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Uniqueness and reciprocal theorems in linear micropolar electro-magnetic thermoelasticity with two relaxation times

机译:具有两个松弛时间的线性微极电磁热弹性的唯一性和倒易定理

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摘要

A general model for the linear micropolar electro-magnetic thermoelastic continuum based on the hyperbolic heat equation, which is physically more relevant than the classical thermoelasticity theory in analyzing problems involving very short intervals of time and/or very high heat fluxes, is introduced. An integral identity that involves two admissible processes at different instants is established. Uniqueness theorem is proved, with no definiteness assumption on the elastic constitutive coefficients and no restrictions on the electro-elastic coupling moduli, magneto-elastic coupling moduli, and thermal coupling coefficients other than symmetry conditions. The reciprocity theorem is derived, without the use of Laplace transforms. The integral representation formula is obtained in case instantaneous concentrated, time-continuous or time-harmonic loads are applied. The Maysel’s, Somigliana’s and Green’s formulas are derived. The mixed boundary value problem is considered and a system of five singular Fredholm integral equations is obtained. The results for dynamic classical coupled theory can be easy deduced from the given general model formulated for the temperature-rate dependent thermoelasticity.
机译:引入了基于双曲热方程的线性微极电磁热弹性连续体的通用模型,该模型在分析涉及非常短的时间间隔和/或非常高的热通量的问题上比经典的热弹性理论更重要。建立了涉及不同时刻两个可允许过程的完整身份。证明了唯一性定理,除了对称性条件外,没有对弹性本构系数的确定性假设,对电弹性耦合模量,磁弹性耦合模量和热耦合系数没有限制。在不使用拉普拉斯变换的情况下,得出了互易定理。如果应用瞬时集中载荷,时间连续载荷或时间谐波载荷,则可获得积分表示公式。推导了Maysel,Somigliana和Green的公式。考虑混合边值问题,得到一个包含五个奇异Fredholm积分方程的系统。动态经典耦合理论的结果可以很容易地从给定的基于温度速率的热弹性公式中得出。

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