Mayer Andreas P, Kovalev Alexander S
Institut für Theoretische Physik, Universität Regensburg, 93040 Regensburg, Germany.
Phys Rev E Stat Nonlin Soft Matter Phys. 2003 Jun;67(6 Pt 2):066603. doi: 10.1103/PhysRevE.67.066603. Epub 2003 Jun 9.
The problem of the existence of evelope solitons in elastic plates and at solid surfaces covered by an elastic film is revisited with special attention paid to nonlinear long-wave short-wave interactions. Using asymptotic expansions and multiple scales, conditions for the existence of envelope solitons are established and it is shown how their parameters can be expressed in terms of the elastic moduli and mass densities of the materials involved. In addition to homogeneous plates, weak periodic modulation of the plate's material parameters are also considered. In the case of wave propagation in an elastic plate, modulations of weakly nonlinear carrier waves are governed by a coupled system of partial differential equations consisting of evolution equations for the complex amplitude of the carrier wave (the nonlinear Schrödinger equation for envelope solitons and the Mills-Trullinger equations for gap solitons), and the wave equation for long-wavelength acoustic plate modes. In contrast to this situation, envelope solitons of surface acoustic waves in a layered structure are normally described by the nonlinear Schrödinger equation alone. However, at higher orders of the carrier wave amplitude, the envelope soliton is found to be accompanied by a quasistatic long-wavelength strain field, which may be localized at the surface with penetration depth into the substrate of the order of the inverse amplitude or which may radiate energy into the bulk. A new set of modulation equations is derived for the resonant case of the carrier wave's group velocity being equal to the phase velocity of long-wavelength Rayleigh waves of the uncoated substrate.
重新审视了弹性板以及覆盖有弹性薄膜的固体表面中包络孤子的存在问题,特别关注非线性长波 - 短波相互作用。利用渐近展开和多尺度方法,建立了包络孤子存在的条件,并展示了如何根据所涉及材料的弹性模量和质量密度来表示它们的参数。除了均匀板之外,还考虑了板材料参数的弱周期调制。在弹性板中的波传播情况下,弱非线性载波的调制由一个耦合的偏微分方程组控制,该方程组由载波复振幅的演化方程(包络孤子的非线性薛定谔方程和能隙孤子的米尔斯 - 特鲁林格方程)以及长波长声学板模式的波动方程组成。与这种情况相反,分层结构中表面声波的包络孤子通常仅由非线性薛定谔方程描述。然而,在载波振幅的高阶情况下,发现包络孤子伴随着一个准静态长波长应变场,该应变场可能局域在表面,穿透深度进入基底的量级为振幅的倒数,或者可能向体中辐射能量。针对载波群速度等于未涂层基底的长波长瑞利波相速度的共振情况,推导了一组新的调制方程。