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Photonic crystals in biology

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Poster Session, Tuesday, June 15<br />

Theme A1 - B702<br />

The Effect of Vacancies on the Mechanical Properties of (10,10) S<strong>in</strong>gle Walled Carbon Nanotubes<br />

Gülay Dereli*, Banu Süngü* and Önder Eyeciolu<br />

Department of Physics, Yildiz Technical University, stanbul 34210, Turkey<br />

Abstract— In this work, we aimed to show the effect of vacancies on the structural stability, tensile strength and Young modulus of (10,10)<br />

S<strong>in</strong>gle Walled Carbon Nanotubes (SWCNTs). We used O(N) tight-b<strong>in</strong>d<strong>in</strong>g molecular dynamics (TBMD) simulation method. We studied at 300K<br />

to except the effect of temperature and to study with the brittle SWCNTs. We have concluded the results with respect to the defect free and s<strong>in</strong>gle<br />

vacancy defect results of (10,10) SWCNTs.<br />

Soon after their discovery, carbon nanotubes become<br />

most promis<strong>in</strong>g materials due to their extremely small<br />

dimensions, mechanical strength, as well as, elasticity and<br />

adjustible electronic properties. These remarkable<br />

characteristics lead to many important applications <strong>in</strong><br />

nanotechnology. In our previous works, we have shown that<br />

temperature has significant effects on the thermal stability and<br />

mechanical properties of nanotubes [1-3]. On the other hand,<br />

the recent high-resolution transmission electron microscopy<br />

(HR-TEM) studies and computational simulation results po<strong>in</strong>t<br />

out that the structural defects play a crucial role on the<br />

electronic, optical and mechanical properties of carbon<br />

nanotubes [4-13]. These studies show variety of results<br />

accord<strong>in</strong>g to the methods and the defects. Several k<strong>in</strong>ds of<br />

defects may occur on carbon nanotubes. Here we exam<strong>in</strong>ed<br />

the vacancy defects on the atomic structure. We used a parallel<br />

O(N) TBMD code designed by Dereli et al [14-16]. We<br />

studied at 300K to except the effect of temperature and to<br />

study with the brittle SWCNTs.<br />

Dur<strong>in</strong>g our simulations, we first optimized a prist<strong>in</strong>e<br />

(10,10) SWCNT us<strong>in</strong>g the “thermal equilibrium” method as<br />

described <strong>in</strong> [1]. Then multiple amount of vacancies are<br />

generated on the tube structure and the tensile load<strong>in</strong>g is<br />

applied to the defected tube. Us<strong>in</strong>g this procedure, we<br />

<strong>in</strong>vestigated the structural stability and the bond break<strong>in</strong>g<br />

stra<strong>in</strong> values of the (10,10) SWCNT. The stress-stra<strong>in</strong> curve of<br />

the nanotube is obta<strong>in</strong>ed and the mechanical parameters such<br />

as the tensile strength, elastic limit, Young modulus are<br />

calculated. In our work of [17], we <strong>in</strong>vestigated the effect of<br />

s<strong>in</strong>gle vacancy defect on the tensile properties of (10,10)<br />

SWCNTs and we compared the results with the prist<strong>in</strong>e tube<br />

[2]. In the study, we have shown that a s<strong>in</strong>gle vacancy defect<br />

decreased the bond break<strong>in</strong>g stra<strong>in</strong> from 23% to 16%. The<br />

elastic limit ma<strong>in</strong>ta<strong>in</strong>ed its value as 10%. A s<strong>in</strong>gle vacancy<br />

defect did not represent a significant effect on the Young’s<br />

modulus of SWCNTs, which is calculated as a decrease of<br />

1.5%. However it is shown that a s<strong>in</strong>gle vacancy defect is<br />

observed to reduce the tensile strength from 83.23 GPa to<br />

64.14 GPa which corresponds to 23% decrease.<br />

Here we reach one step ahead from these studies to<br />

clarify the decreas<strong>in</strong>g ratios of tensile strength and mechanical<br />

parameters with respect to the certa<strong>in</strong> amount of vacancies.<br />

Figure 1(a), shows the difference between the total energy<br />

values of prist<strong>in</strong>e (10,10) tube and the (10,10) tube with 4 -<br />

vacancies. Last 2000MD Step <strong>in</strong> Figure 1(b), (c) and (d) show<br />

the total energy results of (10,10) tube under 5%, 10% and<br />

15% stra<strong>in</strong>, respectively. Figure 1 and the correspond<strong>in</strong>g<br />

simulation pictures of Figure 2, show that the simulated<br />

carbon nanotube with 4 - vacancies can not carry the stra<strong>in</strong><br />

when it is stretched to 10 -15% of its orig<strong>in</strong>al length. This<br />

work will set lights to the applications of carbon nanotubes<br />

with vacancy defects which is very common dur<strong>in</strong>g their<br />

formation. Careful study on the bond break<strong>in</strong>g values of these<br />

SWCNTs dur<strong>in</strong>g stretch<strong>in</strong>g will be done. Effect of 4-vacancies<br />

on the structural stability, tensile strength and Young modulus<br />

will be reported.<br />

Total energy (eV/atom)<br />

Total energy (eV/atom)<br />

-7,8<br />

-8,0<br />

-8,2<br />

-8,20<br />

-8,24<br />

-8,28<br />

-8,32<br />

(a)<br />

0 2000 4000 6000<br />

MD Step<br />

10%<br />

-8,15<br />

-8,20<br />

-8,25<br />

-8,30<br />

(b)<br />

-8,35<br />

0 2000 4000 6000 8000<br />

MD Step<br />

-7,6<br />

15%<br />

-7,8<br />

(c)<br />

(d)<br />

-8,4<br />

-8,4<br />

0 2000 4000 6000 8000 0 2000 4000 6000 8000<br />

MD Step<br />

MD Step<br />

Figure:1 Total energy per atom results of (10,10) SWCNT (a) with 4 –vacancies;<br />

(b) under 5% stra<strong>in</strong>; (c) under 10% stra<strong>in</strong>; (d) under 15% stra<strong>in</strong>.<br />

-8,0<br />

-8,2<br />

Figure:2 Simulation pictures of (10,10) tube (a) with 4 –vacancies;<br />

(b) under 5% stra<strong>in</strong>; (c) under 10% stra<strong>in</strong>; (d) under 15% stra<strong>in</strong>.<br />

The research reported here is supported through the Yildiz<br />

Technical University Research Fund Project No: 24-01-01-04.<br />

The simulations are performed at the Carbon Nanotubes<br />

Simulation Laboratory at the Department of Physics, Yildiz<br />

Technical University, Istanbul, Turkey.<br />

(http://www.yildiz/edu/tr/~gdereli/lab_homepage/<strong>in</strong>dex.html)<br />

*Correspond<strong>in</strong>g author: gdereli@yildiz.edu.tr<br />

5%<br />

6th Nanoscience and Nanotechnology Conference, zmir, 2010 399

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