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 <title>iMechanica - Effect of Surface Morphology on the Stability of Thin Nanostructures - Comments</title>
 <link>http://imechanica.org/node/3245</link>
 <description>Comments for &quot;Effect of Surface Morphology on the Stability of Thin Nanostructures&quot;</description>
 <language>en</language>
<item>
 <title>Ashfaq Adnan


Phd Student,</title>
 <link>http://imechanica.org/node/3245#comment-7594</link>
 <description>&lt;p&gt;
Ashfaq Adnan
&lt;/p&gt;
&lt;p&gt;
Phd Student, Schoold of Aeronautics and Astronautics
&lt;/p&gt;
&lt;p&gt;
Purdue University, West Lafayette, Indiana 47907
&lt;/p&gt;
&lt;br class=&quot;clear&quot; /&gt;</description>
 <pubDate>Wed, 28 May 2008 17:31:58 -0400</pubDate>
 <dc:creator>Ashfaq Adnan</dc:creator>
 <guid isPermaLink="false">comment 7594 at http://imechanica.org</guid>
</item>
<item>
 <title>Effect of Surface Morphology on the Stability of Thin Nanostructures</title>
 <link>http://imechanica.org/node/3245</link>
 <description>&lt;p&gt;
&lt;span&gt;We have recently studied the atomic scale structural stability of&lt;br /&gt;
freestanding wavy gold (Au) nanofilms using molecular dynamics&lt;br /&gt;
simulations. In recent years, wavy or patterned structurs have shown great promise for applications in &lt;/span&gt;&lt;span&gt;various emerging technologies including fuel cells&lt;br /&gt;
engineering, tissue engineering, biomedical engineering, creation&lt;br /&gt;
of counterfeit-resistant documents , nanolithography in microelectronics, optoelectronics, nanomachinesand many others. It is out of question that the &lt;/span&gt;&lt;font face=&quot;times new roman,times&quot; size=&quot;3&quot;&gt;success of these novel applications lies on one crucial factor &amp;ndash; the&lt;br /&gt;
integrity and stability of the patterned structures during their manufacturing&lt;br /&gt;
process as well as during their service life.&lt;/font&gt;&lt;br /&gt;
&lt;span&gt;However, predicting material stability from the macroscopic physical&lt;br /&gt;
laws often becomes challenging due to the size dependent behavior of&lt;br /&gt;
nanostructured materials. The size dependency in nanostructures are primarily arises from &amp;quot;surface effects&amp;quot; and &amp;quot;quantum effects&amp;quot; where surface effects include activities at the free surface due to surface energy and surface stress, and quantum effects include quantum confinement effect or quantum hall effect. Between these two effects, &amp;quot;surface effects&amp;quot; play the primary role in determining the structural stability of materials. &lt;/span&gt;
&lt;/p&gt;
&lt;p&gt;
&amp;nbsp;
&lt;/p&gt;
&lt;p&gt;
&amp;nbsp;
&lt;/p&gt;
&lt;p&gt;
&lt;font face=&quot;times new roman,times&quot; size=&quot;3&quot;&gt;In&lt;br /&gt;
this study, we have obtained equilibrium configurations of various wavy gold films at different temperatures &lt;/font&gt;&lt;font face=&quot;times new roman,times&quot; size=&quot;3&quot;&gt;using molecular dynamics simulations.&lt;/font&gt;&lt;font face=&quot;times new roman,times&quot; size=&quot;3&quot;&gt; The degree of waviness was&lt;br /&gt;
controlled by varying the wavelength of a sinusoidal surface. Four different&lt;br /&gt;
films were thus constructed. The&lt;br /&gt;
stability of these thin films was studied at five different temperatures which&lt;br /&gt;
were below the melting point of bulk gold.&lt;span&gt;&amp;nbsp;&lt;br /&gt;
&lt;/span&gt;Some critical observations are:&lt;/font&gt;
&lt;/p&gt;
&lt;p&gt;
&lt;font face=&quot;times new roman,times&quot; size=&quot;3&quot;&gt;(a) It was observed from the equilibrated shapes of these structures that&lt;br /&gt;
