Example of a solution for Dorodnitzyn’s limit formula

C.V. Valencia-Negrete
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Abstract

In the present paper, we show an example of a solution for Dorodnitzyn’s gaseous boundary layer limit formula. Oleinik’s no back-flow condition ensures the existence and uniqueness of solutions for the Prandtl equations in a rectangular domain RR2. It also allowed us to find a limit formula for Dorodnitzyn’s stationary compressible boundary layer with constant total energy on a bounded convex domain in the plane R2. Under the same assumption, we can give an approximate solution u for the limit formula if |u|<<<1 such that: u(z)δcz+62512i04U23z4+o(z5),that corresponds to an approximate horizontal velocity component when a small parameter ϵ given by the quotient of the maximum height of the domain divided by its length tends to zero. Here, c>0, δ is the boundary layer’s height in Dorodnitzyn’s coordinates, U is the free-stream velocity at the upper boundary of the domain, and T0 is the absolute surface temperature.

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Dorodnitzyn极限公式解的例子
本文给出了Dorodnitzyn气体边界层极限公式的一个解的例子。Oleinik的无回流条件保证了矩形域R⊂R2中Prandtl方程解的存在性和唯一性。它还使我们能够在平面R2的有界凸域上找到具有恒定总能量的Dorodnitzyn静止可压缩边界层的极限公式。在相同的假设下,如果|u|<<<;1使得:u(z)Şδ*c*z+625∙12i0∙4U23z4+o(z5),当由域的最大高度除以其长度的商给出的小参数ε趋于零时,这对应于近似的水平速度分量。这里,c>;0,δ是Dorodnitzyn坐标中的边界层高度,U是域上边界的自由流速度,T0是绝对表面温度。
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