The onset of flow instability and transition to turbulence in fluids is traditionally characterized using macroscopic parameters such as the Reynolds number. In this work, we propose a complementary microscopic mechanism based on kinetic-theory considerations. Building on a velocity-dependent anisotropic distribution of particle velocities introduced in a recent preprint (Gonuguntla, Zenodo DOI: 10.5281/zenodo.19386768), we show that transverse momentum fluctuations decrease with increasing flow speed, leading to a reduction in transverse pressure and a corresponding loss of restoring forces against perturbations. A critical velocity scale is derived at which transverse fluctuations vanish, and the approach to this regime naturally induces instability. The framework provides a physically transparent connection between microscopic velocity distribution anisotropy and macroscopic flow instability, complementing classical approaches.
Srinivasa Rao Gonuguntla (Fri,) studied this question.
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