<node id="66345">
  <nid>66345</nid>
  <type>event</type>
  <uid>
    <user id="27388"><![CDATA[27388]]></user>
  </uid>
  <created>1306926380</created>
  <changed>1475891703</changed>
  <title><![CDATA[MSE Ph.D. Defense - Seung Geol Lee]]></title>
  <body><![CDATA[<p><strong>Title: </strong>STRUCTURE-PROPERTY RELATIONSHIP OF HYDROGEL: MOLECULAR
DYNAMICS SIMULATION APPROACH

</p>

<p><strong>Summary: </strong>We have used a molecular modeling of both random and
blocky sequence hydrogel networks of poly(N-vinyl-2-pyrrolidone-co-2-hydroxyethyl

</p><p>methacrylate) (P(VP-co-HEMA)) with a composition of
VP:HEMA = 37:13 to investigate the effect of the monomeric sequence and the
water content on the equilibrium structures and the mechanical and transport
properties by full-atomistic molecular dynamics (MD) simulations.&nbsp; The degree of randomness of the monomer
sequence for the random and the blocky copolymers, were 1.170 and 0.104,
respectively, and the degree of polymerization was fixed at 50.&nbsp; The equilibrated density of the hydrogel was
found to be larger for the random sequence than for the blocky sequence at low
water contents (&lt; 40 wt %), but this density difference decreased with
increasing water content.&nbsp; The pair
correlation function analysis shows that VP is more hydrophilic than HEMA and
that the random sequence hydrogel is solvated more than the blocky sequence
hydrogel at low water content, which disappears with increasing water content.</p>

<p>Correspondingly, the water structure is more disrupted by
the random sequence hydrogel at low water content but eventually develops the
expected bulk-water-like structure with increasing water content.&nbsp; From mechanical deformation simulations, the
stress-strain analysis showed that the VP is found to relax more efficiently,
especially in the blocky sequence, so that the blocky sequence hydrogel shows
less stress levels compared to the random sequence hydrogel.&nbsp; As the water content increases, the stress
level becomes identical for both sequences.&nbsp;
The elastic moduli of the hydrogels calculated from the constant strain
energy minimization show the same trend with the stress-strain analysis.&nbsp; Ascorbic acid and D-glucose were used to
study the effect of the monomeric sequence on the diffusion of small guest
molecules within the hydrogels.&nbsp; By
analyzing the pair correlation functions, it was found that the guest molecule
has greater accessibility to the VP units than to the HEMA units with both
monomeric sequences due to its higher hydrophilicity compared to the HEMA
units.&nbsp; The monomeric sequence effect on
the P(VP-co-HEMA) hydrogel is clearly observed with 20 wt % water content, but
the monomeric sequence effect is significantly reduced with 40 wt % water
content and disappears with 80 wt % water content.&nbsp; This is because the hydrophilic guest
molecules are more likely to be associated with water molecules than with the
polymer network at the high water content.&nbsp;
By analyzing the mean square displacement, the displacement of the guest
molecules and the inner surface area, it is also found that the guest molecule
is confined in the system at 20 wt % water content, resulting in highly
anomalous subdiffusion.&nbsp; Therefore, the
diffusion of the guest molecules is directly affected by their interaction with
the monomer units, the monomeric sequence and the geometrical confinement in
the hydrogel at a low water content, but the monomeric sequence effect and the
restriction on the diffusion of the guest molecule are significantly decreased
with increasing the water content.</p>

