首页> 外文期刊>Journal of thermal stresses >D'ALEMBERT'S SOLUTION IN THERMOELASTICITY - IMPACT OF A ROD AGAINST A HEATED BARRIER: PART II. A CASE OF COUPLED STRAIN AND TEMPERATURE FIELDS
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D'ALEMBERT'S SOLUTION IN THERMOELASTICITY - IMPACT OF A ROD AGAINST A HEATED BARRIER: PART II. A CASE OF COUPLED STRAIN AND TEMPERATURE FIELDS

机译:D'ALEMBERT的热弹性解决方案-杆对加热壁垒的影响:第二部分。应变和温度场耦合的情况

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The problem of impact of a thermoelaslic rod against a heated rigid harrier is considered, in so doing lateral surfaces and free end of the rod are heat insulated, and free heat exchange between the rod and the rigid obstacle or ideal thermal contact occurs within contacting end. The rod's thermoelastic behavior is described by the Green-Naghdi theory of thermoelasticity. D'Alembert's method, which is based on the analytical solution of equations of the hyperbolic type describing the dynamic behavior of the thermoelastic rod, is used as the method of solution. This solution involves four arbitrary functions which are determined from the initial and boundary conditions and are piecewise constant functions. The procedure developed enables one to analyze the influence of thermoelastic parameters on the values to be found and to investigate numerically the longitudinal coordinate dependence of the desired functions at each fixed instant of the time beginning from the moment of the rod's collision with the barrier up to the moment of its rebound both without account for the stress and temperature fields coupling (in the companion paper, Part I) and in the case of coupling thermoelasticity (in this paper). As a numerical example, the impact of a thermoelastic rod against a heated barrier is considered with a small parameter of coupling between the strain and temperature fields. It has been shown that the presence of small coupling results in the generation of a new shock wave of small amplitude, namely: the reflected thermal wave from the incident elastic wave at the free rod's end. The rod's rebound may occur either at the moment of simultaneous arrival at the contact place of two reflected waves: elastic wave from the incident thermal wave and thermal wave from the incident elastic wave-or at the time when the reflected elastic-wave from the incident elastic wave reaches the contact point.
机译:考虑了热弹性杆对加热的刚性的撞击问题,这样做是为了使杆的侧面和自由端隔热,并且杆和刚性障碍物之间的自由热交换或理想的热接触发生在接触端内。杆的热弹性行为由Green-Naghdi热弹性理论描述。求解方法是基于描述双曲线类型方程的热解的D'Alembert方法,该双曲线类型的方程描述了热弹性杆的动态行为。此解决方案涉及四个任意函数,这些函数是根据初始条件和边界条件确定的,它们是分段常数函数。所开发的程序使人们能够分析热弹性参数对要找到的值的影响,并从杆与障碍物碰撞的时刻开始,一直到从固定杆到碰撞的每一固定时刻,以数字方式研究所需功能的纵向坐标依赖性。它的回弹力矩既不考虑应力场和温度场的耦合(在随附的论文,第I部分)中,又不考虑热弹性的耦合(在本文中)。作为一个数值示例,考虑了热弹性杆对热障的冲击,其应变和温度场之间的耦合参数很小。已经表明,小耦合的存在会导致产生新的小振幅冲击波,即:自由杆端部入射弹性波反射的热波。杆的回弹可能在同时到达两个反射波的接触点时发生:从入射热波产生的弹性波和从入射弹性波产生的热波-或从入射波反射的弹性波时弹性波到达接触点。

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