Third Day Poster Session, 17 June 2010 - NanoTR-VI
Third Day Poster Session, 17 June 2010 - NanoTR-VI
Third Day Poster Session, 17 June 2010 - NanoTR-VI
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<strong>Poster</strong> <strong>Session</strong>, Thursday, <strong>June</strong> <strong>17</strong><br />
Theme F686 - N1123<br />
Free vibration analysis of carbon nanotubes based on nonlocal continuum and gradient<br />
elasticity theories<br />
Ömer Civalek 1 , Bekir Akgöz, Hakan Ersoy<br />
1 Akdeniz University, Civil Engineering Department, Division of Mechanics<br />
Antalya-TURKIYE, Tel: + 90- 242-310 6319, Fax: + 90-242-310 6306<br />
Abstract- Free vibration analysis of single walled carbon nanotubes (CNT) is presented based on the Euler-Bernoulli beam<br />
theory. The size effect is taken into consideration using the Eringen’s non-local elasticity theory. Gradient elasticity theory is<br />
also adopted for modeling. The governing differential equations for CNT vibration is being solved using the differential<br />
quadrature (DQ) method. Numerical results are presented to show the effect of nonlocal behavior on frequencies of CNT.<br />
The concept of carbon nanotubes (CNTs) was first<br />
introduced in 1991 by Iijima [1] in Japan. Reviews on the<br />
development and application of such nano structures have<br />
been presented [2]. So, the studies of mechanical behaviors<br />
of carbon nanotubes have being attracted more and more<br />
attentions of scientists in the world and also have become a<br />
new research area of applied mechanics [3,4]. In the<br />
present work, the consistent governing equations for the<br />
beam model for CNTs are derived for free vibration<br />
analysis. Nonlocal beam and couple stress beam theories<br />
are adopted for modeling. It is known that, the stress state<br />
of any body at a point x is related to strain state at the same<br />
point x in the classical elasticity. But this theory is not<br />
conflict the atomic theory of lattice dynamics and<br />
experimental observation of phonon dispersion. As stated<br />
by Eringen [5] the linear theory of nonlocal elasticity leads<br />
to a set of integropartial differential equations for the<br />
displacements field for homogeneous, isotropic bodies.<br />
According to the nonlocal elasticity theory of Eringen’s,<br />
the stress at any reference point in the body depends not<br />
only on the strains at this point but also on strains at all<br />
points of the body. This definition of the Eringen’s<br />
nonlocal elasticity is based on the atomic theory of lattice<br />
dynamics and some experimental observations on phonon<br />
dispersion. In the present manuscript two different<br />
approaches are used for modeling of carbon nanotubes.<br />
Euler-Bernoulli beam-nonlocal model [5]<br />
4<br />
2<br />
W<br />
2<br />
2 W<br />
EI A W ( e0a)<br />
A 0 (1)<br />
4<br />
2<br />
x<br />
x<br />
Euler-Bernoulli beam-gradient elasticity theory [6]<br />
W<br />
x<br />
W<br />
x<br />
4<br />
4<br />
2<br />
2<br />
EI g EI A 0 (2)<br />
4<br />
4<br />
7<br />
Table 1. First three frequencies (10<br />
) of S-S carbon<br />
8<br />
nanotubes via gradient theory ( L 510<br />
m ,<br />
3<br />
12 2<br />
2300kg<br />
/ m , m , t 510 10<br />
E 10 N /<br />
m )<br />
Mode<br />
g/L (DQ results)<br />
0.005 0.015 0.125<br />
1 0.10388 0.10669 0.11374<br />
2 0.41065 0.41103 0.42301<br />
3 0.91863 0.92007 0.93485<br />
7<br />
Table 2. First three frequencies (10<br />
) of S-S carbon<br />
8<br />
nanotubes via nonlocal theory( L 510<br />
m ,<br />
3<br />
12 2<br />
2300kg<br />
/ m , m , t 510 10<br />
E 10 N /<br />
m )<br />
Mode (e 0 a) 2 (DQ results)<br />
0 2 4<br />
1 0.10273 0.10158 0.09962<br />
2 0.40967 0.40863 0.40553<br />
3 0.9<strong>17</strong>2 0.90864 0.90637<br />
[1] S. Iijima, Nature, 354, 56 (2001).<br />
[2] D. Qian, G.J. Wagner, W.K. Liu, Appl. Mech. Rev.,<br />
55, 495(2002).<br />
[3] C.M. Wang, V.B.C. Tan, T.Y. Zhang, J. Sound Vib.<br />
294, 1060 (2006).<br />
[4] J.N. Reddy, S.D. Pang, J. Appl. Phys. 103, 023511<br />
(2008).<br />
[5] A.C. Eringen, J. Appl. Phys., 54, 4703 (1983).<br />
[6] S.P. Beskou, D. Polyzos, D.E. Beskos, Struct. Eng.<br />
Mech. 15, 705(2003).<br />
[7] Ö. Civalek, Engineering Structures, 26, <strong>17</strong>1(2004).<br />
The results obtained by differential quadrature (DQ)<br />
method [7] using two higher order elasticity theories are<br />
listed in Tables 1-2. In table 1, first three frequencies of<br />
simple supported (S-S) carbon nanotubes are listed for<br />
different gradient parameter. It is shown that, the<br />
frequencies are increased gradually with the increasing<br />
value of g for all modes. Nonlocal parameter also affected<br />
on frequencies (Table 2). When the nonlocal parameters<br />
are increased, the values of frequencies are decreased,<br />
significantly. It is possible to say that, the classical beam<br />
theories can not to capture to size effect on mechanical<br />
behavior of nano sized structures. So, it is suitable to use<br />
some higher order continuum theory such as nonlocal<br />
elasticity theory or gradient strain theory to investigate the<br />
size effect on mechanical behaviour of nano/micro<br />
structures.<br />
6th Nanoscience and Nanotechnology Conference, zmir, <strong>2010</strong> 705