290 research outputs found
Sign changing solutions of Lane Emden problems with interior nodal line and semilinear heat equations
We consider the semilinear Lane Emden problem in a smooth bounded simply
connected domain in the plane, invariant by the action of a finite symmetry
group G. We show that if the orbit of each point in the domain, under the
action of the group G, has cardinality greater than or equal to four then, for
p sufficiently large, there exists a sign changing solution of the problem with
two nodal regions whose nodal line does not touch the boundary of the domain.
This result is proved as a consequence of an analogous result for the
associated parabolic problem
Asymptotic profile of positive solutions of Lane-Emden problems in dimension two
We consider families of solutions to the problem
\begin{equation}\label{problemAbstract} \left\{\begin{array}{lr}-\Delta u= u^p
& \mbox{ in }\Omega\\ u>0 & \mbox{ in }\Omega\\ u=0 & \mbox{ on }\partial
\Omega \end{array}\right.\tag{} \end{equation} where and
is a smooth bounded domain of . We give a complete
description of the asymptotic behavior of as ,
under the condition \[p\int_{\Omega} |\nabla u_p|^2\,dx\rightarrow
\beta\in\mathbb R\qquad\mbox{ as }.\
Exact Morse index computation for nodal radial solutions of Lane-Emden problems
We consider the semilinear Lane-Emden problem
\begin{equation}\label{problemAbstract} \left\{\begin{array}{lr}-\Delta u=
|u|^{p-1}u\qquad \mbox{ in }B u=0\qquad\qquad\qquad\mbox{ on }\partial B
\end{array}\right.\tag{} \end{equation} where is the unit
ball of , , centered at the origin and , with
if and if . Our main result
is to prove that in dimension the Morse index of the least energy
sign-changing radial solution of \eqref{problemAbstract} is exactly
if is sufficiently large. As an intermediate step we compute explicitly the
first eigenvalue of a limit weighted problem in in any dimension
Asymptotic analysis and sign changing bubble towers for Lane-Emden problems
We consider the semilinear Lane-Emden problem in a smooth bounded domain of
the plane. The aim of the paper is to analyze the asymptotic behavior of sign
changing solutions as the exponent p of the nonlinearity goes to infinity.
Among other results we show, under some symmetry assumptions on the domain,
that the positive and negative parts of a family of symmetric solutions
concentrate at the same point, as p goes to infinity, and the limit profile
looks like a tower of two bubbles given by a superposition of a regular and a
singular solution of the Liouville problem in the plane
Aggregates relaxation in a jamming colloidal suspension after shear cessation
The reversible aggregates formation in a shear thickening, concentrated
colloidal suspension is investigated through speckle visibility spectroscopy, a
dynamic light scattering technique recently introduced [P.K. Dixon and D.J.
Durian, Phys. Rev. Lett. 90, 184302 (2003)]. Formation of particles aggregates
is observed in the jamming regime, and their relaxation after shear cessation
is monitored as a function of the applied shear stress. The aggregates
relaxation time increases when a larger stress is applied. Several phenomena
have been proposed to interpret this behavior: an increase of the aggregates
size and volume fraction, or a closer packing of the particles in the
aggregates.Comment: 7 pages, 7 figures; added figures included in the pdf versio
Blow up of solutions of semilinear heat equations in non radial domains of
We consider the semilinear heat equation
\begin{equation}\label{problemAbstract}\left\{\begin{array}{ll}v_t-\Delta v=
|v|^{p-1}v & \mbox{in}\Omega\times (0,T)\\ v=0 & \mbox{on}\partial \Omega\times
(0,T)\\ v(0)=v_0 & \mbox{in}\Omega \end{array}\right.\tag{}
\end{equation} where , is a smooth bounded domain of , and belongs to a suitable space. We give general
conditions for a family of sign-changing stationary solutions of
\eqref{problemAbstract}, under which the solution of \eqref{problemAbstract}
with initial value blows up in finite time if
is sufficiently small and is sufficiently large. Since for the
solution is global, this shows that, in general, the set of the initial
conditions for which the solution is global is not star-shaped with respect to
the origin. In previous paper by Dickstein, Pacella and Sciunzi this phenomenon
has already been observed in the case when the domain is a ball and the sign
changing stationary solution is radially symmetric. Our conditions are more
general and we provide examples of stationary solutions which are not
radial and exhibit the same behavior
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