Second-order interface equations for nonlinear diffusion with very strong absorption

Citation
Va. Galaktionov et al., Second-order interface equations for nonlinear diffusion with very strong absorption, COMMUN C M, 1(1), 1999, pp. 51-64
Citations number
20
Categorie Soggetti
Mathematics
Journal title
COMMUNICATIONS IN CONTEMPORARY MATHEMATICS
ISSN journal
02191997 → ACNP
Volume
1
Issue
1
Year of publication
1999
Pages
51 - 64
Database
ISI
SICI code
0219-1997(199902)1:1<51:SIEFND>2.0.ZU;2-J
Abstract
We derive the interface equations for weak (or maximal) nonnegative solutio ns u(x, t) of the porous medium equation with strong absorption in one dime nsion u(t) = (u(m))xx - u(P), x is an element of R, t > 0. We consider here the very singular range where the exponents m > 1 and p < 1 satisfy 0 < m + p < 2. Unlike the range m + p greater than or equal to 2, where we have shown that the movement of the interface x = eta(t) is descr ibed by a first-order equation, we prove that in this case there is actuall y a system of two equations: (i) a universal law N-1(u(., t)) = a(0), where a(0) = a(0)(m,p) is a fixed constant and N-1(u) = (u((m-p)/2))(x) calculat ed at the interface (again a first-order operator), and (ii) a specific mov ement law, D(+)eta(t) = N-2(u(., t)), where N-2 is of the second order and D(+)eta(t) is the right-hand derivative. We establish the instantaneous smo othing effect and prove optimal gradient bounds on the solutions as well as the second-order estimate on the interface. The analysis is based on inter section comparison with the set of the travelling wave solutions. The resul ts apply to the linear diffusion m = 1 with p is an element of (-1, 1) and for fast diffusion, m is an element of (0, 1), when p is an element of (-m, m). They can be also applied to equations of diffusion-convection type.