30.10.2014 Views

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

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

<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

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!