407 research outputs found
Blow-up problem for nonlinear nonlocal parabolic equation with absorption under nonlinear nonlocal boundary condition
In this paper we consider initial boundary value problem for nonlinear
nonlocal parabolic equation with absorption under nonlinear nonlocal boundary
condition and nonnegative initial datum. We prove comparison principle, global
existence and blow-up of solutions.Comment: arXiv admin note: text overlap with arXiv:1602.0501
On the lifespan of classical solutions to a non-local porous medium problem with nonlinear boundary conditions
In this paper we analyze the porous medium equation
\begin{equation}\label{ProblemAbstract} \tag{} %\begin{cases}
u_t=\Delta u^m + a\io u^p-b u^q -c\lvert\nabla\sqrt{u}\rvert^2 \quad
\textrm{in}\quad \Omega \times I,%\\ %u_\nu-g(u)=0 & \textrm{on}\; \partial
\Omega, t>0,\\ %u({\bf x},0)=u_0({\bf x})&{\bf x} \in \Omega,\\ %\end{cases}
\end{equation} where is a bounded and smooth domain of , with
, and is the maximal interval of existence for . The
constants are positive, proper real numbers larger than 1 and
the equation is complemented with nonlinear boundary conditions involving the
outward normal derivative of . Under some hypothesis on the data, including
intrinsic relations between and , and assuming that for some positive
and sufficiently regular function u_0(\nx) the Initial Boundary Value Problem
(IBVP) associated to \eqref{ProblemAbstract} possesses a positive classical
solution u=u(\nx,t) on : \begin{itemize} \item
[] when and in 2- and 3-dimensional domains, we determine
a \textit{lower bound of} for those becoming unbounded in
at such ; \item [] when and in
-dimensional settings, we establish a \textit{global existence criterion}
for . \end{itemize
Boundedness and homogeneous asymptotics for a fractional logistic Keller-Segel equations
In this paper we consider a -dimensional () parabolic-elliptic
Keller-Segel equation with a logistic forcing and a fractional diffusion of
order . We prove uniform in time boundedness of its solution
in the supercritical range , where is an explicit
constant depending on parameters of our problem. Furthermore, we establish
sufficient conditions for , where
is the only nontrivial homogeneous solution. Finally, we
provide a uniqueness result
Global solutions for a supercritical drift-diffusion equation
We study the global existence of solutions to a one-dimensional
drift-diffusion equation with logistic term, generalizing the classical
parabolic-elliptic Keller-Segel aggregation equation arising in mathematical
biology. In particular, we prove that there exists a global weak solution, if
the order of the fractional diffusion , where is
an explicit constant depending on the physical parameters present in the
problem (chemosensitivity and strength of logistic damping). Furthermore, in
the range with , the solution is globally
smooth. Let us emphasize that when , the diffusion is in the
supercritical regime
On Blow-up Solutions of A Parabolic System Coupled in Both Equations and Boundary Conditions
يهتم هذا البحث بالحلول المنفجرة لنظام يتكون من معادلتي انتشارو رد الفعل مقترنتين في كلا من المعادلات والشروط الحدودية. لغرض فهم كيفية تاثير مقاطع رد العفل والشروط الحدودية على خواص الانفجار، تم القيام باشتقاق القيد السفلي والعلوي للانفجار. علاوة على ذلك، تمت دراسة مجموعة النقاط المنفجرة تحت شروط محددة.This paper is concerned with the blow-up solutions of a system of two reaction-diffusion equations coupled in both equations and boundary conditions. In order to understand how the reaction terms and the boundary terms affect the blow-up properties, the lower and upper blow-up rate estimates are derived. Moreover, the blow-up set under some restricted assumptions is studied
Blow-up analysis in a quasilinear parabolic system coupled via nonlinear boundary flux
This paper deals with the blow-up of the solution for a system of evolution pLaplacian equations uit = div(|∇ui p−2∇ui) (i = 1, 2, . . . , k) with nonlinear boundary flux. Under certain conditions on the nonlinearities and data, it is shown that blow-up will occur at some finite time. Moreover, when blow-up does occur, we obtain the upper and lower bounds for the blow-up time. This paper generalizes the previous results
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