2005
DOI: 10.1103/physrevb.71.195412
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Flexural wave propagation in single-walled carbon nanotubes

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Cited by 474 publications
(216 citation statements)
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“…Also the range of e 0 is rather wide from a value of near 0-4. This result is significantly different from the constant value of 0.288 adopted by Wang and Hu, 1 3 There is a critical value of ͑for different modes͒ after which the scaling parameter e 0 takes on a zero value; in other words, the beam theory reduces to a local beam model. Figure 3 shows the calibrated e 0 for the second, third, and fourth flexural modes of SWCNT with CF boundary condition.…”
Section: MD Calibration Of E 0 and Discussioncontrasting
confidence: 45%
“…Also the range of e 0 is rather wide from a value of near 0-4. This result is significantly different from the constant value of 0.288 adopted by Wang and Hu, 1 3 There is a critical value of ͑for different modes͒ after which the scaling parameter e 0 takes on a zero value; in other words, the beam theory reduces to a local beam model. Figure 3 shows the calibrated e 0 for the second, third, and fourth flexural modes of SWCNT with CF boundary condition.…”
Section: MD Calibration Of E 0 and Discussioncontrasting
confidence: 45%
“…Since the first publication of nonlocal elasticity theory by Eringen and his associate, 1-3 many articles have been published on the application of this model in nanomechanics, particularly in the early 21st century, such as Peddieson et al, 4 Sudak, 5 Zhang et al, 6 Wang, 7,8 Lu et al, 9 Xu, 10 Wang and Hu, 11 etc. Almost all articles presented a simplified nonlocal beam model by assuming that the beam midplane is governed by a second-order ordinary differential equation, while in the transverse direction the classical Euler-Bernoulli beam model or the Timoshenko beam model applies.…”
Section: Introductionmentioning
confidence: 99%
“…So far, no experi- 49 who adopted the second-order strain gradient constitutive relation, proposed e 0 = 0.288 for the flexural wave propagation study in a single walled carbon nanotube through the use of the nonlocal Timoshenko beam model and MD simulations. Eringen 50 himself proposed e 0 as 0.39 based on the matching of the dispersion curves via nonlocal theory for plane wave and Born-Karman model of lattice dynamics at the end of the Brillouin zone, ka = , where a is the distance between atoms and k is the wave number in the phonon analysis.…”
Section: Small Length Scale Effect and Vibrations Of Nonlocal CImentioning
confidence: 99%