<html xmlns:v="urn:schemas-microsoft-com:vml" xmlns:o="urn:schemas-microsoft-com:office:office" xmlns:w="urn:schemas-microsoft-com:office:word" xmlns:m="http://schemas.microsoft.com/office/2004/12/omml" xmlns="http://www.w3.org/TR/REC-html40">
<head>
<meta http-equiv="Content-Type" content="text/html; charset=us-ascii">
<meta name="Generator" content="Microsoft Word 15 (filtered medium)">
<!--[if !mso]><style>v\:* {behavior:url(#default#VML);}
o\:* {behavior:url(#default#VML);}
w\:* {behavior:url(#default#VML);}
.shape {behavior:url(#default#VML);}
</style><![endif]--><style><!--
/* Font Definitions */
@font-face
{font-family:"Cambria Math";
panose-1:2 4 5 3 5 4 6 3 2 4;}
@font-face
{font-family:Calibri;
panose-1:2 15 5 2 2 2 4 3 2 4;}
@font-face
{font-family:"Trebuchet MS";
panose-1:2 11 6 3 2 2 2 2 2 4;}
/* Style Definitions */
p.MsoNormal, li.MsoNormal, div.MsoNormal
{margin:0in;
margin-bottom:.0001pt;
font-size:11.0pt;
font-family:"Calibri",sans-serif;}
a:link, span.MsoHyperlink
{mso-style-priority:99;
color:blue;
text-decoration:underline;}
a:visited, span.MsoHyperlinkFollowed
{mso-style-priority:99;
color:purple;
text-decoration:underline;}
p.msonormal0, li.msonormal0, div.msonormal0
{mso-style-name:msonormal;
margin:0in;
margin-bottom:.0001pt;
font-size:11.0pt;
font-family:"Calibri",sans-serif;}
span.EmailStyle21
{mso-style-type:personal-reply;
font-family:"Calibri",sans-serif;
color:windowtext;}
.MsoChpDefault
{mso-style-type:export-only;
font-size:10.0pt;}
@page WordSection1
{size:8.5in 11.0in;
margin:1.0in 1.0in 1.0in 1.0in;}
div.WordSection1
{page:WordSection1;}
--></style><!--[if gte mso 9]><xml>
<o:shapedefaults v:ext="edit" spidmax="1026" />
</xml><![endif]--><!--[if gte mso 9]><xml>
<o:shapelayout v:ext="edit">
<o:idmap v:ext="edit" data="1" />
</o:shapelayout></xml><![endif]-->
</head>
<body lang="EN-US" link="blue" vlink="purple">
<div class="WordSection1">
<p class="MsoNormal"><o:p> </o:p></p>
<div>
<div align="center">
<table class="MsoNormalTable" border="0" cellpadding="0" width="600" style="width:6.25in">
<tbody>
<tr>
<td style="padding:.75pt .75pt .75pt .75pt">
<div>
<p class="MsoNormal"><span style="font-size:13.5pt;font-family:"Arial",sans-serif"><a href="https://www.chee.uh.edu" target="_blank"><span style="color:#C8102E;text-decoration:none"><img border="0" width="600" height="165" style="width:6.25in;height:1.7187in" id="_x0000_i1025" src="https://www.egr.uh.edu/sites/www.egr.uh.edu/files/enews/2022/images/sa_header.png" alt="William A. Brookshire Department of Chemical and Biomolecular Engineering Seminar Series"></span></a><o:p></o:p></span></p>
</div>
<div align="center">
<table class="MsoNormalTable" border="0" cellpadding="0">
<tbody>
<tr>
<td style="padding:.75pt .75pt .75pt .75pt">
<p align="center" style="mso-margin-top-alt:11.25pt;margin-right:0in;margin-bottom:11.25pt;margin-left:0in;text-align:center;mso-line-height-alt:16.5pt">
<strong><span style="font-size:18.0pt;font-family:"Arial",sans-serif">Glass Transition and Dynamics of
<o:p></o:p></span></strong></p>
<p align="center" style="mso-margin-top-alt:11.25pt;margin-right:0in;margin-bottom:11.25pt;margin-left:0in;text-align:center;mso-line-height-alt:16.5pt">
<strong><span style="font-size:18.0pt;font-family:"Arial",sans-serif">Nanoscopically Confined Polymer</span></strong><span style="font-size:18.0pt;font-family:"Arial",sans-serif"><o:p></o:p></span></p>
<p class="MsoNormal" align="center" style="text-align:center"><span style="font-size:14.0pt;font-family:"Arial",sans-serif"><o:p> </o:p></span></p>
<p align="center" style="mso-margin-top-alt:11.25pt;margin-right:0in;margin-bottom:11.25pt;margin-left:0in;text-align:center;mso-line-height-alt:16.5pt">
