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Global consequences of a local Casimir force: Adhered cantilever

机译:卡西米尔当地部队的全球后果:依附的悬臂

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摘要

Although stiction is a cumbersome problem for microsystems, it stimulates investigations of surface adhesion. In fact, the shape of an adhered cantilever carries information of the adhesion energy that locks one end to the substrate. We demonstrate here that the system is also sensitive to the dispersion forces that are operative very close to the point of contact, but their contribution to the shape is maximum at about one third of the unadhered length. When the force exceeds a critical value, the cantilever does not lose stability but settles at a smaller unadhered length, whose relation to adhesion energy is only slightly affected by the force. Our calculations suggest the use of adhered cantilevers to measure the dispersion forces at short separations, where other methods suffer from jump-to-contact instability. Simultaneous measurement of the force and adhesion energy allows the separation of the dispersion contribution to the surface adhesion.
机译:尽管粘滞对于微系统来说是一个麻烦的问题,但它刺激了对表面附着力的研究。实际上,粘附的悬臂的形状带有将一端锁定在基板上的粘附能的信息。我们在此证明,该系统对在非常接近接触点时起作用的色散力也很敏感,但它们对形状的贡献最大,约为未粘连长度的三分之一。当力超过临界值时,悬臂不会失去稳定性,而是停留在较小的未粘附长度上,该长度与粘附能的关系仅受该力的影响很小。我们的计算建议使用粘附的悬臂来测量短距离分离时的分散力,而其他方法则存在跳变接触不稳定的问题。力和粘附能的同时测量允许分散体对表面粘附的贡献的分离。

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  • 来源
    《Applied Physics Letters》 |2017年第1期|011603.1-011603.5|共5页
  • 作者单位

    Zernike Institute for Advanced Materials, University of Groningen, Nijenborgh 4, 9747 AG Groningen,The Netherlands,Yaroslavl Branch of the Institute of Physics and Technology, Russian Academy of Sciences,Universitetskaya 21,150007 Yaroslavl, Russia;

    P. G. Demidov Yaroslavl State University, Sovetskaya 14,150000 Yaroslavl, Russia;

    P. G. Demidov Yaroslavl State University, Sovetskaya 14,150000 Yaroslavl, Russia;

    Zernike Institute for Advanced Materials, University of Groningen, Nijenborgh 4, 9747 AG Groningen,The Netherlands;

  • 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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  • 入库时间 2022-08-18 03:14:08

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