2003
DOI: 10.1016/s0020-7683(03)00056-8
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A structural mechanics approach for the analysis of carbon nanotubes

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Cited by 1,255 publications
(998 citation statements)
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References 28 publications
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“…Odegard et al [18] developed a model that links the molecular mechanics and solid mechanics, which is established by equating the molecular potential energy terms with the mechanical strain energy of a representative volume element of a continuum model. Li and Chou in the works [19][20][21][22] developed a similar approach to model CNTs and GSs similar to space-frame structures and investigated the elastic, vibrational and buckling characteristics of CNTs and/or GSs. Cantilevered and bridged single walled carbon nanotubes (SWCNTs) are taken into account to predict fundamental frequencies of SWCNTs [21] that are found to be in the range of 10 GHz -1.5 THz.…”
Section: Introductionmentioning
confidence: 99%
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“…Odegard et al [18] developed a model that links the molecular mechanics and solid mechanics, which is established by equating the molecular potential energy terms with the mechanical strain energy of a representative volume element of a continuum model. Li and Chou in the works [19][20][21][22] developed a similar approach to model CNTs and GSs similar to space-frame structures and investigated the elastic, vibrational and buckling characteristics of CNTs and/or GSs. Cantilevered and bridged single walled carbon nanotubes (SWCNTs) are taken into account to predict fundamental frequencies of SWCNTs [21] that are found to be in the range of 10 GHz -1.5 THz.…”
Section: Introductionmentioning
confidence: 99%
“…Li and Chou [22] reported that the buckling load in axial compression is higher than bending load. Tserpes and Papanikos [23] introduced an atomistic FE method based on the approach of Li and Chou [19] to model CNTs by using commercial FE codes; they identified the C-C bond thickness d, Young's modulus E and shear modulus G by using the AMBER force model [19]. By using the methods developed by Li and Chou [19] and Tserpes and Papanikos [23]; Hashemnia et al [24] and Sakhaee-Pour et al [25] examined natural frequencies and mode shapes of single-layered graphene sheets (SLGSs) and Sakhaee-Pour et al [25] predicted fundamental frequencies of SLGSs with equivalent lengths that are found to be in the range of 2.4 GHz -3.5 THz; Sakhaee-Pour et al [26] studied natural frequencies and mode shapes SWCNTs; Sakhaee-Pour [27] analyzed elastic buckling of SLGSs; Lee and Lee [28] studied vibrational behaviors of SWCNTs and SWCNCs, and predicted fundamental frequencies of SWCNCs below 20 GHz with a cone having the height of 20 Ǻ; Mir et al [29] studied natural frequencies and mode shapes of SWCNTs; Cheng et al [30] and Fan et al [31] examined mechanical properties of CNTs such as Young's modulus, shear modulus, natural frequency and buckling load; Avila et al [32] analyzed elastic and vibrational properties of GSs and CNTs; we studied twoand three-dimensional modal and transient analyses of SLGSs in [33].…”
Section: Introductionmentioning
confidence: 99%
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