<p>&nbsp;</p>

<p>We also investigated the de-swelling mechanisms of the
surface-grafted</p>

<p>poly(N-isopropylacrylamide) (P(NIPAAm)) brushes
containing 1300 water molecules at 275 K, 290 K, 320 K, 345 K, and 370 K.&nbsp; We clearly observed the de-swelling of the
water molecules for P(NIPAAm) above the lower critical solution temperature
(LCST) (~305 K).&nbsp; Below the LCST, we did
not observe the de-swelling of water molecules.&nbsp;
Using the upper critical solution temperature (UCST) systems
(poly(acrylamide) brushes) for comparison purposes, we did not observe the
de-swelling of water molecules at a given range of temperatures.&nbsp; By analyzing the pair correlation functions
and the coordination numbers, the de-swelling of the water molecules occurred
distinctly around the isopropyl group of the P(NIPAAm) brush above the LCST
because C(NIPAAm) does not offer sufficient interaction with the water
molecules via the hydrogen bonding type of secondary interaction.&nbsp; We also found that the contribution of the</p>

<p>N(NIPAAm)-O(water) pair is quite small because of the
steric hindrance of the isopropyl group.&nbsp;
By analyzing the change in the hydrogen bonds, the hydrogen bonds
between polar groups and water molecules in the P(NIPAAm) brushes weaken with
increasing temperature, which leads to the de-swelling of the water molecules
out of the brushes above the LCST.&nbsp; Below
the LCST, the change in the hydrogen bonds is not significant.&nbsp; Again, the contribution of the
NH(NIPAAm)-water pairs is insignificant; the total number of hydrogen bonds is
~20, indicating that the interaction between the NH group and the water
molecules is not significant due to steric hindrances.&nbsp; Lastly, we observed that the total surface
area of the</p>

<p>P(NIPAAm) brushes that is accessible to water molecules
is decreased by collapsing the brushes followed by the de-swelling of water
molecules above the LCST.</p>]]></body>
  <field_summary_sentence>
    <item>
      <value><![CDATA[MSE Ph.D. Defense - Seung Geol Lee]]></value>
    </item>
  </field_summary_sentence>
  <field_summary>
    <item>
      <value><![CDATA[<p><strong>Title:</strong> STRUCTURE-PROPERTY RELATIONSHIP OF HYDROGEL:
MOLECULAR DYNAMICS SIMULATION APPROACH</p>]]></value>
    </item>
  </field_summary>
  <field_time>
    <item>
      <value><![CDATA[2011-06-06T11:00:00-04:00]]></value>
      <value2><![CDATA[2011-06-06T13:00:00-04:00]]></value2>
      <rrule><![CDATA[]]></rrule>
      <timezone><![CDATA[America/New_York]]></timezone>
    </item>
  </field_time>
  <field_fee>
    <item>
      <value><![CDATA[]]></value>
    </item>
  </field_fee>
  <field_extras>
      </field_extras>
  <field_audience>
      </field_audience>
  <field_media>
      </field_media>
  <field_contact>
    <item>
      <value><![CDATA[]]></value>
    </item>
  </field_contact>
  <field_location>
    <item>
      <value><![CDATA[]]></value>
    </item>
  </field_location>
  <field_sidebar>
    <item>
      <value><![CDATA[]]></value>
    </item>
  </field_sidebar>
  <field_phone>
    <item>
      <value><![CDATA[]]></value>
    </item>
  </field_phone>
  <field_url>
    <item>
      <url><![CDATA[]]></url>
      <title><![CDATA[]]></title>
            <attributes><![CDATA[]]></attributes>
    </item>
  </field_url>
  <field_email>
    <item>
      <email><![CDATA[]]></email>
    </item>
  </field_email>
  <field_boilerplate>
    <item>
      <nid><![CDATA[]]></nid>
    </item>
  </field_boilerplate>
  <links_related>
      </links_related>
  <files>
      </files>
  <og_groups>
          <item>1238</item>
      </og_groups>
  <og_groups_both>
          <item><![CDATA[School of Materials Science and Engineering]]></item>
      </og_groups_both>
  <field_categories>
          <item>
        <tid>1791</tid>
        <value><![CDATA[Student sponsored]]></value>
      </item>
      </field_categories>
  <field_keywords>
          <item>
        <tid>10802</tid>
        <value><![CDATA[MSE_Interal_Event]]></value>
      </item>
      </field_keywords>
  <field_userdata><![CDATA[]]></field_userdata>
</node>
