拉伸/收缩表面上的滞止点流动分析

IF 0.7 Q3 MATHEMATICS, APPLIED
M'bagne F. 'bengue, J. Paullet
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引用次数: 0

摘要

。本文分析了幂律外流流过与外流速度成正比的表面时的滞止点流动的边值问题。流动由两个物理参数表征;ε表示薄片相对于外部流动的拉伸(ε >)或收缩(ε < 0), n >表示幂律指数。对于辅助流(ε > 0),当(拉伸)表面与外流沿同一方向运动时,我们证明了所有n值的解的存在性。对于ε < 0的反向流动,即(收缩)表面与外流方向相反,情况就复杂得多。对于−1 < ε < 0和所有n,证明了一个解的存在。然而,对于ε (cid:2)−1,我们证明了ε (cid:2)−1存在一个值ε crit (n) (cid:2)−1,使得ε (cid:2) ε crit不存在解。对于n = 1 / 7和n = 1 / 3,证明了ε临界值= - 1。对于n的其他值,我们推导了边界,说明了相反(ε < 0)流的存在/不存在边界的复杂性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Analysis of stagnation point flow over a stretching/shrinking surface
. In this article we analyze the boundary value problem governing stagnation-point fl ow of a fl uid with a power law outer fl ow over a surface moving with a speed proportional to the outer fl ow. The fl ow is characterized by two physical parameters; ε , which measures the stretching ( ε > 0) or shrinking ( ε < 0) of the sheet relative to the outer fl ow, and n > 0, the power law exponent. In the case of aiding fl ow ( ε > 0), where the (stretching) surface and the outer fl ow move in the same direction, we prove existence of a solution for all values of n . For opposing fl ow ( ε < 0), where the (shrinking) surface and the outer fl ow move in opposite directions, the situation is much more complicated. For − 1 < ε < 0 and all n we prove a solution exists. However, for ε (cid:2) − 1, we prove there exists a value, ε crit ( n ) (cid:2) − 1, such that no solutions exist for ε (cid:2) ε crit . For n = 1 / 7 and n = 1 / 3 we prove that ε crit = − 1. For other values of n , we derive bounds which illustrate the complicated nature of the existence/nonexistence boundary for opposing ( ε < 0) fl ows.
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