Faculty of Mechanical Engineering, Technion-Israel Institute of Technology, Haifa, Israel.
Phys Rev E. 2019 Sep;100(3-1):032209. doi: 10.1103/PhysRevE.100.032209.
We study solitary waves in a one-dimensional lattice of identical masses that are connected in series by nonlinear springs. The potential of each spring is nonconvex, where two disjoint convex regions, phase I and phase II, are separated by a concave, spinodal region. Consequently, the force-strain relation of the spring is nonmonotonous, which gives rise to a bistable behavior. Based on analytical treatment, with some approximations, combined with extensive numerical simulations, we are able to reveal important insights. For example, we find that the solitary-wave solution is indifferent to the energy barrier that separates the two energy wells associated with phase I and phase II, and that the shape of the wave can be described by means of merely two scalar properties of the potential of the springs, namely, the ratio of stiffness in phase II and phase I, and the ratio between the Maxwell's force and corresponding transition strain. The latter ratio provides a useful measure for the significance of the spinodal region. Linear stability of the solitary-wave solution is studied analytically using the Vakhitov-Kolokolov criterion applied to the approximate solutions obtained in the first part. These results are validated by numerical simulations. We find that the solitary-wave solution is stable provided that its velocity is higher than some critical value. It is shown that, practically, the solitary waves are stable for almost the entire range of possible wave velocities. This is also manifested in the interaction between two solitary waves or between a solitary wave and a wall (rigid boundary). Such interaction results in a minor change of height and shape of the solitary wave along with the formation of a trail of small undulations that follow the wave, as expected in a nonintegrable system. Even after a significant number of interactions the changes in the wave height and shape are minor, suggesting that the bistable chain may be a useful platform for delivering information over long distances, even concurrently with additional information (other solitary waves) passing through the chain.
我们研究了由相同质量的个体通过非线性弹簧串联而成的一维晶格中的孤波。每个弹簧的势是非凸的,其中两个不相交的凸区域,相 I 和相 II,被一个凹的、旋节线区域隔开。因此,弹簧的力-应变关系是非单调的,这导致了双稳行为。基于解析处理,结合一些近似,以及广泛的数值模拟,我们能够揭示重要的见解。例如,我们发现孤波解对分离相 I 和相 II 两个能量阱的能量势垒不敏感,波的形状可以通过弹簧势的两个标量性质来描述,即相 II 和相 I 的刚度比,以及麦克斯韦力与相应的转变应变之比。后一个比值为旋节线区域的重要性提供了一个有用的度量。利用应用于第一部分中得到的近似解的 Vakhitov-Kolokolov 准则,对孤波解的线性稳定性进行了分析。这些结果通过数值模拟得到了验证。我们发现,只要孤波的速度高于某个临界值,孤波解就是稳定的。实际上,孤波在几乎整个可能的波速范围内都是稳定的。这也体现在两个孤波之间或孤波与刚性边界之间的相互作用中。这种相互作用导致孤波的高度和形状发生微小变化,同时形成跟随波的小波动的尾流,这在不可积系统中是预期的。即使在经过大量相互作用后,波高和形状的变化也很小,这表明双稳链可能是一个有用的平台,可以远距离传输信息,甚至可以同时传输其他信息(其他孤波)。