The paper deals with the blow-up rate of positive solutions to the system l 11 l 12 l 21 l 22 Ε½ . u s u q u Β¨, Β¨s Β¨q u Β¨with boundary conditions u 1, t s t x x t x x x Ε½ p 11 p 12 .Ε½ . Ε½ . Ε½ p 21 p 22 .Ε½ . u Β¨1, t and Β¨1, t s u Β¨1, t . Under some assumptions on the x Ε½ . Ε½ . Ε½ . matrices L s l and
Blow-up analysis for a system of heat equations coupled via nonlinear boundary conditions
β Scribed by Xianfa Song
- Publisher
- John Wiley and Sons
- Year
- 2007
- Tongue
- English
- Weight
- 128 KB
- Volume
- 30
- Category
- Article
- ISSN
- 0170-4214
- DOI
- 10.1002/mma.832
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β¦ Synopsis
Abstract
In this paper, we study a system of heat equations $u_t=\Delta u, , v_t=\Delta v,{\rm in},\Omega\times(0,T)$ coupled via nonlinear boundary conditions
Here p, q>0. We prove that the solutions always blow up in finite time for nonβtrivial and nonβnegative initial values. We also prove that the blowβup occurs only on S~R~ = βB~R~ for Ξ© = B~R~ = {x Ο΅ β^n^:|x|<R}and $C_1(T-t)^{-1/2q}\le u(R, t) \le C_2(T-t)^{-1/2q},,\log(c_3(T-t)^{-(q+1)/2pq})\le v(R, t)\le \log(C_4(T-t)^{-(q+1)/2pq})$ under some assumptions on the initial values. Copyright Β© 2007 John Wiley & Sons, Ltd.
π SIMILAR VOLUMES
Under some natural hypothesis on the matrix P"(p GH ) that guarrantee the blow-up of the solution at time ΒΉ, and some assumptions of the initial data u G , we find that if "" x """1 then u G (x , t)goestoinfinitylike(ΒΉ!t) G /2 , where the G (0 are the solutions of (P!Id) ( , )R"(!1, !1)R. As a corol
This note establishes the blow up estimates near the blow up time for a system of heat equations coupled in the boundary conditions. Under certain assumptions, the exact rate of blow up is established. We also prove that the only solution with vanishing initial values when pq G 1 is the trivial one.