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首页> 外文期刊>International Journal of Thermal Sciences >Heat conduction in a semi-infinite medium with time-periodic boundary temperature and a circular inhomogeneity
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Heat conduction in a semi-infinite medium with time-periodic boundary temperature and a circular inhomogeneity

机译:具有时间周期边界温度和圆形不均匀性的半无限介质中的热传导

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We solve the problem of heat conduction in a 2D homogeneous medium (of diffusivity a) below a boundary subjected to time-periodic temperature (of frequency ω), in the presence of a circular in-homogeneity (of radius R), whose center is at distance d > R (depth) from the boundary. This study is a continuation of a previous one which considers a 3D medium with a spherical inhomogeneity. The general solution depends on four dimensionless parameters: d/R, the heat conductivity ratio K, the heat capacity ratio C and the displacement thickness δ/R = {the square root of}(2α/(ωR~2)). An analytical solution is derived as an infinite series of eigenfunctions pertaining to the 2D Helmholtz equation. The solution converges quickly and is shown to be in agreement with a finite element numerical solution. The results are illustrated and analyzed for a given accuracy and for a few values of the governing parameters. A comparison is held with the previous 3D solution pointing out the differences between the two. To widen the range of possible applications, an extension of the solution to a domain of finite depth is also presented. The general solution can be simplified considerably for asymptotic values of the parameters. A first approximation, obtained for R/d1, pertains to an unbounded domain. A further approximate solution, for R/δ1, while κ and C are fixed, can be regarded as pertaining to a quasi-steady regime. However, its accuracy deteriorates for κ1, and a solution, coined as the insulated circle approximation, is derived for this case. Comparison with the exact solution shows that these approximations are accurate for a wide range of parameter values.
机译:我们解决了在圆形非均匀性(半径为R)存在的情况下,在时间周期温度(频率为ω)的边界以下的二维均匀介质(扩散系数为a)中的导热问题。距边界的距离d> R(深度)。这项研究是先前研究的延续,该研究考虑了具有球形不均匀性的3D介质。通用解取决于四个无量纲参数:d / R,导热系数K,热容比C和位移厚度δ/ R = {平方根}(2α/(ωR〜2))。解析解作为与二维Helmholtz方程有关的无穷本征函数序列而得出。该解快速收敛并且显示出与有限元数值解一致。对于给定的精度和一些控制参数值,将对结果进行说明和分析。与之前的3D解决方案进行比较,指出两者之间的差异。为了扩大可能的应用范围,还提出了将解决方案扩展到有限深度域的方法。对于参数的渐近值,一般解决方案可以大大简化。针对R / d 1获得的第一近似值属于无界域。在κ和C固定的情况下,对于R /δ 1的另一种近似解可以被认为与准稳态机制有关。但是,对于κ 1,其精度会下降,并且在这种情况下,得出了一种称为绝缘圆近似的解决方案。与精确解决方案的比较表明,这些近似值对于各种参数值都是准确的。

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