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首页> 外文期刊>Journal of the Mechanics and Physics of Solids >Corrigendum: “Band-gaps in electrostatically controlled dielectric laminates subjected to incremental shear motions” (Journal of the Mechanics and Physics of Solids (2012) 60(11) (1970-1981) (S0022509612001159) (10.1016/j.jmps.2012.05.006))
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Corrigendum: “Band-gaps in electrostatically controlled dielectric laminates subjected to incremental shear motions” (Journal of the Mechanics and Physics of Solids (2012) 60(11) (1970-1981) (S0022509612001159) (10.1016/j.jmps.2012.05.006))

机译:勘误:“受到增量剪切运动的静电控制介电层压板中的带隙”(《固体力学与物理学杂志》(2012年)60(11)(1970-1981)(S0022509612001159)(10.1016 / j.jmps.2012.05)。 006))

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摘要

There is a typo in Eq. (47), where λ should be raised to the power 4. We also fix typos in Eqs. (62)-(64), where the correct form of these equations, respectively, is [Formula presented] should read [Formula presented]. Eq. (59) contains associated errors, and its corrected version is [Formula presented]. Following these corrections, the figures are reproduced as follows. Figs. 1-4 revise Figs. 3-7, respectively. In the examples considered in Fig. 1, we observe that larger volume fractions of the soft phase result in gaps at higher frequencies. The width of the gaps increases when the contrast parameters are larger. The dependency on the volume fraction is highlighted in Fig. 2. Therein, we conclusively observe how as the volume fraction of the softer phase increases, the frequencies of the gaps are shifted towards higher frequencies. Conversely, Figs. 3 and 4 show that as the contrast parameters α and β increase, the frequency of the gaps are shifted towards lower frequencies. However, depending on the specific combination of α and β and the number of the gap, its width can either increase or decrease. The quantities in the dispersion relation that affect the width and the location of the gaps are γ, which serves as a measure of the mismatch in the impedance of the phases, and the ratio [Formula presented] and 2. We observe that in general γ does not depend monotonically on α and β, and different values of [Formula presented] demonstrate different dependency on the contrast parameters. Fig. 6 herein revises Fig. 7 of the original paper. Figs. 7 and 8 revise Figs. 8 and 9 of the original paper, respectively, taking H = 100 µm. The revised Figs show that the gaps are shifted towards higher frequencies as functions of the bias field, in agreement with the results of Shmuel (2013).
机译:等式中有一个错字。 (47),其中应将λ提升至4的幂。 (62)-(64),其中这些方程式的正确形式分别为[公式表示],应改为[公式表示]。等式(59)包含相关的错误,其更正版本为[公式表示]。经过这些更正后,这些图复制如下。无花果1-4修改图。 3-7。在图1中考虑的示例中,我们观察到较大的软相体积分数会导致较高频率的间隙。当对比度参数较大时,间隙的宽度会增加。在图2中突出显示了对体积分数的依赖性。在此我们可以确定地观察到,随着软相体积分数的增加,间隙的频率如何向更高的频率偏移。相反,无花果。图3和图4示出,随着对比度参数α和β的增加,间隙的频率朝着更低的频率偏移。但是,根据α和β的特定组合和间隙的数量,其宽度可以增加或减小。色散关系中影响间隙宽度和位置的量为γ,它可以衡量相阻抗的不匹配,其比率为[公式]和2。我们注意到,通常情况下,γ并不单调地依赖于α和β,并且[表示的公式]的不同值表现出对对比度参数的不同依赖。这里的图6修改了原始论文的图7。无花果7和8修改无花果。原始纸张的8和9分别为H = 100 µm。修改后的图显示,随着Shmuel(2013)的结果,作为偏置场的函数,间隙朝着更高的频率移动。

著录项

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  • 作者

    Shmuel Gal; deBotton Gal;

  • 作者单位

    Department of Mechanical Engineering, Ben-Gurion University, Beer-Sheva, Israel;

    Department of Mechanical Engineering, Ben-Gurion University, Beer-Sheva, Israel,Department of Biomedical Engineering, Ben-Gurion University, Beer-Sheva, Israel;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);
  • 原文格式 PDF
  • 正文语种 eng
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