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A body-force analogy for dynamics of elastic bodies with eigenstrains

机译:具有特征应变的弹性体动力学的体力类比

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In the linear static theory of thermoelasticity, the body force analogy dates back to Duhamel. In its classical form, it reads: Consider the static deformation of an isotropic linear thermoelastic body under the action of a given temperature. Then the thermal stresses can be obtained by addition of an imaginary pressure to the isothermal stresses, which follow by solving the isothermal governing equations with certain imaginary body forces and surface tractions. Moreover, the thermal displacements due to the given temperature are identical to the isothermal displacements due to the imaginary body forces and surface tractions. In the present paper, a dynamic extension of this body force analogy is presented in the framework of the three-dimensional theory of linear anisotropic elastodynamics with eigenstrains. Our formulation thus includes not only effects such as thermal expansion strains or piezoelectric expansion strains, but also inelastic parts of strains in the framework of a geometrically linear theory. We treat two problems, namely a problem with a given distribution of eigenstrains and with assigned body and surface forces, and a second problem without eigenstrains, but with an auxiliary system of body and surface forces, which we determine such that the required body force analogy holds. It turns out that all what is needed for an extension of the classical static analogy to dynamics is the requirement of identical initial conditions and displacement boundary conditions in the two problems under consideration. We finally present the proper form of the jump conditions for balance of momentum that must be taken into account in the auxiliary problem in order that the body force analogy holds in the presence of a singular surface also.
机译:在热弹性线性静态理论中,体力的类比可以追溯到杜哈默尔(Duhamel)。经典形式为:考虑在给定温度作用下各向同性线性热弹性体的静态变形。然后,可以通过在等温应力上加上虚压来获得热应力,然后通过用一定的虚体力和表面牵引力求解等温控制方程来获得热应力。此外,由于给定温度引起的热位移与由于虚体力和表面牵引力引起的等温位移相同。在本文中,在具有特征应变的线性各向异性弹性动力学的三维理论的框架内,提出了这种体力类比的动态扩展。因此,我们的公式不仅包括诸如热膨胀应变或压电膨胀应变的效应,而且还包括几何线性理论框架内的应变的非弹性部分。我们处理两个问题,即具有给定的本征应变分布和具有指定的体力和表面力的问题,以及第二个不具有本征应变但具有体力和表面力的辅助系统的问题,我们确定该问题使得所需的体力比喻持有。事实证明,将经典的静态类比扩展到动力学所需的全部是对所考虑的两个问题中相同的初始条件和位移边界条件的要求。最后,我们提出了用于动量平衡的跳跃条件的适当形式,在辅助问题中必须考虑这些动量平衡,以便在存在奇异表面的情况下保持体力类比。

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