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arXiv 0907.0223physics.flu-dynphysics.ao-phphysics.comp-ph
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原始turbulence:动力学、普朗特混合长度和冯卡门常数

Primitive turbulence: kinetics, Prandtl's mixing length, and von Karman's constant

Helmut Z. Baumert

摘要:

本文提出了一种渐近高雷诺数下的剪切湍流理论。它是基于作为准粒子的偶极涡管的系综,并以潜在有限长度的环,发夹或细丝对的形式实现。在一个非平行平面的横截面区域,通过一个漩涡缠结,采取局部正交通过每个单独的管,偶极子是经典的偶极子速度移动。旋涡半径与普朗特的经典混合长度直接相关。准粒子表现出偶极混沌,类似于实际气体中的分子混沌。准粒子之间的碰撞导致粒子湮灭(湍流耗散)或粒子散射(湍流扩散)。这些想法足以发展一个封闭的理论剪切产生的湍流没有经验参数,类比的出生和死亡过程的大分子。它几乎与应用于许多科学和技术分支的著名的K-Omega湍流闭合完全一致。在自由均匀衰变的情况下,TKE遵循1/t。对于固体壁的绝热条件,理论预测对数平均流边界层,其冯卡门常数为1/SQRT(2 π)=0.399。

英文摘要:

The paper presents a theory of shear-generated turbulence at asymptotically high Reynolds numbers. It is based on an ensemble of dipole vortex tubes taken as quasi-particles and realized in form of rings, hairpins or filament couples of potentially finite length. In a not necesserily planar cross sectional area through a vortex tangle, taken locally orthogonal through each individual tube, the dipoles are moving with the classical dipole velocity. The vortex radius is directly related with Prandtl's classical mixing length. The quasi-particles perform dipol chaos which reminds of molecular chaos in real gases. Collisions between quasi-particles lead either to particle annihilation (turbulent dissipation) or to particle scattering (turbulent diffusion). These ideas suffice to develop a closed theory of shear-generated turbulence without empirical parameters, with analogies to birth and death processes of macromolecules. It coincides almost perfectly with the well-known K-Omega turbulence closure applied in many branches of science and technology. In the case of free homogeneous decay the TKE is shown to follow 1/t. For an adiabatic condition at a solid wall the theory predicts a logarithmic mean-flow boundary layer with von Karman's constant as 1/SQRT(2 pi)=0.399.

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