the stability of wavy surfaces significantly depends on temperature and degree&lt;br /&gt;
of waviness. &lt;/font&gt;
&lt;/p&gt;
&lt;p&gt;
&lt;font face=&quot;times new roman,times&quot; size=&quot;3&quot;&gt;(b) It was also found that the size dependent melting of Au films occurred&lt;br /&gt;
in a progressive manner over a range of temperature rather than occurring at&lt;br /&gt;
some fixed temperature - as expected from fundamental thermodynamics of bulk crystal. &lt;/font&gt;
&lt;/p&gt;
&lt;p&gt;
&lt;font face=&quot;times new roman,times&quot; size=&quot;3&quot;&gt;We have proposed a new method to identify the progressive melting temperature of crystal structures and using this method we have demonsrtated that the progressive melting is caused by the non-uniform&lt;br /&gt;
melting of film along the thickness direction. The melting in the film starts when&lt;br /&gt;
only the atomic layers at the two free surfaces melt at temperatures lower than&lt;br /&gt;
the so-called bulk melting temperature. As heating continues, the entire film&lt;br /&gt;
then gradually melts.&lt;/font&gt;
&lt;/p&gt;
&lt;p&gt;
&lt;font face=&quot;times new roman,times&quot; size=&quot;3&quot;&gt;We have discussed that the low temperature pre-melting of the surface boundary&lt;br /&gt;
layers plays the foremost role in the instability of wavy films. It is shown&lt;br /&gt;
than for a particular temperature, e.g. at 810 K, there exist a critical film thickness&lt;br /&gt;
below which melting occurs in the entire structures; otherwise it is confined&lt;br /&gt;
at the boundary layers only. &lt;span&gt;&amp;nbsp;&lt;/span&gt;It is&lt;br /&gt;
recognized that the film thickness of the wavy films were five times thicker&lt;br /&gt;
than the critical thickness at 810 K. However, it was demonstrated that the surface&lt;br /&gt;
waviness in the films behaved as secondary thin films, and for smaller&lt;br /&gt;
wavelengths, the major fractions of the sub-film thickness fell below the&lt;br /&gt;
critical thickness at 810K. As a result, some wavy films became unstable. At&lt;br /&gt;
elevated temperatures, e.g. 1080 K or higher, films are unable to maintain&lt;br /&gt;
their structure due to melting point depression of Au films. &lt;span&gt;&amp;nbsp;&lt;/span&gt;&lt;/font&gt;
&lt;/p&gt;
&lt;p&gt;
&lt;font size=&quot;3&quot;&gt;&lt;font face=&quot;times new roman,times&quot;&gt;In short, the current work demonstrates that stability of wavy surface are critically dependent on temperature and degree of surface roughness.&lt;/font&gt;&lt;/font&gt;
&lt;/p&gt;
&lt;p&gt;
&lt;em&gt;This work has been accepted for publication in Nanotechnology and will appear online on June 2008.&lt;/em&gt;
&lt;/p&gt;
&lt;br class=&quot;clear&quot; /&gt;</description>
 <comments>http://imechanica.org/node/3245#comments</comments>
 <category domain="http://imechanica.org/taxonomy/term/76">research</category>
 <category domain="http://imechanica.org/taxonomy/term/2359">Melting Point Depression</category>
 <category domain="http://imechanica.org/taxonomy/term/93">molecular dynamics</category>
 <category domain="http://imechanica.org/taxonomy/term/963">stability</category>
 <category domain="http://imechanica.org/taxonomy/term/17">thin film</category>
 <enclosure url="http://imechanica.org/files/Adnan_Stability_Nanotech_2008.pdf" length="2013889" type="application/pdf" />
 <pubDate>Wed, 28 May 2008 17:31:18 -0400</pubDate>
 <dc:creator>Ashfaq Adnan</dc:creator>
 <guid isPermaLink="false">3245 at http://imechanica.org</guid>
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