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Unsteady separated stagnation-point flow and heat transfer of a viscous fluid over a moving flat surface

机译:在移动平坦表面上不稳定分离的停滞点流量和粘性流体的传热

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摘要

In this paper, we have investigated numerically the laminar unsteady separated stagnation-point flow and heat transfer of a viscous fluid over a moving flat surface in the presence of a time dependent free stream velocity which causes the unsteadiness of this flow problem. The plate is assumed to move in the same or opposite direction of the free stream velocity. The flow is therefore governed by the velocity ratio parameter lambda (ratio of the plate velocity to the free stream velocity) and the unsteadiness parameter beta. When the plate surface moves in the same direction of the free stream velocity (i.e., when lambda 0), the solution of this flow problem continues for any given value of beta. On the other hand, when they move in opposite directions (i.e., when lambda 0), the solution does not exist after a certain value of lambda depending upon the values of beta. In this case, separation appears inside the layer only for a negative value of beta, and for a positive value of beta, the boundary layer solution is terminated after a certain distance from the plate surface with an attached flow solution with no point of inflection. The concerning issue of the steady flow (beta = 0) case has also been considered and two types of attached flow solutions have been found-one with a point of inflection and the other with no point of inflection, in a definite range of lambda (-1.246 58 = lambda = -1.07). However, this range decreases with an increase in vertical bar beta vertical bar when beta 0. A novel result which arises from the heat transfer analysis is that for a given value of lambda (= 0), first the heat transfer rate increases with the increase of the Prandtl number Pr and after attaining a maximum value, it decreases and finally tends to be zero for large values of Pr depending upon the values of beta 0. On the contrary, for a given value of beta (= 0), the rate of heat transfer increases consistently with the increase of Pr. Publ
机译:在本文中,我们已经在数量上研究了层状不稳定分离的停滞点流量,在存在时间依赖的自由流速度存在下在移动平坦表面上通过移动平坦的表面传热,这导致该流动问题的不稳定性。假设板以在自由流速度的相同或相反方向上移动。因此,流动由速度比参数Lambda(板速度与自由流速度的比率)管辖,并且不稳定参数β。当板表面在自由流速度的相同方向上移动时(即,当Lambda& 0)时,该流动问题的溶液继续β的任何给定值。另一方面,当它们沿相反方向移动(即,当LABDA <0时)时,根据β的值,在λ的一定值之后不存在溶液。在这种情况下,分离仅出现在层内,仅针对β的负值,并且对于β的正值,在从板表面与附接流程溶液的一定距离,没有拐点的情况下终止边界层溶液。还考虑了稳定流量(Beta = 0)案例的问题,并发现了两种类型的附加流程解决方案 - 一个具有拐点的点,另一类在一个明确的Lambda范围内,没有拐点没有拐点-1.246 58& λ& = -1.07)。然而,该范围随着ββ垂直杆的增加而减小。从传热分析产生的新结果是,对于λ(= 0)的给定值,首先随着Prandtl数Pr的增加和达到最大值之后,传热速率增加,它降低并最终降低根据β&gt的值,PR值趋于为零。相反,对于给定值的β(& = 0),随着Pr的增加,传热速率始终始终增加。公布

著录项

  • 来源
    《Physics of fluids》 |2018年第4期|共11页
  • 作者

    Dholey S.;

  • 作者单位

    MUC Womens Coll Dept Math Burdwan 713104 W Bengal India;

  • 收录信息
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 流体力学;
  • 关键词

  • 入库时间 2022-08-19 18:20:53

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