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1.
This paper deals with simultaneous and non-simultaneous blow-up for heat equations coupled via nonlinear boundary fluxes
\frac?u?h = um + vp, \frac?v?h = uq + vn\frac{\partial u}{\partial\eta} = u^{m} + v^{p}, \frac{\partial v}{\partial\eta} = u^{q} + v^{n}  相似文献   

2.
In this paper, we consider the multiple existence of nonradial positive solutions of coupled nonlinear Schr?dinger system
where μ1, μ2 > 0 with and β < 0. It is known that the solutions of (P) is not necessarily radial [12]. We show that problem (P) has multiple nonradial solutions in case that |β| is sufficiently small.   相似文献   

3.
Our first basic model is the fully nonlinear dual porous medium equation with source
for which we consider the Cauchy problem with given nonnegative bounded initial data u0. For the semilinear case m=1, the critical exponent was obtained by H. Fujita in 1966. For p ∈(1, p0] any nontrivial solution blows up in finite time, while for p > p0 there exist sufficiently small global solutions. During last thirty years such critical exponents were detected for many semilinear and quasilinear parabolic, hyperbolic and elliptic PDEs and inequalities. Most of efforts were devoted to equations with differential operators in divergent form, where classical techniques associated with weak solutions and integration by parts with a variety of test functions can be applied. Using this fully nonlinear equation, we propose and develop new approaches to calculating critical Fujita exponents in different functional settings. The second models with a “semi-divergent” diffusion operator is the thin film equation with source
for which the critical exponent is shown to be   相似文献   

4.
The paper deals with the radially symmetric solutions of ut=Δu+um(x,t)vn(0,t)ut=Δu+um(x,t)vn(0,t), vt=Δv+up(0,t)vq(x,t)vt=Δv+up(0,t)vq(x,t), subject to null Dirichlet boundary conditions. For the blow-up classical solutions, we propose the critical exponents for non-simultaneous blow-up by determining the complete and optimal classification for all the non-negative exponents: (i) There exist initial data such that uu (vv) blows up alone if and only if m>p+1m>p+1 (q>n+1q>n+1), which means that any blow-up is simultaneous if and only if m≤p+1mp+1, q≤n+1qn+1. (ii) Any blow-up is uu (vv) blowing up with vv (uu) remaining bounded if and only if m>p+1m>p+1, q≤n+1qn+1 (m≤p+1mp+1, q>n+1q>n+1). (iii) Both non-simultaneous and simultaneous blow-up may occur if and only if m>p+1m>p+1, q>n+1q>n+1. Moreover, we consider the blow-up rate and set estimates which were not obtained in the previously known work for the same model.  相似文献   

5.
This paper deals with the existence and stability properties of positive weak solutions to classes of nonlinear systems involving the (p,q)-Laplacian of the form
$ \left\{{ll} -\Delta_{p} u = \lambda \,a(x)\,v^{\alpha}-c, & x\in \Omega,\\ -\Delta_{q} v = \lambda \,b(x)\,u^{\beta}-c, & x\in \Omega,\\ u=0=v, & x\in\partial \Omega, \right. $ \left\{\begin{array}{ll} -\Delta_{p} u = \lambda \,a(x)\,v^{\alpha}-c, & x\in \Omega,\\ -\Delta_{q} v = \lambda \,b(x)\,u^{\beta}-c, & x\in \Omega,\\ u=0=v, & x\in\partial \Omega, \end{array}\right.  相似文献   

6.
We consider the 2-D Keller-Segel system (KS) for γ > 0. We first construct a mild solution of (KS) for every . The local existence time is characterized for with 1 < q * < 2. Next, we prove the finite time blow-up of strong solution under the assumption and , where g(s) is an increasing function of s > 1 with an explicit representation. As an application of our mild solutions, an exact blow-up rate near the maximal existence time is obtained.   相似文献   

7.
Intervals of the parameters λ and μ are determined for which there exist positive solutions to the system of dynamic equations $$ \begin{array}{lll} && (-1)^nu^{\Delta^{2n}}(t)+\lambda p(t)f(v(\sigma(t)))=0,\quad t\in[a, b], \\ &&(-1)^n v^{\Delta^{2n}}(t)+\mu q(t)g(u(\sigma(t)))=0, \quad t\in[a, b], \end{array} $$ satisfying the Sturm–Liouville boundary conditions $$ \begin{array}{lll} &&\alpha_{i+1} u^{\Delta^{2i}}(a)-\beta_{i+1} u^{\Delta^{2i+1}}(a)=0,\;\gamma_{i+1} u^{\Delta^{2i}}(\sigma(b))+\delta_{i+1} u^{\Delta^{2i+1}}(\sigma(b))=0,\\ &&\alpha_{i+1} v^{\Delta^{2i}}(a)-\beta_{i+1} v^{\Delta^{2i+1}}(a)=0,\; \gamma_{i+1} v^{\Delta^{2i}}(\sigma(b))+\delta_{i+1} v^{\Delta^{2i+1}}(\sigma(b))=0, \end{array} $$ for 0?≤?i?≤?n???1. To this end we apply a Guo–Krasnosel’skii fixed point theorem.  相似文献   

