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From: "Stacey, Lisa A" <staceyl@purdue.edu>
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Please see attached Seminar Reminder for today

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Date: Thu, 19 Apr 2012 10:21:53 -0400
Subject: REMINDER:  4/19/12 3:30 PM SEMINAR Ph.D. Final Exam-K. Vishnu
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MATERIALS SCIENCE AND ENGINEERING
SEMINAR


Shape Memory in Nanostructured Metallic Alloys

by

Karthik Guda Vishnu
Purdue Ph.D. Final Exam

Advisor
Professor A. Strachan

ABSTRACT

Materials with nano-scale dimensions show mechanical and structural propert=
ies different to those at the macro scale and engineering their nano-struct=
ure opens up potential avenues for designing materials tailored for a speci=
fic application. This work is focused on shape memory materials, an importa=
nt class of active materials with wide variety of applications in medical i=
ndustry, aerospace and automobile industries, due to their two important pr=
operties of super-elasticity and shape memory. These unique properties orig=
inate from a solid-solid transformation called martensite transformation an=
d the main objectives of this research are to i) study the atomic mechanism=
s of the martensite transformation, ii) study the effect of nano-structure =
on shape memory behavior and iii) computationally explore avenues through w=
hich their performance is optimized. A combination of density functional th=
eory (DFT) and molecular dynamics (MD) simulations is used to achieve this.=
 This approach gives an atomic level description and the effects of size, s=
urfaces and interfaces are explicitly described. Detailed analysis of the a=
tomic mechanisms of the martensite transformation in NiTi using DFT reveale=
d a new phase transformation (B19=92=92) that sheds light on why the theore=
tically predicted ground state (BCO) is not observed experimentally and tha=
t the experimentally observed martensite phase (B19=92) can be stabilized b=
y internal stresses. This finding is very important as the theoretically pr=
edicted ground state does not allow for shape memory in nano-scale NiTi sam=
ples.
The size effects caused by the presence of free surfaces and the role of na=
no-structure in martensite transformation have been investigated in thin Ni=
Ti slabs. Surface energies of B2 phase (austenite), B19 (orthorhombic), B19=
=92 (martensite) and the body centered orthorhombic phase (BCO) are calcula=
ted using DFT. (110)B2 surfaces with in-plane atomic displacements stabiliz=
e the austenite phase with respect to B19=92 and BCO, thus slabs with such =
orientations are predicted to exhibit a decrease in martensite transition t=
emperature with decreasing thickness. It has been predicted that a thicknes=
s of 2 nm is critical for the transition to occur. The opposite trend is ob=
served in slabs with atomic displacements along the surface normal; the pha=
se transformation temperature increases with decreasing size.
Finally, it has also been demonstrated via large scale molecular dynamics s=
imulations that the austenite =96 martensite energy landscapes of NiAl base=
d thermo-elastic shape memory superlattice structures can be engineered via=
 epitaxial integration. This allows for tuning their thermal hysteresis and=
 transition temperatures. This resulted in materials with very low thermal =
hysteresis and with minimal degradation in phase transition strain thereby =
making them ideal for actuating applications.

Date:   Thursday, April 19, 2012
Time:   3:30 P.M.
Place:   ARMS Room 1028



Lisa Stacey
Secretary/Development Assistant
Purdue University
School of Materials Engineering
765/494-4100


