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Open Path Optical Sensing of Particulate Matter
Byung J. Kim, Mike KemmeRavi Varma, Ram Hashmonay
Background
• ERDC-CERL• Environmental Quality Technology User
Requirements• Fugitive dust (PM) monitoring technology• No standards, no emission factor data• Filter method/ in-plume• Collaboration: ARCADIS, U of Illinois• Strategic Environmental Research and
Development Program (SERDP)
Concept Development
• ARCADIS• Oct 2002, Dec 2003-Jan 2004, Sep 2004• OP-FTIR spectrometers, Visible
spectrometers, and APS• Dust , Fog oil, Graphite • Yuma Proving Ground• Artillery back blast, Tracked vehicle
movement, Rotary & Fixed wing aircraft landing and take-off
Sample plumes with ORS instrumentation and in situaerodynamic particle sizer (APS)
Quantify mass flux and emission factors
Field campaigns to measure military unique
dust sources
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Particle Diameter [µm]
Mas
s C
once
ntra
tion
[RU
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Lower OP-FTIR Upper OP-FTIR Average APS
Rapid time-resolved (seconds) PM type identification and size-distribution determination
Movie of Dust Plume Measured with OP-FTIR (mean particle
size of several microns)
Press to skip
Movie of Fogoil Plume Measured with OP-FTIR
(sub-micron mean particle size)
Press to skip
Derivative-like Features in Fingerprint Region
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Extin
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Dust Plume Features Measured by a Monostatic OP-FTIR System
[Explanation of figure on next slide]
Dust Plume Features Measured by a Monostatic OP-FTIR System
• Typical dust plume absorbance spectra from active OP-FTIR (70 m optical pathlength)
• Specific derivative-like features (example near 900 cm-1are unique for dust
• Smoothed baseline (in green) contains mass distribution information for the plume
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Wavelength (micron)
Ext
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Midac-2002/10/14 Unisearch-2002/10/14IMACC-2003/12/17 IMACC-2004/9/24
Comparison of Dust Plume Measurements by OP-FTIR
Explanation of figure on next slide
Comparison of Dust Plume Measurements by OP-FTIR
• Comparison of dust plume extinction spectra from different instruments and experiments reveals similarities
• Unisearch & Midac OP-FTIR exhibit identical extinction features because they are from the same dust sample
• 2003 and 2004 samples (both from IMACC OP-FTIR) contain smaller particles, evident from the sloping of the baselines towards the smaller wavelength region
• Strong absorption feature around 11 micron is present in all four samples
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Wavelength (micron)
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Spectral Feature for Dust Particles
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Wavelength (micron)
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Spectral Feature for Fogoil Particles
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Wavelength (micron)
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Baseline Shift for Dust PM Plumes
(2004 experiments)
Baseline Shift for Fogoil PM Plumes
(2004 experiments)
Inverse Mie TheoryMass Distribution Retrieval
• Inverse Mie Theory algorithm was used to retrieve mass distribution for PM plumes
• Following figures show example dust and fogoil plumes observed by both the OP-FTIR and the APS, and uses values averaged over the duration of the selected plumes
• Baseline points were selected from the OP-FTIR spectra, avoiding atmospheric carbon dioxide and water absorption regions and the specific absorption features of the PM plume materials
• LIDAR extinction values measured for a plume maximum were used as extinction input point at 650 nm and the baseline of extinction spectra from OP-FTIR were interpolated to get slope between 650 nm and 2 micron
• Where no absorption features are present, the elevation of the baseline is due to the scattering of the light by plume particles
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Measured OP-FTIR Data
Reconstructed Algorithm Fit
OP-FTIR Spectrum
Inverse Mie TheoryMass Distribution Retrieval
OP-FTIR Data and Algorithm Input and Fit for Dust
Inverse Mie TheoryMass Distribution Retrieval
OP-FTIR Data and Algorithm Input and Fit for Fogoil
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Measured OP-FTIR DataReconstructed Algorithm FitOP-FTIR Spectrum
Inverse Mie TheoryMass Distribution Retrieval
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dM/d
logD
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OP-FTIR SizeDist. Retrieval
Size Distribution Retrieval for Dust with APS Data
Inverse Mie TheoryMass Distribution Retrieval
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dM/d
logD
pAverage APS Data
OP-FTIR Size Dist.Retrieval
Size Distribution Retrieval for Fogoil with APS Data
Measurement Approach for Ongoing SERDP Project
Explanation of figures in next couple of slides
Measurement Approach
• By situating hard targets over the measurement domain we obtain: – reliable inversion of the lidar equation – better penetration into the dust plume in the
dense near-field conditions and significant extension of the lidar measurement distance
Measurement Approach
• OP-FTIR, OP-UV-VIS spectroscopy and real-time point dust monitors (APS) used concurrently with lidar and wind measurements, in a downwind vertical plane from the studied activity.
• This measurement configuration will provide important information for converting the lidarextinction distribution data into mass concentration distributions and thus in conjunction with the wind measurements, reliable mass fluxes