193 research outputs found

    Large time behavior for a quasilinear diffusion equation with critical gradient absorption

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    International audienceWe study the large time behavior of non-negative solutions to thenonlinear diffusion equation with critical gradient absorption\partial_t u-\Delta_{p}u+|\nabla u|^{q_*}=0 \quad \hbox{in} \(0,\infty)\times\mathbb{R}^N\ ,for p∈(2,∞)p\in(2,\infty) and q∗:=p−N/(N+1)q_*:=p-N/(N+1). We show that theasymptotic profile of compactly supported solutions is given by asource-type self-similar solution of the pp-Laplacian equation with suitable logarithmic time and space scales. In the process, we also get optimal decay rates for compactly supported solutions and optimal expansion rates for their supports that strongly improve previous results

    Instantaneous shrinking and single point extinction for viscous Hamilton-Jacobi equations with fast diffusion

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    International audienceFor a large class of non-negative initial data, the solutions to the quasilinear viscous Hamilton-Jacobi equation ∂tu−Δpu+∣∇u∣q=0\partial_t u-\Delta_p u+|\nabla u|^q=0 in (0,∞)×RN(0,\infty)\times\mathbb{R}^N are known to vanish identically after a finite time when 2N/(N+1)02N/(N+1) 0, the positivity set of u(t)u(t) is a bounded subset of RN\mathbb{R}^N even if u0>0u_0 > 0 in RN\mathbb{R}^N. This decay condition on u0u_0 is also shown to be optimal by proving that the positivity set of any solution emanating from a positive initial condition decaying at a slower rate as ∣x∣→∞|x|\to\infty is the whole RN\mathbb{R}^N for all times. The time evolution of the positivity set is also studied: on the one hand, it is included in a fixed ball for all times if it is initially bounded (\emph{localization}). On the other hand, it converges to a single point at the extinction time for a class of radially symmetric initial data, a phenomenon referred to as \emph{single point extinction}. This behavior is in sharp contrast with what happens when qq ranges in [p−1,p/2)[p-1,p/2) and p∈(2N/(N+1),2]p\in (2N/(N+1),2] for which we show \emph{complete extinction}. Instantaneous shrinking and single point extinction take place in particular for the semilinear viscous Hamilton-Jacobi equation when p=2p=2 and q∈(0,1)q\in (0,1) and seem to have remained unnoticed
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