2020
DOI: 10.48550/arxiv.2009.06513
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Well-posedness of the MHD boundary layer system in Gevrey function space without Structural Assumption

Abstract: We establish the well-posedness of the MHD boundary layer system in Gevrey function space without any structural assumption. Compared to the classical Prandtl equation, the loss of tangential derivative comes from both the velocity and magnetic fields that are coupled with each other. By observing a new type of cancellation mechanism in the system for overcoming the loss derivative degeneracy, we show that the MHD boundary layer system is well-posed with Gevrey index up to 3/2 in both two and three dimensional… Show more

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“…Yang [13] with Gevrey index up to 3/2, and it remains interesting to relax the Gevrey index therein to 2 inspired the previous works of [4,11] on the well-posedness for the Prandtl equations in Gevrey space with optimal index 2. • Under the structural assumption that the tangential magnetic field dominates, i.e., f = 0, the well-posedness in weighted Sobolev space was established by Liu-Xie-Yang [17] and Liu-Wang-Xie-Yang [15] without Oleinik's monotonicity assumption, where the two cases that with both viscosity and resistivity and with only viscosity are considered, respectively.…”
Section: Introductionmentioning
confidence: 95%
“…Yang [13] with Gevrey index up to 3/2, and it remains interesting to relax the Gevrey index therein to 2 inspired the previous works of [4,11] on the well-posedness for the Prandtl equations in Gevrey space with optimal index 2. • Under the structural assumption that the tangential magnetic field dominates, i.e., f = 0, the well-posedness in weighted Sobolev space was established by Liu-Xie-Yang [17] and Liu-Wang-Xie-Yang [15] without Oleinik's monotonicity assumption, where the two cases that with both viscosity and resistivity and with only viscosity are considered, respectively.…”
Section: Introductionmentioning
confidence: 95%