two sensors on rotational stages to make in-plane horizontal scans over the region of interest. – Pathlength retrieval with rangefinders.  Log signals to rugged laptop for software processing  A Graphical User Interface computer displays methane spatial concentration VG15-020-10
  • 12. Physical Sciences Inc. Tomography: Coal Mine Face Simulation Lab Tests • Performed tomographic scans with varying flow rates and leak sources (2.1% methane) − 20 ft. distance from wall − Single source (0.5 L/min) − Single source (>2 L/min) − Three sources (> 2 L/min) • 2.1% methane flow at 2 L/min is equivalent to 0.08 scfh pure methane − Less than a pilot light X2X1 X=RMLD + laser rangefinder mounted on tripod (~4ft. High) 40ft.roomdepth 16.5 ft. room width Control cables Simulated coal face with leak(s) single source Three sources X1 X2 leak sources VG15-020-11
  • 13. Physical Sciences Inc. Tomographic Scan of Single Leak Source – 20 ft. away Single source high flow (>2L/min.)Single source low flow (0.5 L/min.)  Leak source is located in the middle of the face; Background methane is less than 15 ppmv – Methane collects near far wall (conforms with historical observation)  Tomographic low flow peak is ~25 ppmv; high flow peak is ~60 ppmv – Note: These values are 2-3 orders-of-magnitude below concentrations of concern at coal mine faces  Electrochemical sensors deployed for comparison – Detected high flow (~2% methane) when placed at leak source • Could not detect methane several inches from leak source – Could not detect low (0.5L/min.) flow VG15-020-12
  • 14. Physical Sciences Inc. Three sources high flow (sources near scan plane) Tomographic Scan of Three Leak Sources – 20 ft. away X2X1 X=RMLD + laser rangefinder mounted on tripod (~4ft. High) 40ft.roomdepth 16.5 ft. room width Control cables Simulated coal face with leak(s) Three sources  2.1% methane; Flow rate > 2 L/min.  Peak of 0.01% (100 ppm) detected from stronger (upstream) source – All three sources are distinguishable VG15-020-13
  • 15. Physical Sciences Inc. Coal Mine Face Simulation Lab Tests – 40 ft. away X2X1 X=RMLD + laser rangefinder mounted on tripod (~4ft. High) 40ft.roomdepth 16.5 ft. room width Control cables  2.1% methane flow rate of > 2 L/min.  Peak of 0.08% (800 ppm) detected from stronger (upstream) source  Two sources are distinguishable Three sources high flow (sources near scan plane) VG15-020-14
  • 16. Physical Sciences Inc. Summary 1. Successful remote methane detection inside an experimental mine – Single laser backscatter sensor readily identified areas of increased methane from distances > 150 ft. – Successfully located the source of a controlled 2.1% methane release from a distance of 50 ft. • Tests were done against wet coal faces and a fresh coal mine face 2. Tomographic scans located and quantified methane near simulated mine faces from distances of 20 ft. to 40 ft. – Identified releases of 2.1% methane at 0.5 L/min and 2 L/min – Sensitivity > 100x better than concentrations of concern in mines – New application for backscatter TDLAS laser sensor systems. VG15-020-15
  • 17. Physical Sciences Inc. Acknowledgments VG15-020 Research funded by CDC/NIOSH Contract #200-2011-40565 and Heath Consultants Inc. -16
  • 19. Physical Sciences Inc. Machine Mounted Mapping Tool Scenario VG15-020  Automated tool installed on mining machine that continuously maps methane concentrations at mine face -18
  • 20. Physical Sciences Inc. VG15-020 Absorption Spectroscopy Fundamentals • Gas molecules absorb light at specific colors (“absorption lines”) Beer-Lambert law Iν = Iνo exp [S(T) g( - o) N] where:  = optical frequency (= c/l) o = line center frequency g() = lineshape function  = path length N = absorbing species number density S(T) = temperature dependent linestrength Iνo = unattenuated laser intensity I = laser intensity with absorption DI = change in intensity (= I0-I) c = speed of light l = wavelength of light Absorbance = - ℓn (I /Io) ≈ DI/I0 ( with small DI) CH4 Spectrum Mid-IR fundamental Near-IR overtone 200x linestrength advantage is the mid-IR appeal (when deployed judiciously) -19

Notes de l'éditeur

  1. Work funded through the CDC Office of Mine Safety and Health Research (OMSHR). Want to thank Gerrit Goodman and his colleagues for participating in and assisting with exps. Photo here is from a research coal mine operated by CDC National Institute for Occupational Safety and Health (NIOSH) in Brewston, PA (outside Pittsburgh).
  2. -Despite best efforts and procedures in place, accidents in coal mines do happen. -consequently, coal industry is interested in supplementing current technology to enhance miner safety -We’re funded to evaluate our backscatter laser sensor product inside coal mines to estimate what value it can bring to the coal mine industry. Should also point out that these same experiments (that you will see) were performed in a working coal mine but are not presented today.
  3. RMLD is commercial product sold by Heath Consultants for nat’l gas pipeline surveying. Laser expands by 0.5 cm /ft.
  4. Key Test here is to evaluate laser return signal both as function of distance from coal mine wall and wall composition. To give a sense of effectiveness: Vast majority of applications of interest here (as an enhanced safety tool) generally deal with distances <50 ft.
  5. -Before we were looking at path integrated methane measurements. -There is also interest in spatially mapping the methane concentration.
  6. Not sure if tomography is appropriate for coal mines but can be applied to other situations (e.g., quantifitying gas leaks above ground…perhaps in processing facilities)
  7. Call out Gerrit Goodman and Andrew Mazzella