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Transient laminar compressible boundary layers over a permeable circular cone near a plane of symmetry

机译:对称平面附近的可渗透圆锥上的瞬态层状可压缩边界层

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The transient laminar compressible boundary layer over a circular cone at an angle of attack near a plane of symmetry in hypersonic flow has been investigated. The case of the boundary layer near the windward and leeward planes has been considered. The effect of suction is included in the analysis which plays an important role in obtaining unique solution. We have examined the situation where the flow is steady at time t = 0 and at time t > 0, the total enthalpy at the wall is suddenly increased and subsequently maintained at that value. This imports unsteadiness in the flow field. The effects of the variable fluid properties, non-unity Prandtl number and viscous dissipation are considered. By suitable transformations, the coupled nonlinear parabolic partial differential equations with three independent variables governing the flow have been reduced to partial differential equations with two independent variables. The resulting partial differential equations have been solved by using an implicit finite-difference scheme in combination with the quasilinearization technique. Computations have been carried out from the initial steady state to the final steady state. It is found that in a small time interval immediately after the start of the impulsive motion, the direction of the heat transfer changes. The surface shear stresses in the streamwise and cross-wise directions and the surface heat transfer, in general, increase with time and attain final steady state values rather quickly (i.e., spin-up time is small). The total enthalpy at the wall strongly affects the surface shear stresses in the streamwise and cross-flow directions and the surface heat transfer, the suction strongly affects the surface shear stress in the streamwise direction and the surface heat transfer, and the cross-flow parameter strongly affects only the cross-flow surface shear stress.
机译:已经研究了在高超声速流动的对称平面附近以一定攻角在圆锥上的瞬态层状可压缩边界层。已经考虑了在迎风面和背风面附近的边界层的情况。分析中包括吸力的影响,在获得独特溶液方面起着重要作用。我们检查了在时间t = 0时流量稳定且在时间t> 0时流量稳定的情况,壁上的总焓突然增加并随后保持在该值。这会导致流场不稳定。考虑了可变流体特性,非单位普朗特数和粘性耗散的影响。通过适当的变换,具有控制流量的三个自变量的耦合非线性抛物型偏微分方程已简化为具有两个自变量的偏微分方程。通过使用隐式有限差分方案结合准线性化技术,可以解决所得的偏微分方程。已经从初始稳态到最终稳态进行了计算。可以发现,在脉冲运动刚开始之后的很小的时间间隔内,传热的方向发生了变化。通常,沿流向和横向的表面剪切应力和表面热传递随时间增加,并且相当快地达到最终稳态值(即,起转时间很小)。壁上的总焓强烈地影响沿流向和横流方向的表面剪切应力以及表面传热,吸力极大地影响沿流向和表面热传递的表面剪切应力以及横流参数仅强烈影响横流表面剪切应力。

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