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</o:shapelayout></xml><![endif]--></head><body lang=EN-US link=blue vlink=purple><div class=WordSection1><p class=MsoNormal align=center style='text-align:center'><b><span style='font-size:16.0pt;line-height:115%;font-family:"Tahoma","sans-serif";color:black'>MS Thesis Defense<o:p></o:p></span></b></p><p class=MsoNormal align=center style='text-align:center'><b><span style='font-size:16.0pt;line-height:115%;font-family:"Tahoma","sans-serif";color:black'>A Numerical Study of the Flow and Heat Transfer in the Near Field of a Cylindrical Bubble <o:p></o:p></span></b></p><p class=MsoNormal align=center style='text-align:center'><b><span style='font-size:16.0pt;line-height:115%;font-family:"Tahoma","sans-serif";color:black'>Moving in a Narrow Channel<o:p></o:p></span></b></p><p class=MsoNormal align=center style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto;text-align:center;line-height:150%'><b><span style='font-size:14.0pt;line-height:150%;font-family:"Tahoma","sans-serif";color:black'>Shashank Natesh</span></b><b><span style='font-size:12.0pt;line-height:150%;font-family:"Tahoma","sans-serif";color:black'><o:p></o:p></span></b></p><p class=MsoNormal align=center style='margin-bottom:0in;margin-bottom:.0001pt;text-align:center;line-height:normal'><b><span style='font-size:12.0pt;color:black'>Date:</span></b><span style='font-size:12.0pt;color:black'> <b>Friday, August 24, 2012</b><o:p></o:p></span></p><p class=MsoNormal align=center style='margin-bottom:0in;margin-bottom:.0001pt;text-align:center;line-height:normal'><span style='font-size:12.0pt;color:black'><o:p> </o:p></span></p><p class=MsoNormal align=center style='margin-bottom:0in;margin-bottom:.0001pt;text-align:center;line-height:normal'><b><span style='font-size:12.0pt;color:black'>Location:</span></b><span style='font-size:12.0pt;color:black'> Engineering Bldg 1, Lab - N-284<o:p></o:p></span></p><p class=MsoNormal align=center style='margin-bottom:0in;margin-bottom:.0001pt;text-align:center;line-height:normal'><b><span style='font-size:12.0pt;color:black'>Time:</span></b><span style='font-size:12.0pt;color:black'> 2:00 PM<o:p></o:p></span></p><p class=MsoNormal align=center style='margin-bottom:0in;margin-bottom:.0001pt;text-align:center;line-height:normal'><span style='font-size:12.0pt;color:black'><o:p> </o:p></span></p><p class=MsoNormal align=center style='margin-bottom:0in;margin-bottom:.0001pt;text-align:center;line-height:normal'><b><span style='font-size:12.0pt;color:black'>Committee Chair: </span></b><span style='font-size:12.0pt;color:black'>Dr. Stanley J. Kleis<o:p></o:p></span></p><p class=MsoNormal align=center style='margin-bottom:0in;margin-bottom:.0001pt;text-align:center;line-height:normal'><b><span style='font-size:12.0pt;color:black'>Committee Members:</span></b><b><span style='font-size:12.0pt;color:#1F497D'> </span></b><span style='font-size:12.0pt;color:black'>Dr. Larry C. Witte</span><b><span style='font-size:12.0pt;color:#1F497D'><o:p></o:p></span></b></p><p class=MsoNormal align=center style='margin-bottom:0in;margin-bottom:.0001pt;text-align:center;line-height:normal'><span style='font-size:12.0pt;color:black'>Dr. D. Keith Hollingsworth</span><span style='font-size:12.0pt;color:black'><o:p></o:p></span></p><p class=MsoNormal style='margin-bottom:0in;margin-bottom:.0001pt;line-height:normal'><span style='font-size:12.0pt;color:black'><o:p> </o:p></span></p><p class=MsoNormal align=center style='margin-bottom:0in;margin-bottom:.0001pt;text-align:center;line-height:normal'><span style='font-size:12.0pt;color:black'><o:p> </o:p></span></p><p class=MsoNormal style='text-align:justify;text-indent:.5in;line-height:200%'><span style='font-size:12.0pt;line-height:200%;color:black'>A direct numerical simulation is performed of a cylindrical bubble moving in a pressure-driven flow of Novec<sup>TM</sup> 649 in a heated channel. The upper wall is an electrically heated metal foil, and the bubble diameter is on the order of the channel spacing. Phase change is not included to isolate the contribution of the liquid motion to the heat transfer. The simulation is performed with Fluent<sup>TM</sup>, the volume-of-fluid method tracks the interface, and the reference frame translates with the bubble. <o:p></o:p></span></p><p class=MsoNormal style='text-align:justify;text-indent:.5in;line-height:200%'><span style='font-size:12.0pt;line-height:200%;color:black'>The heat transfer coefficient increases tenfold due to the bubble passage. A lobed structure immediately behind the bubble forms in the surface heat flux, and the surface temperature is depressed over several bubble diameters. A complex horseshoe-like vortex system wraps the bubble and drives the heat flux lobes. The evolution of the heat flux at a point on the surface compares well to predictions of an existing quenching/diffusion model.<o:p></o:p></span></p><p class=MsoNormal style='text-align:justify;line-height:200%'><span style='font-size:12.0pt;line-height:200%'><o:p> </o:p></span></p><p class=MsoNormal style='text-align:justify;line-height:200%'><o:p> </o:p></p></div></body></html>