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111.
A GENERALIZED THERMOELASTIC DIFFUSION PROBLEM OF THIN PLATE HEATED BY THE ULTRASHORT LASER PULSES 1)
由于超短激光脉冲具有功率密度高、持续时间短、加工精度高等优势, 近年来被广泛应用于超精细加工、光学储存和微电子器件制造等领域. 本文基于L-S型广义热弹扩散理论, 建立了考虑材料记忆依赖效应和空间非局部效应的记忆依赖型非局部广义热弹扩散耦合理论, 它能够准确预测几何尺寸与内部特征尺寸相近结构的热弹扩散瞬态响应. 推导了所建理论的控制方程, 并基于拉普拉斯积分变换获得了控制方程的解. 作为算例, 利用所建理论和求解方法研究了半无限大薄板受非高斯激光脉冲加热和化学冲击联合作用下的热弹扩散瞬态响应问题, 得到了薄板的温度、化学势、位移、应力和浓度等随非局部参数、热时间迟滞因子和扩散时间迟滞因子等参数变化的分布规律. 结果表明: 传热对传质影响显著, 传质对传热影响甚微; 非局部参数对位移、应力影响显著, 对温度、化学势和浓度几乎没有影响. 该理论及求解方法的建立, 旨在实现材料在机械、热、化学势等冲击作用下传热传质瞬态响应的准确预测. 相似文献
112.
Moncef Aouadi 《Zeitschrift für Angewandte Mathematik und Physik (ZAMP)》2006,57(6):1057-1074
The model of the equations of generalized linear micropolar thermoelasticity with two relaxation times in an isotropic medium
with temperature-dependent mechanical properties is established. The modulus of elasticity is taken as a linear function of
reference temperature. Laplace and exponential Fourier transform techniques are used to obtain the solution by a direct approach.
The integral transforms have been inverted by using a numerical technique to obtain the temperature, displacement, force and
couple stress in the physical domain. The results of these quantities are given and illustrated graphically. A comparison
is made with results obtained in case of temperature-independent modulus of elasticity. The problem of generalized thermoelasticity
has been reduced as a special case of our problem. 相似文献
113.
研究了在应力自由和刚性固定边界条件下,无能量耗散的均匀、各向同性微极热弹性无限板的轴对称自由振动波的传播,导出了相应的对称和斜对称模态波传播的闭合式特征方程和不同区域的特征方程.对短波的情况,应力自由热绝缘和等温板中对称和斜对称模态波传播的特征方程退化为Rayleigh表面波频率方程.根据导出的特征方程得到了热弹性、微极弹性和弹性板的结果.在对称和斜对称运动中计算了板的位移分量幅值、微转动幅值和温度分布,给出了对称和斜对称模式的频散曲线,并示出了位移分量和微转动幅值和温度分布的曲线.能够发现理论分析和数值结论是非常一致的. 相似文献
114.
115.
I. Chudinovich 《Applicable analysis》2013,92(7):961-975
The initial-boundary value problem for bending of a thermoelastic plate weakened by a crack, with Neumann-type boundary conditions along the edges of the crack, is studied, and its unique solvability in spaces of distributions is proved by means of a combination of the Laplace transformation and variational methods. 相似文献
116.
In this article, the propagation of guided thermoelastic waves in the circumferential direction of orthotropic cylindrical curved plates subjected to stress-free, isothermal boundary conditions is investigated in the context of the Green-Naghdi (GN) generalized thermoelastic theory (without energy dissipation). The coupled wave equations and heat conduction equation are solved by the Legendre orthogonal polynomial series expansion approach. The convergency of the method is discussed through a numerical example. The dispersion curves of thermal modes and elastic modes are illustrated simultaneously. Dispersion curves of the corresponding pure elastic cylindrical plate are also shown to analyze the influence of the thermoelasticity on elastic modes. The displacement, temperature and stress distributions are shown to discuss the differences between the elastic modes and thermal modes. A thermoelastic cylindrical plate with a different ratio of radius to thickness is considered to discuss the influence of the ratio on the characteristics of circumferential thermoelastic waves. 相似文献
117.
For β ∈ R, the authors consider the evolution system in the unknown variables u and α { ttu+ xxxxu+ xxtα+(β+|| xu||L2^2) xxu=f, ttα- xxα- xxtα- xxtu=0} describing the dynamics of type III thermoelastic extensible beams, where the dissipation is entirely contributed by the second equation ruling the evolution of the thermal displacement α. Under natural boundary conditions, the existence of the global attractor of optimal regularity for the related dynamical system acting on the phase space of weak energy solutions is established. 相似文献
118.
基于经典弹性薄板理论和单向耦合热传导理论,研究了材料性质沿厚度连续变化的功能梯度微圆板的热弹性阻尼特性.首先,考虑热力耦合效应,建立了功能梯度微圆板轴对称横向自由振动微分方程.然后,忽略温度梯度在面内的变化,建立了单向耦合变系数一维热传导方程.采用分层均匀化近似方法,将变系数热传导方程转化为一系列常系数的微分方程,利用上下表面的热边界条件和层间连续性条件获得了微圆板温度场解析解.将所得温度场代入微圆板的自由振动微分方程,得到了包含热弹性阻尼的复频率,从而获得了反映热弹性阻尼水平的逆品质因子.最后,针对材料性质沿板厚按幂函数变化的陶瓷-金属功能梯度微圆板,定量地分析材料梯度指数、几何尺寸、边界条件、温度环境等对微圆板热弹性阻尼的影响. 相似文献
119.
In this paper we give a necessary and sufficient algebraic conditionfor the approximate controllability of the following thermoelasticplate equation with Dirichlet boundary conditions wtt + 2w + = a1(x)u1 + ... + am(x)um, t 0, x , t ß wt = d1(x)u1 + ... + dm(x)um,t 0, x , = w = w = 0, t 0, x , where 0, ß > 0, is a sufficiently regular boundeddomain in RN, ai, di, L2 (; R), the control functions ui L2(0, t1; R); i = 1, 2, ..., m. This condition is easy to checkand is given by Rank [PjBAjPjBA2jPjB ... A3j1jPjB] = 3j,BU=b1U1+...+bmUm,bi=[0, ai, di], Aj=[0, 2j, 0, 1, 0, j, 0, j, ßj]Pj, j1, where j, S are the eigenvalues of with Dirichlet boundarycondition and Pj, S are the projections on the correspondingeigenspace. 相似文献
120.
Using the method of separation of variables, an exact solution is constructed for some boundary value and boundary-contact problems of thermoelastic equilibrium of one- and multilayer bodies bounded by the coordinate surfaces of generalized cylindrical coordinates , , z. , are the orthogonal coordinates on the plane and z is the linear coordinate. The body, occupying the domain = {0 < < 1, 0 < < 1, 0 < z < z
1}, is subjected to the action of a stationary thermal field and surface disturbances (such as stresses, displacements, or their combinations) for z = 0 and z = z
1. Special type homogeneous conditions are given on the remainder of the surface. The elastic body is assumed to be transversally isotropic with the plane of isotropy z = const and nonhomogeneous along z. The same assumption is made for the layers of the multilayer body which contact along z = const. 相似文献