<node id="682957">
  <nid>682957</nid>
  <type>event</type>
  <uid>
    <user id="27707"><![CDATA[27707]]></user>
  </uid>
  <created>1751311684</created>
  <changed>1751311746</changed>
  <title><![CDATA[PhD Defense by Haripriya Rajagopalan]]></title>
  <body><![CDATA[<p><strong>Haripriya Rajagopalan</strong><br><em>(Advisor: Prof. Tim Lieuwen]</em></p><p><em>will defend a doctoral thesis entitled,</em></p><p><strong>Predicting Turbulent Burning Velocity of High </strong><img src="data:image/png;base64,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" width="27" height="23"><strong>Flames</strong></p><p><em>On</em></p><p><strong>Wednesday, July 9 at 1 p.m.&nbsp;</strong><br><strong>&nbsp;Food Processing Technology Building, Auditorium 102</strong><br><em>North Avenue Research Area, 640 Strong St NW&nbsp;</em></p><p><strong>Abstract</strong><br>Hydrogen (H2) is increasingly being explored as an energy carrier to support a decarbonized energy economy.&nbsp;Both the direct utilization of H2&nbsp;and its blending with conventional fuels such as natural gas are under active consideration to meet the stringent emissions regulations faced by the energy sector.&nbsp;Among the combustion parameters affected by H2, the turbulent burning velocity (<em>S</em>T) plays a central role in determining combustor operability&nbsp;limits,&nbsp;inﬂuencing&nbsp;blowoff,&nbsp;ﬂashback,&nbsp;and&nbsp;combustion&nbsp;instabilities. The&nbsp;impact of H2 on <em>S</em>T becomes particularly complex under lean conditions and at high pressures, where&nbsp;traditional&nbsp;scaling&nbsp;models&nbsp;for&nbsp;<em>S</em>T,&nbsp;based&nbsp;largely&nbsp;on&nbsp;root-mean-square&nbsp;turbulent&nbsp;velocity&nbsp;ﬂuctuations&nbsp;(<img src="data:image/png;base64,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" width="32" height="19">)&nbsp;and&nbsp;the&nbsp;unstretched&nbsp;laminar&nbsp;ﬂame&nbsp;speed&nbsp;(<em>S</em>L,0),&nbsp;are&nbsp;inadequate.</p><p>This&nbsp;dissertation&nbsp;focuses&nbsp;on&nbsp;the&nbsp;co-development&nbsp;of&nbsp;data-driven&nbsp;and&nbsp;physics-based&nbsp;modeling&nbsp;frameworks&nbsp;to&nbsp;predict&nbsp;<em>S</em>T in&nbsp;H2-fueled&nbsp;premixed&nbsp;ﬂames&nbsp;based&nbsp;on&nbsp;leading-point&nbsp;concepts. A&nbsp;physics-based&nbsp;correlation&nbsp;is&nbsp;developed&nbsp;for&nbsp;the&nbsp;turbulent&nbsp;global&nbsp;consumption&nbsp;speed <em>S</em>T,GC, rooted in Damko¨hler’s paradigm, of the form:</p><p><img src="data:image/png;base64,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" width="343" height="44"></p><p>where, <img src="data:image/png;base64,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" width="29" height="21"><em> </em>and&nbsp;<em>S</em>L,ref&nbsp;are&nbsp;generalized&nbsp;forms&nbsp;of&nbsp;the&nbsp;conventionally&nbsp;used&nbsp;root-mean-square turbulent&nbsp;velocity&nbsp;ﬂuctuation&nbsp;(<img src="data:image/png;base64,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" width="32" height="19">)&nbsp;and&nbsp;the&nbsp;laminar&nbsp;unstretched&nbsp;ﬂame&nbsp;speed&nbsp;(<em>S</em>L,0),&nbsp;respectively.