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A phenomenological model for self-rippling energy of free graphene monolayers

机译:游离石墨烯单层自荡能的现象学模型

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摘要

Several candidate phenomenological expressions are studied for self-rippling energy that drives ripple formation of free single-layer graphene sheets. One phenomenological expression is admitted, while all others are rejected because they cannot admit stable periodic ripple mode. The admitted phenomenological expression contains two terms: one quadratic term which acts like a compressive force and has a destabilizing effect, and another fourth-order term which acts like a nonlinear elastic foundation and has a stabilizing effect. The two associated coefficients depend on specific mechanism of self-rippling and can be determined based on observed wavelength and amplitude of ripple mode. Based on the admitted expression, the effect of an applied force on ripple formation is studied. The present model predicts that the rippling can be controlled or even suppressed with an applied tensile force or collapsed into narrow wrinkles (of deformed wavelengths down to around 2 nm) under an applied compressive force, and the estimated minimum tensile strain to suppress rippling is in remarkable agreement with some known data. Our results show that self-rippling energy dominates ripple formation of sufficiently long free graphene ribbons, although it cannot drive self-rippling of sufficiently short free graphene ribbons. Consequently, a critical length is estimated so that self-rippling occurs only when the length of free single-layer graphene ribbons is much longer than the critical length. The estimated critical length is reasonably consistent with the known fact that self-rippling cannot occur in shorter free graphene sheets (say, of length below 20 nm).
机译:研究了自荡能的几种候选现象学表达式,这些动荡能驱动自由单层石墨烯片的波纹形成。一种现象表达被接受,而所有其他现象表达则被拒绝,因为它们不能接受稳定的周期性波动模式。公认的现象学表达包含两个术语:一个平方项像压缩力一样具有稳定作用,而另一个四阶项像非线性弹性基础一样具有稳定作用。这两个相关系数取决于特定的自波纹机制,并且可以根据观察到的波长和波纹模式的振幅来确定。基于允许的表达式,研究了施加力对波纹形成的影响。本模型预测,通过施加拉伸力可以控制甚至抑制波纹,或者在施加压缩力的情况下塌陷成狭窄的皱纹(变形波长低至2 nm左右),并且抑制波纹的估计最小拉伸应变为与某些已知数据的显着一致性。我们的结果表明,自波纹能量主导着足够长的自由石墨烯带的波纹形成,尽管它不能驱动足够短的自由石墨烯带的自波纹。因此,估计了临界长度,使得仅当自由单层石墨烯带的长度比临界长度长得多时,才会发生自荡。估计的临界长度与已知的事实合理地一致,在较短的自由石墨烯片中(例如,长度低于20 nm)不会发生自波纹。

著录项

  • 来源
    《Journal of Applied Physics》 |2016年第2期|024304.1-024304.9|共9页
  • 作者

    Bingjie Wu; C. Q. Ru;

  • 作者单位

    Department of Mechanical Engineering, University of Alberta, Edmonton T6G 2G8, Canada;

    Department of Mechanical Engineering, University of Alberta, Edmonton T6G 2G8, Canada;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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