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oNormal" align=3D"center" style=3D"text-align:center;line-height:150%"><b><=
span style=3D"font-size:14.0pt;line-height:150%">MATERIALS SCIENCE AND ENGI=
NEERING<o:p></o:p></span></b></p><h5 align=3D"center" style=3D"text-align:c=
enter"><span style=3D"font-size:14.0pt">SEMINAR<b><o:p></o:p></b></span></h=
5><p class=3D"MsoTitle"><span style=3D"font-size:14.0pt;font-weight:normal"=
><o:p>&nbsp;</o:p></span></p><p class=3D"MsoNormal" align=3D"center" style=
=3D"text-align:center"><b>Shape Memory in Nanostructured Metallic Alloys<o:=
p></o:p></b></p><p class=3D"MsoNormal" align=3D"center" style=3D"text-align=
:center"><b><o:p>&nbsp;</o:p></b></p><p class=3D"MsoNormal" align=3D"center=
" style=3D"text-align:center">by<o:p></o:p></p><p class=3D"MsoNormal" align=
=3D"center" style=3D"text-align:center"><o:p>&nbsp;</o:p></p><p class=3D"Ms=
oNormal" align=3D"center" style=3D"text-align:center">Karthik Guda Vishnu<o=
:p></o:p></p><p class=3D"MsoNormal" align=3D"center" style=3D"text-align:ce=
nter">Purdue Ph.D. Final Exam<o:p></o:p></p><p class=3D"MsoNormal" align=3D=
"center" style=3D"text-align:center"><o:p>&nbsp;</o:p></p><p class=3D"MsoNo=
rmal" align=3D"center" style=3D"text-align:center">Advisor<o:p></o:p></p><p=
 class=3D"MsoNormal" align=3D"center" style=3D"text-align:center">Professor=
 A. Strachan<o:p></o:p></p><p class=3D"MsoNormal" align=3D"center" style=3D=
"text-align:center"><o:p>&nbsp;</o:p></p><p class=3D"MsoNormal" align=3D"ce=
nter" style=3D"text-align:center"><b><span style=3D"font-size:11.0pt">ABSTR=
ACT<o:p></o:p></span></b></p><p class=3D"MsoNormal" style=3D"text-align:jus=
tify"><o:p>&nbsp;</o:p></p><p class=3D"MsoNormal" style=3D"text-align:justi=
fy">Materials with nano-scale dimensions show mechanical and structural pro=
perties different to those at the macro scale and engineering their nano-st=
ructure opens up potential avenues for designing materials tailored for a s=
pecific application. This work is focused on shape memory materials, an imp=
ortant class of active materials with wide variety of applications in medic=
al industry, aerospace and automobile industries, due to their two importan=
t properties of super-elasticity and shape memory. These unique properties =
originate from a solid-solid transformation called martensite transformatio=
n and the main objectives of this research are to i) study the atomic mecha=
nisms of the martensite transformation, ii) study the effect of nano-struct=
ure on shape memory behavior and iii) computationally explore avenues throu=
gh which their performance is optimized. A combination of density functiona=
l theory (DFT) and molecular dynamics (MD) simulations is used to achieve t=
his. This approach gives an atomic level description and the effects of siz=
e, surfaces and interfaces are explicitly described. Detailed analysis of t=
he atomic mechanisms of the martensite transformation in NiTi using DFT rev=
ealed a new phase transformation (B19=92=92) that sheds light on why the th=
eoretically predicted ground state (BCO) is not observed experimentally and=
 that the experimentally observed martensite phase (B19=92) can be stabiliz=
ed by internal stresses. This finding is very important as the theoreticall=
y predicted ground state does not allow for shape memory in nano-scale NiTi=
 samples.<o:p></o:p></p><p class=3D"MsoNormal" style=3D"text-align:justify"=
>The size effects caused by the presence of free surfaces and the role of n=
ano-structure in martensite transformation have been investigated in thin N=
iTi slabs. Surface energies of B2 phase (austenite), B19 (orthorhombic), B1=
9=92 (martensite) and the body centered orthorhombic phase (BCO) are calcul=
ated using DFT. (110)<sub>B2</sub> surfaces with in-plane atomic displaceme=
nts stabilize the austenite phase with respect to B19=92 and BCO, thus slab=
s with such orientations are predicted to exhibit a decrease in martensite =
transition temperature with decreasing thickness. It has been predicted tha=
t a thickness of 2 nm is critical for the transition to occur. The opposite=
 trend is observed in slabs with atomic displacements along the surface nor=
mal; the phase transformation temperature increases with decreasing size.<o=
:p></o:p></p><p class=3D"MsoNormal">Finally, it has also been demonstrated =
via large scale molecular dynamics simulations that the austenite =96 marte=
nsite energy landscapes of NiAl based thermo-elastic shape memory superlatt=
ice structures can be engineered via epitaxial integration. This allows for=
 tuning their thermal hysteresis and transition temperatures. This resulted=
 in materials with very low thermal hysteresis and with minimal degradation=
 in phase transition strain thereby making them ideal for actuating applica=
tions.<o:p></o:p></p><p class=3D"MsoNormal" style=3D"text-align:justify"><o=
:p>&nbsp;</o:p></p><p class=3D"MsoNormal"><span style=3D"font-size:11.0pt">=
Date:&nbsp;&nbsp; Thursday, April 19, 2012<o:p></o:p></span></p><p class=3D=
"MsoNormal"><span style=3D"font-size:11.0pt">Time:&nbsp;&nbsp; 3:30 P.M.<o:=
p></o:p></span></p><p class=3D"MsoNormal"><span style=3D"font-size:11.0pt">=
Place:&nbsp;&nbsp; ARMS Room 1028<o:p></o:p></span></p><p class=3D"MsoNorma=
l"><span style=3D"font-size:11.0pt;color:windowtext"><o:p>&nbsp;</o:p></spa=
n></p><p class=3D"MsoNormal"><span style=3D"font-size:11.0pt;color:windowte=
xt"><o:p>&nbsp;</o:p></span></p><p class=3D"MsoNormal"><span style=3D"font-=
size:11.0pt;color:windowtext"><o:p>&nbsp;</o:p></span></p><p class=3D"MsoNo=
rmal"><span style=3D"font-size:11.0pt;color:windowtext">Lisa Stacey<o:p></o=
:p></span></p><p class=3D"MsoNormal"><span style=3D"font-size:11.0pt;color:=
windowtext">Secretary/Development Assistant<o:p></o:p></span></p><p class=
=3D"MsoNormal"><span style=3D"font-size:11.0pt;color:windowtext">Purdue Uni=
versity<o:p></o:p></span></p><p class=3D"MsoNormal"><span style=3D"font-siz=
e:11.0pt;color:windowtext">School of Materials Engineering<o:p></o:p></span=
></p><p class=3D"MsoNormal"><span style=3D"font-size:11.0pt;color:windowtex=
t">765/494-4100<o:p></o:p></span></p><p class=3D"MsoNormal"><o:p>&nbsp;</o:=
p></p></div></body></html>=

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