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Photonic crystals in biology - NanoTR-VI

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Poster Session, Thursday, June 17Theme F686 - N1123Free vibration analysis of carbon nanotubes based on nonlocal cont<strong>in</strong>uum and gradientelasticity theoriesÖmer Civalek 1 , Bekir Akgöz, Hakan Ersoy1 Akdeniz University, Civil Eng<strong>in</strong>eer<strong>in</strong>g Department, Division of MechanicsAntalya-TURKIYE, Tel: + 90- 242-310 6319, Fax: + 90-242-310 6306Abstract- Free vibration analysis of s<strong>in</strong>gle walled carbon nanotubes (CNT) is presented based on the Euler-Bernoulli beamtheory. The size effect is taken <strong>in</strong>to consideration us<strong>in</strong>g the Er<strong>in</strong>gen’s non-local elasticity theory. Gradient elasticity theory isalso adopted for model<strong>in</strong>g. The govern<strong>in</strong>g differential equations for CNT vibration is be<strong>in</strong>g solved us<strong>in</strong>g the differentialquadrature (DQ) method. Numerical results are presented to show the effect of nonlocal behavior on frequencies of CNT.The concept of carbon nanotubes (CNTs) was first<strong>in</strong>troduced <strong>in</strong> 1991 by Iijima [1] <strong>in</strong> Japan. Reviews on thedevelopment and application of such nano structures havebeen presented [2]. So, the studies of mechanical behaviorsof carbon nanotubes have be<strong>in</strong>g attracted more and moreattentions of scientists <strong>in</strong> the world and also have become anew research area of applied mechanics [3,4]. In thepresent work, the consistent govern<strong>in</strong>g equations for thebeam model for CNTs are derived for free vibrationanalysis. Nonlocal beam and couple stress beam theoriesare adopted for model<strong>in</strong>g. It is known that, the stress stateof any body at a po<strong>in</strong>t x is related to stra<strong>in</strong> state at the samepo<strong>in</strong>t x <strong>in</strong> the classical elasticity. But this theory is notconflict the atomic theory of lattice dynamics andexperimental observation of phonon dispersion. As statedby Er<strong>in</strong>gen [5] the l<strong>in</strong>ear theory of nonlocal elasticity leadsto a set of <strong>in</strong>tegropartial differential equations for thedisplacements field for homogeneous, isotropic bodies.Accord<strong>in</strong>g to the nonlocal elasticity theory of Er<strong>in</strong>gen’s,the stress at any reference po<strong>in</strong>t <strong>in</strong> the body depends notonly on the stra<strong>in</strong>s at this po<strong>in</strong>t but also on stra<strong>in</strong>s at allpo<strong>in</strong>ts of the body. This def<strong>in</strong>ition of the Er<strong>in</strong>gen’snonlocal elasticity is based on the atomic theory of latticedynamics and some experimental observations on phonondispersion. In the present manuscript two differentapproaches are used for model<strong>in</strong>g of carbon nanotubes.Euler-Bernoulli beam-nonlocal model [5]42 W22 WEI A W ( e0a)A 0 (1)42xxEuler-Bernoulli beam-gradient elasticity theory [6] Wx Wx4422EI g EI A 0 (2)447Table 1. First three frequencies (10) of S-S carbon8nanotubes via gradient theory ( L 510m ,312 2 2300kg/ m , m , t 510 10E 10 N /m )Modeg/L (DQ results)0.005 0.015 0.1251 0.10388 0.10669 0.113742 0.41065 0.41103 0.423013 0.91863 0.92007 0.934857Table 2. First three frequencies (10) of S-S carbon8nanotubes via nonlocal theory( L 510m ,312 2 2300kg/ m , m , t 510 10E 10 N /m )Mode (e 0 a) 2 (DQ results)0 2 41 0.10273 0.10158 0.099622 0.40967 0.40863 0.405533 0.9172 0.90864 0.90637[1] S. Iijima, Nature, 354, 56 (2001).[2] D. Qian, G.J. Wagner, W.K. Liu, Appl. Mech. Rev.,55, 495(2002).[3] C.M. Wang, V.B.C. Tan, T.Y. Zhang, J. Sound Vib.294, 1060 (2006).[4] J.N. Reddy, S.D. Pang, J. Appl. Phys. 103, 023511(2008).[5] A.C. Er<strong>in</strong>gen, J. Appl. Phys., 54, 4703 (1983).[6] S.P. Beskou, D. Polyzos, D.E. Beskos, Struct. Eng.Mech. 15, 705(2003).[7] Ö. Civalek, Eng<strong>in</strong>eer<strong>in</strong>g Structures, 26, 171(2004).The results obta<strong>in</strong>ed by differential quadrature (DQ)method [7] us<strong>in</strong>g two higher order elasticity theories arelisted <strong>in</strong> Tables 1-2. In table 1, first three frequencies ofsimple supported (S-S) carbon nanotubes are listed fordifferent gradient parameter. It is shown that, thefrequencies are <strong>in</strong>creased gradually with the <strong>in</strong>creas<strong>in</strong>gvalue of g for all modes. Nonlocal parameter also affectedon frequencies (Table 2). When the nonlocal parametersare <strong>in</strong>creased, the values of frequencies are decreased,significantly. It is possible to say that, the classical beamtheories can not to capture to size effect on mechanicalbehavior of nano sized structures. So, it is suitable to usesome higher order cont<strong>in</strong>uum theory such as nonlocalelasticity theory or gradient stra<strong>in</strong> theory to <strong>in</strong>vestigate thesize effect on mechanical behaviour of nano/microstructures.6th Nanoscience and Nanotechnology Conference, zmir, 2010 705

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