<span style="font-size:18.0pt;font-family:"Arial",sans-serif">Rodney Priestley<br>
</span><span style="font-size:14.0pt;font-family:"Arial",sans-serif">Professor<br>
Princeton University<o:p></o:p></span></p>
<p align="center" style="mso-margin-top-alt:11.25pt;margin-right:0in;margin-bottom:11.25pt;margin-left:0in;text-align:center;line-height:16.5pt">
<strong><span style="font-size:14.0pt;font-family:"Arial",sans-serif">April 15 2022 | 10:30am Central</span></strong><b><span style="font-size:14.0pt;font-family:"Arial",sans-serif"><br>
</span></b><span style="font-size:14.0pt;font-family:"Arial",sans-serif">Room L2D2<o:p></o:p></span></p>
<p align="center" style="mso-margin-top-alt:11.25pt;margin-right:0in;margin-bottom:11.25pt;margin-left:0in;text-align:center;line-height:16.5pt">
Or virtually at <a href="https://urldefense.com/v3/__https://uh-edu-cougarnet.zoom.us/j/93450248978__;!!LkSTlj0I!EgLbjLNRSgV3FDAa5I2isdC0m08RDPLKGkc-Tni6ZP3s623ifndMA_IMg6JK_-FCpgZx0YbE7HexwNkXrKkwfHMRh-g$">https://uh-edu-cougarnet.zoom.us/j/93450248978</a><o:p></o:p></p>
<p align="center" style="mso-margin-top-alt:11.25pt;margin-right:0in;margin-bottom:11.25pt;margin-left:0in;text-align:center;line-height:16.5pt">
<strong><span style="font-size:12.0pt;font-family:"Arial",sans-serif;color:#C8102E">LECTURE ABSTRACT</span></strong><span style="font-size:12.0pt;font-family:"Arial",sans-serif;color:#C8102E"><o:p></o:p></span></p>
<p class="MsoNormal" style="text-align:justify"><span style="font-family:"Arial",sans-serif">Many technological advances are driven by the ongoing emergence of nanostructured polymers as the critical component to enable innovation. Yet, from a materials design
perspective, we cannot presume that the bulk properties of polymers define their behavior when physically confined to nanoscale dimensions. This is, in fact, not true, as there is now convincing evidence that the nanoscale properties of polymers, including
the glass transition temperature, can be profoundly different from the bulk. In this presentation, I want to highlight two recent examples from my group that aimed to advance the field of understanding polymers in confinement and at interfaces. In the first
part of the talk, we introduce a time-resolved nano-creep experiment to probe the dynamics at the surface of polymer glasses. We reveal a new mode of molecular dynamic at the surface: pseudoentanglements. This phenomenon causes unentangled chains to exhibit
surface mechanical response and dynamics that are characteristic of entangled polymers. For entangled chains, the phenomenon prolongs and stiffens the entangled response. In both cases, the breadth of the entangled response grows on cooling, leading to a breakdown
of time-temperature-superposition at the surface. Counterintuitively, this new mode of slow surface dynamics emerges precisely because surface dynamics are accelerated relative to the bulk. In the second part of the talk, we present an experimental methodology
to allow for the first direct measurement of the local glass transition temperature (T<sub>g</sub>) in block copolymers. This is achieved by incorporating fluorescence-bearing monomers at specific locations along the polymer chain, allowing the labeled monomers
local environment to be interrogated via fluorescence. As an example, in lamellar forming poly(butyl methacrylate-b -methyl methacrylate) diblock copolymers, a strong gradient in glass transition temperature, T<sub>g</sub> , of the higher-T<sub>g</sub> block,
