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Any large solution of a non-linear heat conduction equation becomes monotonic in time

Published online by Cambridge University Press:  14 November 2011

Victor A. Galaktionov
Affiliation:
Keldysh Institute of Applied Mathematics, Miusskaya pl. 4, 125047 Moscow, U.S.S.R
Sergey A. Posashkov
Affiliation:
Keldysh Institute of Applied Mathematics, Miusskaya pl. 4, 125047 Moscow, U.S.S.R

Synopsis

In this paper we prove a certain monotonicity in time of non-negative classical solutions of the Cauchy problem for the quasilinear uniformly parabolic equation u1 = (ϕ(u))xx + Q(u) in wT = (0, T] × R1 with bounded sufficiently smooth initial function u(0, x) = uo(x)≧0 in Rl. We assume that ϕ(u) and Q(u) are smooth functions in [0, +∞) and ϕ′(u) >0, Q(u) > 0 for u > 0. Under some additional hypothesis on the growth of Q(u)ϕ′(u) at infinity, it is proved that if u(to, xo) becomes sufficiently large at some point (to, xo) ∈ wT, then ut(t, x0) ≧0 for all t ∈ [t0, T]. The proof is based on the method of intersection comparison of the solution with the set of the stationary solutions of the same equation. Some generalisations of this property for a quasilinear degenerate parabolic equation are discussed.

Type
Research Article
Copyright
Copyright © Royal Society of Edinburgh 1991

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References

1Angenent, S.. The zero set of a solution of a parabolic equation. J. Reine Angew. Math. 390 (1988), 7996.Google Scholar
2Friedman, A.. On the regularity of the solutions of non-linear elliptic and parabolic systems of partial differential equations. J. Math. Mech. 7 (1958), 4359.Google Scholar
3Friedman, A.. Partial Differential Equations of Parabolic Type (Englewood Cliffs, New Jersey: Prentice-Hall, 1964).Google Scholar
4Galaktionov, V. A. and Posashkov, S. A.. New variants of using of strong maximum principle for parabolic equations and some applications (Preprint, Keldysh Inst. Appl. Math. Acad. Sci. USSR, Moscow, 1985, no. 167 (in Russian)).Google Scholar
5Galaktionov, V. A. and Posashkov, S. A.. Applications of new comparison theorems for unbounded solutions of nonlinear parabolic equations. Differntsial'nye Uravneniya 22 (1986), 11651173 (in Russian).Google Scholar
6Kinderlehrer, G. and Nirenberg, L.. Analyticity at the boundary of solutions of nonlinear second-order parabolic equations. Comm. Pure Appl. Math. 31 (1978), 283338.CrossRefGoogle Scholar
7Komatsu, G.. Analyticity up to the boundary of solutions of nonlinear parabolic equations. Comm. Pure Appl. Math. 32 (1979), 669720.CrossRefGoogle Scholar
8Samarskii, A. A., Galaktionov, V. A., Kurdjumov, S. P. and Mikhailov, A. P., Blow-up in Problems for Quasilinear Parabolic Equations (Moscow: Nauka, 1987 (in Russian)).Google Scholar
9Sattinger, D. H.. On the total variation of solution of parabolic equations. Math. Ann. 183 (1969), 7892.Google Scholar