On Degenerate Parabolic Equations
Abstract
The paper deals with the existence of solutions of some generalized Stefan-type equation in the framework of Orlicz spaces.
1. Introduction
In [7], a different approach was introduced to study the porous and Stefan problems.The enthalpy formulation and the variational technique are used. Nonstandard semidiscretization in time is used, and Newton-like iterations are applied to solve the corresponding elliptic problems.
Due to the possible jumps of θ, problem P enters the class of Stefan problems. In the present paper, we are interested in the parabolic problem with regular data. It is similar in many respects to the so-called porous media equation. However, the equation we consider has a more general structure than that in the references above.
Two main difficulties appear in the study of existence of solutions of problem P. The first one comes from the diffusion terms in P since they do not depend on u but on θ(u), and, moreover, at the same time, P poses big problems, since in general we have not information on u but on θ(u). For the last reason, the authors in [8] define a new notion of weak solution to overcome this problem.
In the above cited references, the authors have shown the existence of a weak solution when the function a(x, t, ξ) was assumed to satisfy a polynomial growth condition with respect to ∇u. When trying to relax this restriction on the function a(·, ξ), we are led to replace the space Lp(0, T; W1,p(Ω)) by an inhomogeneous Sobolev space W1,xLB built from an Orlicz space LB instead of Lp, where the N-function B which defines LB is related to the actual growth of the Carathéodory’s function.
Our goal in this paper is, on the one hand, to give a generalization of E in the case of one equation in the framework of Leray-Lions operator in Orlicz-Sobolev spaces. on the second hand, we prove the existence of solutions in the BV(Q) space.
2. Preliminaries
Let M : R+ → R+ be an N-function, that is, M is continuous, convex, with M(t) > 0 for t > 0, M(t)/t → 0 as t → 0, and M(t)/t → ∞ as t → ∞. The N-function conjugate to M is defined by .
Note that LM(Ω) is a Banach space under the norm ∥u∥M,Ω = inf {λ > 0 : ∫ΩM(u(x)/λ)dx ≤ 1} and ℒM(Ω) is a convex subset of LM(Ω). The closure in LM(Ω) of the set of bounded measurable functions with compact support in is denoted by EM(Ω). In general, EM(Ω) ≠ LM(Ω) and the dual of EM(Ω) can be identified with by means of the pairing ∫Ωu(x)v(x)dx, and the dual norm on is equivalent to .
We say that un converges to u for the modular convergence in LM(Ω) if, for some λ > 0, ∫ΩM((un − u)/λ)dx → 0. This implies convergence for .
The inhomogeneous Orlicz-Sobolev spaces are defined as follows: . These spaces are considered as subspaces of the product space ΠLM(Q) which have as many copies as there are α-order derivatives, |α | ≤ 1. We define the space . (For more details, see [9].)
3. Main Result
Before giving our main result, we give the following lemma which will be used.
Lemma 3.1 (see [10].)Under the hypothesis (1.2)–(1.4), θ(s) = s, the problem P admits at least one solution u in the following sense:
Theorem 3.2. Under the hypothesis (1.2)–(1.5), the problem (P0) admits at least one solution u in the following sense:
Proof.
Step 1 (approximation and a priori estimate). Consider the approximate problem:
The approximate problem has a regular solution un and in particular (by Lemma 3.1).
Let .
Let v = θ(un)χ(0,τ) as test function, one has
There exist a measurable function v and a subsequence, also denoted (un), such that,
Let us consider the C2 function defined by
Multiplying the approximating equation by , we get
Following the same way as in [11], we obtain θ(un)⇀θ(u), weakly in for , strongly in L1(Q) and a.e in Q.
Step 2 (passage to the limit). Let set b(·, ∇u) = (M(|∇u|)/|∇u|2)∇u.
Let , one has
Step 3 (u ∈ BVloc (Q)). Let K be a compact in Q, and let φ ∈ D(Q) with K ⊂ supp (φ) such that
For all compact K ⊂ Q,
We recall that , and are bounded on R, (θ(un)) is bounded in , and (a(·, ∇θ(un))) is bounded in .
Using now the test function φ (defined below), we obtain, as for (3.14),