42 K over 4 nm, was mapped with nanometer resolution. These measurements also revealed a strongly asymmetric influence of the domain interface on T<sub>g</sub> , with a much smaller dynamic gradient being observed for the lower-T<sub>g</sub> block. We also
find that chain connectivity plays an important role in setting the glassy dynamics in diblock copolymers.<o:p></o:p></span></p>
<p align="center" style="mso-margin-top-alt:11.25pt;margin-right:0in;margin-bottom:11.25pt;margin-left:0in;text-align:center;line-height:16.5pt">
<span style="font-size:10.5pt;font-family:"Arial",sans-serif"><o:p> </o:p></span></p>
<p align="center" style="mso-margin-top-alt:11.25pt;margin-right:0in;margin-bottom:11.25pt;margin-left:0in;text-align:center;line-height:16.5pt">
<strong><span style="font-size:12.0pt;font-family:"Arial",sans-serif;color:#C8102E">SPEAKER BIOSKETCH</span></strong><span style="font-size:12.0pt;font-family:"Arial",sans-serif;color:#C8102E"><o:p></o:p></span></p>
<p align="center" style="mso-margin-top-alt:11.25pt;margin-right:0in;margin-bottom:11.25pt;margin-left:0in;text-align:center;line-height:16.5pt">
<span style="font-family:"Arial",sans-serif;color:black">Rodney D Priestley is the Vice Dean for Innovation and the incoming Dean of the Graduate School at Princeton University. He is the Pomeroy Betty Perry Smith Professor in the Department of Chemical and Biological
Engineering and the Associate Director of the Princeton Center for Complex Materials. He obtained his Ph.D. in Chemical Engineering from Northwestern University in 2008. His research involves describing and developing complex materials, especially nanoparticles,
thin polymer films, and nanocomposites, focusing on material properties at small length scales. From designing next-generation biocompatible surfactants to creating ultra-stable polymer films resistant to properties changes upon heating, his work impacts industries
ranging from personal care to aerospace. His recent interests include the use of polymers in sustainability and their implications on the environment. Recent recognitions include the 2020 American Physical Society Dillon Medal and 2020 American Chemical Society
Macro Letters-Biomacromolecules-Macromolecules Young Investigator Award. </span><span style="font-size:10.5pt;font-family:"Arial",sans-serif"><o:p></o:p></span></p>
<p align="center" style="mso-margin-top-alt:11.25pt;margin-right:0in;margin-bottom:11.25pt;margin-left:0in;text-align:center;line-height:16.5pt">
<span style="font-size:10.5pt;font-family:"Arial",sans-serif"> <o:p></o:p></span></p>
<p align="center" style="mso-margin-top-alt:11.25pt;margin-right:0in;margin-bottom:11.25pt;margin-left:0in;text-align:center;line-height:16.5pt">
<em><span style="font-size:8.5pt;font-family:"Arial",sans-serif">This is an official message sent by the William A. Brookshire Department of Chemical & Biomolecular Engineering.</span></em><span style="font-size:8.5pt;font-family:"Arial",sans-serif"><o:p></o:p></span></p>
</td>
</tr>
</tbody>
</table>
</div>
</td>
</tr>
<tr>
<td style="padding:.75pt .75pt .75pt .75pt">
<p class="MsoNormal"><span style="font-size:13.5pt;font-family:"Arial",sans-serif"><a href="https://www.chee.uh.edu" target="_blank"><span style="color:#C8102E;text-decoration:none"><img border="0" width="600" height="165" style="width:6.25in;height:1.7187in" id="_x0000_i1027" src="https://www.egr.uh.edu/sites/www.egr.uh.edu/files/enews/2022/images/sa_footer.png" alt="William A. Brookshire Department of Chemical and Biomolecular Engineering"></span></a><o:p></o:p></span></p>
</td>
</tr>
</tbody>
</table>
</div>
<p class="MsoNormal"><span style="font-size:10.0pt;font-family:"Trebuchet MS",sans-serif;color:black"><o:p> </o:p></span></p>
</div>
</div>
</body>
</html>