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        <article-title>Relationship between LII Signal and Soot Volume Fraction - Effect of Primary Particle Diameter Polydispersity</article-title>
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        <contrib contrib-type="author">
          <string-name>Fengshan Liu</string-name>
          <email>Fengshan.Liu@nrc-cnrc.gc.ca</email>
          <xref ref-type="aff" rid="aff0">0</xref>
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        <contrib contrib-type="author">
          <string-name>Gregory J. Smallwood</string-name>
          <email>Greg.Smallwood@nrc-cnrc.gc.ca</email>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>National Research Council</institution>
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          <addr-line>Building M-9, 1200 Montreal Road, Ottawa, ON.</addr-line>
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          <country country="CA">Canada</country>
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      <abstract>
        <p>It is shown numerically that for a polydisperse primary soot particles the soot temperature derived in two-color LII is biased towards the temperature of those larger and hotter particles. As smaller particles cool faster than larger ones, smaller particles gradually 'disappear', leading to a decrease soot volume fraction determined by the two-color LII. Based on numerically results, the relationship between LII signal and soot volume fraction can be summarized as: (1) It is linear in the two-color LII during and shortly after the laser pulse in the low-fluence regime (2) It is linear in the two-color LII only briefly around the peak of the laser pulse in the high-fluence regime (3) It is in general non-linear in the conventional LII method 5th international workshop on Laser-Induced Incandescence May 9-11, 2012, Palais des Congrès, Le Touquet, France</p>
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