&nbsp;Unlike traditional deﬁnitions, in this study, these parameters are determined based on leading-point scaling and data-driven ﬁtting of large experimental databases.&nbsp;<em>S</em>T,GC measurements were acquired at a high-pressure Bunsen burner facility across different&nbsp;H2&nbsp;fuel&nbsp;blends—(H2<em>/</em>CO,&nbsp;H2<em>/</em>CH4,&nbsp;H2<em>/</em>CO<em>/</em>CH4<em>/</em>N2)—operated&nbsp;at&nbsp;gas&nbsp;turbine–relevant pressures (1–20 bar) and preheat temperatures (300–450 K). The global turbulent consumption&nbsp;speed&nbsp;(<em>S</em>T,GC), representing&nbsp;the&nbsp;average&nbsp;conversion&nbsp;rate&nbsp;of&nbsp;premixed&nbsp;reactants&nbsp;to combustion&nbsp;products,&nbsp;is&nbsp;measured&nbsp;at&nbsp;the&nbsp;facility&nbsp;using&nbsp;OH*&nbsp;chemiluminescence,&nbsp;while&nbsp;the ﬂow&nbsp;ﬁeld&nbsp;turbulence&nbsp;characteristics&nbsp;are&nbsp;quantiﬁed&nbsp;using&nbsp;laser&nbsp;Doppler&nbsp;velocimetry&nbsp;(LDV). The primary focus of this work is on the <em>S</em>T<em>,</em>GC&nbsp;measurements of H2<em>/</em>CH4&nbsp;fuel blends.</p><p>The <em>S</em>T correlation is derived by ﬁrst applying feature selection techniques to identify the most relevant non-dimensional parameters governing <em>S</em>T,GC, based on their predictive&nbsp;importance&nbsp;across&nbsp;the&nbsp;dataset.&nbsp;This&nbsp;analysis&nbsp;reveals&nbsp;that&nbsp;a&nbsp;small&nbsp;subset&nbsp;of&nbsp;features - namely,&nbsp;the&nbsp;turbulence&nbsp;intensity <img src="data:image/png;base64,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" width="32" height="19"><em>/S</em>L,max,&nbsp;normalized&nbsp;bulk&nbsp;ﬂow&nbsp;Reynolds&nbsp;number&nbsp;(<img src="data:image/png;base64,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" width="27" height="20">),&nbsp;and&nbsp;a&nbsp;time&nbsp;scale&nbsp;ratio&nbsp;associated&nbsp;with&nbsp;the&nbsp;ﬂame&nbsp;leading&nbsp;edge&nbsp;(<em>Ka</em>max&nbsp;=&nbsp;<em>τS</em>L<em>,</em>max&nbsp;<em>/τ</em>ﬂow)&nbsp;- captures&nbsp;most&nbsp;of&nbsp;the&nbsp;observed&nbsp;variance&nbsp;in&nbsp;<em>S</em>T,GC. This&nbsp;is&nbsp;followed&nbsp;by&nbsp;symbolic&nbsp;regression, which&nbsp;produced&nbsp;an&nbsp;interpretable&nbsp;functional&nbsp;form&nbsp;capturing&nbsp;the&nbsp;nonlinear&nbsp;relationship&nbsp;between&nbsp;the&nbsp;selected&nbsp;features&nbsp;and&nbsp;<em>S</em>T,GC.&nbsp;We&nbsp;observe&nbsp;that&nbsp;the&nbsp;optimal <img src="data:image/png;base64,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" width="33" height="21">scales&nbsp;as:</p><p><img src="data:image/png;base64,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" width="397" height="39"></p><p>Unlike&nbsp;conventional&nbsp;Reynolds&nbsp;number&nbsp;considerations&nbsp;in&nbsp;<em>S</em>T,GC&nbsp;correlations,&nbsp;we&nbsp;hypothesize&nbsp;that&nbsp;this&nbsp;scaling&nbsp;highlights&nbsp;the&nbsp;inﬂuence&nbsp;of&nbsp;intermittent, extreme&nbsp;velocity&nbsp;ﬂuctuation events, which occur in the tails of the velocity distribution and become more pronounced with increasing <img src="data:image/png;base64,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" width="27" height="20">.