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Open Path Optical Sensing of Particulate Matter Byung J. Kim, Mike Kemme Ravi Varma, Ram Hashmonay

Open Path Optical Sensing of Particulate MatterConcept Development •ARCADIS • Oct 2002, Dec 2003-Jan 2004, Sep 2004 • OP-FTIR spectrometers, Visible spectrometers, and APS •

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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]

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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)

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  • Movie of Fogoil Plume Measured with OP-FTIR

    (sub-micron mean particle size)

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  • Derivative-like Features in Fingerprint Region

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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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    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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    Spectral Feature for Fogoil Particles

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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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    0 2 4 6 8 10 12 14 16 18 20Aerodynamic Diameter (micron)

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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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    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