1999
DOI: 10.1090/s0025-5718-99-01063-7
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Numerical solution of a fast diffusion equation

Abstract: Abstract. In this paper, the authors consider the first boundary value problem for the nonlinear reaction diffusion equation: ut − ∆u m = αu p 1 in Ω, a smooth bounded domain in R d (d ≥ 1) with the zero lateral boundary condition and with a positive initial condition, m ∈ ]0, 1[ (fast diffusion problem), α ≥ 0 and p 1 ≥ m. Sufficient conditions on the initial data are obtained for the solution to vanish or become infinite in a finite time. A scheme for the discretization in time of this problem is proposed. T… Show more

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Cited by 13 publications
(14 citation statements)
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“…√ 5 2 , 2 only the slow diffusion is possible under the condition m > p. In the case of the fast diffusion and superlinear growth in u, v of the right hand sides, the solutions may blow up or vanish in some finite time depending on the initial conditions as illustrated in [11], [40], [41], [46] and the references therein for the simple equation obtained from the first of system (1.1) by letting p = 2, a > 0 constant and all the kernels K i ≡ 0 (observe that in the case when p = q = 2 no restriction on m, n are required, see Remark 2.2). If Ω = R N for such equation we have that the solution blows up for any initial condition in the case when the superlinear growth in u is less than a certain critical exponent, see [46], and the same occurs for doubly degenerate parabolic equations, see [47].…”
Section: +mentioning
confidence: 99%
See 1 more Smart Citation
“…√ 5 2 , 2 only the slow diffusion is possible under the condition m > p. In the case of the fast diffusion and superlinear growth in u, v of the right hand sides, the solutions may blow up or vanish in some finite time depending on the initial conditions as illustrated in [11], [40], [41], [46] and the references therein for the simple equation obtained from the first of system (1.1) by letting p = 2, a > 0 constant and all the kernels K i ≡ 0 (observe that in the case when p = q = 2 no restriction on m, n are required, see Remark 2.2). If Ω = R N for such equation we have that the solution blows up for any initial condition in the case when the superlinear growth in u is less than a certain critical exponent, see [46], and the same occurs for doubly degenerate parabolic equations, see [47].…”
Section: +mentioning
confidence: 99%
“…If Ω = R N for such equation we have that the solution blows up for any initial condition in the case when the superlinear growth in u is less than a certain critical exponent, see [46], and the same occurs for doubly degenerate parabolic equations, see [47]. If the growth is linear or sublinear we do not have blow up of any solution, see [41], hence solutions exist for all t ≥ 0 and in the linear case, depending on the initial condition, they may vanish in finite time or become unbounded as t → +∞ and, thus, the considered initial conditions cannot give rise to a periodic solution.…”
Section: +mentioning
confidence: 99%
“…Recently, a numerical method was proposed in [14] to solve this problem in the special case p 1 = m + 1. An implicit time-discretization was also investigated in [15][16][17] for solving analogous fast and slow diffusion problems on a bounded domain with zero lateral boundary condition and positive initial data. The proposed scheme preserves the essential properties of the initial problem, namely the (possibly) existence of an extinction or a finite blow up time.…”
Section: Introductionmentioning
confidence: 99%
“…Those works were done in the literature of porous media or that of Stefan problems. For fast diffusion problems, we refer to [23,24].…”
Section: Introductionmentioning
confidence: 99%