&nbsp;These extreme events are hypothesized to represent ﬂow velocity ﬂuctuations&nbsp;interacting&nbsp;with&nbsp;the&nbsp;turbulent&nbsp;ﬂame&nbsp;front&nbsp;at&nbsp;the&nbsp;leading&nbsp;points. Some&nbsp;evidence for the inﬂuence of <img src="data:image/png;base64,iVBORw0KGgoAAAANSUhEUgAAACgAAAAeCAMAAABpA6zvAAAAAXNSR0IArs4c6QAAAJxQTFRFAAAAAAAAAAA6AABmADo6ADpmADqQAGa2OgAAOjoAOjo6OjpmOmaQOma2OpDbZgAAZjoAZjo6ZmaQZpC2ZpDbZrbbZrb/kDoAkDo6kGY6kGZmkJC2kLbbkLb/kNv/tmYAtmY6tpA6tpBmttvbttv/tv//25A625Bm27Zm27aQ27a229u229vb2////7Zm/9uQ/9u2/9vb//+2///bv26eQwAAAAF0Uk5TAEDm2GYAAAAJcEhZcwAAFiUAABYlAUlSJPAAAAAZdEVYdFNvZnR3YXJlAE1pY3Jvc29mdCBPZmZpY2V/7TVxAAABO0lEQVQ4T9VTy0KDMBBkEWy0KFatFa2iVZH4CEj+/9/cF8VChZMH98AjO8zOTEgQ/K+qsyMAiJL1VrZ/WA4t1FnyhKv+7cZAfPtBj3axB+evu8WvzcIg93z9+deROBxDNe9c/DKyhIOXILAGriY0OTgk2XobARcwo25liHiscpk5CfSr8J6ASoxJb3CL4ucBtzLVqeCRGUGlyNkpR2vemrjFkbXKsMGdyjnFcCkNFVLAaR/nV+iFLzp4Fvj3DJIBYZNSKtsQC6I/Pmcr/AzhpVAIpGmtaFbSy5HDP+owUdPObrNSveKL5baIXNUr4yvNa1LKyAljaYA1OP4zNJc647wrgxBrTqSPRdSVgeiOVuwZHhzJis2Ee86DOOhKvOiG9Zs/3kWiehnBKcQN96j/UUFD7eRfKj4humBf369YGhTP+r/IAAAAAElFTkSuQmCC" width="27" height="20"><em> </em>on the tail events of turbulent velocity distributions is provided through ﬂow characterization using LDV studies.</p><p>Meanwhile, the data clearly indicates that <em>S</em>L<em>,</em>ref closely corresponds to the maximum laminar burning velocity, <em>S</em>L<em>,</em>max, of critically stretched ﬂames, with only a weak dependence&nbsp;on&nbsp;the&nbsp;Karlovitz&nbsp;number&nbsp;(<em>Ka</em>max).&nbsp;These&nbsp;ﬁndings&nbsp;provide&nbsp;useful&nbsp;insights&nbsp;into&nbsp;datasets&nbsp;showing&nbsp;the&nbsp;important&nbsp;effects&nbsp;of&nbsp;hydrogen&nbsp;composition&nbsp;and&nbsp;pressure&nbsp;on&nbsp;the&nbsp;turbulent&nbsp;ﬂame speed, as well as the underlying ﬂuid mechanic and chemical kinetic roots of these dependencies.</p><p>&nbsp;</p><p>.&nbsp; <strong>Committee</strong></p><ul><li>Prof. Tim Lieuwen – School of Aerospace Engineering (advisor)</li><li>Prof. Adam Steinberg– School of Aerospace Engineering</li><li>Prof. P.K. Yeung – School of Aerospace Engineering</li><li>Dr. Jackie Chen – Senior Scientist, Sandia National Labs</li><li>Dr Debolina Dasgupta – Research Scientist, Argonne National Lab</li></ul><p>&nbsp;</p>]]></body>
  <field_summary_sentence>
    <item>
      <value><![CDATA[Predicting Turbulent Burning Velocity of High Flames]]></value>
    </item>
  </field_summary_sentence>
  <field_summary>
    <item>
      <value><![CDATA[<p><strong>Predicting Turbulent Burning Velocity of High </strong><img src="data:image/png;base64,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" width="27" height="23"><strong>Flames</strong></p>]]></value>
    </item>
  </field_summary>
  <field_time>
    <item>
      <value><![CDATA[2025-07-09T13:00:00-04:00]]></value>
      <value2><![CDATA[2025-07-09T15:00:00-04:00]]></value2>
      <rrule><![CDATA[]]></rrule>
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