SCALING AND CORRELATION OF FLUCTUATING VORTICITY IN TURBULENT WALL LAYERS

R. Panton
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Abstract

Asymptotic expansions for the profiles of fluctuating vorticity in boundary layers are proposed based on DNS data. The inner region requires two terms with different scalings; < ! i ! i > /(U 0 u " 3 / # 2 ) and < ! i ! i > /(u " 4 / # 2 ) . The first term decays exponentially and needs no matching term in the outer region. The second term has an overlap behavior of ~ C / y . To match the outer region this requires a third scaling for the outer expansion < ! i ! i > /(u " 3 / #$ ) . This scaling turns out to be the Kolmogorov time scale. INTRODUCTION From a mathematical viewpoint the theory of turbulent wall layers is a singular perturbation problem for large Reynolds numbers. Profiles are expressed as matched asymptotic expansions. There are three parts; an expansion for the outer region, an expansion for the inner region, and a common part that matches the two. The velocity profile is a well-known example. For the outer region the profile has an expansion consisting of two terms.
紊流壁层脉动涡度的标度及相关性
基于DNS数据,提出了边界层波动涡度剖面的渐近展开式。内部区域需要两个不同比例的项;< !我!i > /(U 0 U " 3 / # 2) and < !我!I > /(u " 4 / # 2)。第一项呈指数衰减,在外区域不需要匹配项。第二项具有~ C / y的重叠行为。为了匹配外部区域,这需要第三次缩放外部扩展< !我!I > /(u " 3 / #$)这个尺度就是柯尔莫哥洛夫时间尺度。从数学角度看,紊流壁层理论是一个大雷诺数下的奇异摄动问题。轮廓被表示为匹配的渐近展开式。有三个部分;外部区域的扩展,内部区域的扩展,以及与两者匹配的公共部分。速度剖面就是一个众所周知的例子。对于外部区域,轮廓具有由两项组成的展开。
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