2019/08/17 by Almog, Yaniv, Helffer, Bernard · 2 citations
#FOS: Physical sciences #Mathematical Physics (math-ph)
paper · doi:10.48550/arxiv.1908.06328
Consider a two-dimensional laminar flow between two plates, so that (x1,x2)∈ \mathbb R ×[-1,1], given by \mathbf v(x1,x2)=(U(x2),0), where U∈ C4([-1,1]) satisfies U^′≠0 in [-1,1]. We prove that the flow is linearly stable in the large Reynolds number limit, in two different cases: \bullet supx∈[-1,1] |U"(x)| + supx∈[-1,1] |U"(x)| ≪ minx∈[-1,1]|U^′(x)| (nearly Couette flows), \bullet U′′≠0 in [-1,1]. We assume either no-slip or fixed traction force conditions on the plates, and an arbitrary large (but much smaller than the Reynolds number) period in the x1 direction.