Asymptotic behaviour of solutions of the fast diffusion equation near its extinction time

preprint2014arXivOpen access

Abstract

Let n≥3n\ge 3, 0<m<n−2n0<m<\frac{n-2}{n}, ρ1>0ρ_1>0, β≥mρ1n−2−nmβ\ge\frac{mρ_1}{n-2-nm} and α=2β+ρ11−mα=\frac{2β+ρ_1}{1-m}. For any λ>0λ>0, we will prove the existence and uniqueness (for β≥ρ1n−2−nmβ\ge\frac{ρ_1}{n-2-nm}) of radially symmetric singular solution gλ∈C∞(Rn∖{0})g_λ\in C^{\infty}(R^n\setminus\{0\}) of the elliptic equation Δvm+αv+βx⋅∇v=0Δv^m+αv+βx\cdot\nabla v=0, v>0v>0, in Rn∖{0}R^n\setminus\{0\}, satisfying lim⁡∣x∣→0∣x∣α/βgλ(x)=λ−ρ1(1−m)β\displaystyle\lim_{|x|\to 0}|x|^{α/β}g_λ(x)=λ^{-\frac{ρ_1}{(1-m)β}}. When ββ is sufficiently large, we prove the higher order asymptotic behaviour of radially symmetric solutions of the above elliptic equation as ∣x∣→∞|x|\to\infty. We also obtain an inversion formula for the radially symmetric solution of the above equation. As a consequence we will prove the extinction behaviour of the solution uu of the fast diffusion equation ut=Δumu_t=Δu^m in Rn×(0,T)R^n\times (0,T) near the extinction time T>0T>0.

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