8.
We prove the existence of a unique solution of the following Neumann problem , u > 0, in (a, b) × (0, T), u(x, 0) = u 0(x) ≥ 0 in (a, b), and , where if m < 0, if m = 0, and m≤ 0, , and the case −1 < m ≤ 0, , for some constant p > 1 − m. We also obtain a similar result in higher dimensions. As a corollary we will give a new proof of a result of A. Rodriguez and J.L. Vazquez on the existence of infinitely many finite mass solutions of the above equation in for any −1 < m ≤ 0. We also obtain the exact decay rate of the solution at infinity.  相似文献   

9.
In this paper we deal with the following quasilinear parabolic problem $$\left\{\begin{array}{l@{\quad}l} (u^\theta)_t - \Delta_p {u} = \lambda \frac{u^{p - 1}}{|x|^{p}} + u^q + f,\,\, u \geq 0 \quad {\rm in} \;\;\Omega \times (0, T),\\ u(x, t) = 0 \quad\qquad\qquad\qquad\qquad\qquad\qquad {\rm on}\; \partial \Omega \times(0, T),\\ u(x, 0) = u_0(x), \,\,\, \qquad\qquad\qquad\qquad\qquad x \in\; \Omega,\end{array}\right.$$ where θ is either 1 or (p ? 1), \({N \geq 3, \,\Omega \subset \mathcal{IR}^N}\) is either a bounded regular domain containing the origin or \({\Omega \equiv \mathcal{IR}^N}\) , 1 < p < N, q > 0 and u 0 ≥  0, f ≥  0 with suitable hypotheses. The aim of this work is to get natural conditions to show the existence or the nonexistence of nonnegative solutions. In the case of nonexistence result, we analyze blow-up phenomena for approximated problems in connection with the classical Harnack inequality, in the Moser sense, more precisely in connection with a strong maximum principle. We also study when finite time extinction (1 < p < 2) and finite speed propagation (p > 2) occur related to the reaction power.  相似文献   

10.
We consider the following semilinear elliptic equation with singular nonlinearity:
where and Ω is an open subset in . Let u be a non-negative finite energy stationary solution and be the rupture set of u. We show that the Hausdorff dimension of Σ is less than or equal to [(n−2) α+(n+2)]/(α +1).  相似文献   

11.
The following regularity of weak solutions of a class of elliptic equations of the form are investigated.  相似文献   

12.
Approaching a vertex in a shrinking domain under a nonlinear flow   总被引:1,自引:0,他引:1  
We consider here the homogeneous Dirichlet problem for the equation , in a noncylindrical domain in space-time given by . By means of matched asymptotic expansion techniques we describe the asymptotics of the maximal solution approaching the vertex x=0, t=T, in the three different cases p>1/2, p=1/2(vertex regular), p<1/2 (vertex irregular).  相似文献   

13.
This paper concerns boundary value problems for quasilinear second order elliptic systems which are, for example, of the type
Here Ω is a Lipschitz domain in νj are the components of the unit outward normal vector field on ∂Ω, the sets Γβ are open in ∂Ω and their relative boundaries are Lipschitz hypersurfaces in ∂Ω. The coefficient functions are supposed to be bounded and measurable with respect to the space variable and smooth with respect to the unknown vector function u and to the control parameter λ. It is shown that, under natural conditions, such boundary value problems generate smooth Fredholm maps between appropriate Sobolev-Campanato spaces, that the weak solutions are H?lder continuous up to the boundary and that the Implicit Function Theorem and the Newton Iteration Procedure are applicable.  相似文献   

14.
In this paper we present a parabolic approach to studying the diffusive long time behaviour of solutions to the Cauchy problem:
(1)
where u0 and u1 satisfy suitable assumptions. After an appropriate scaling we obtain the convergence to a stationary solutio n in Lq norm (1 ≤  q  <  ∞).  相似文献   

15.
A solution u of a Cauchy problem for a semilinear heat equation
is said to undergo Type II blowup at tT if lim sup Let be the radially symmetric singular steady state. Suppose that is a radially symmetric function such that and (u 0) t change sign at most finitely many times. We determine the exact blowup rate of Type II blowup solution with initial data u 0 in the case of p > p L , where p L is the Lepin exponent.  相似文献   

16.
We study the radially symmetric Schr?dinger equation
with N ≥ 1, ɛ > 0 and p > 1. As ɛ→ 0, we prove the existence of positive radially symmetric solutions concentrating simultaneously on k spheres. The radii are localized near non-degenerate critical points of the function Supported by the Alexander von Humboldt foundation in Germany and NSFC (No:10571069) in China.  相似文献   

17.
Given (M,g) a smooth compact Riemannian manifold of dimension n ≥ 5, we consider equations like
where is a Paneitz-Branson type operator with constant coefficients α and aα, u is required to be positive, and is critical from the Sobolev viewpoint. We define the energy function Em as the infimum of over the u’s which are solutions of the above equation. We prove that Em (α ) →+∞ as α →+∞ . In particular, for any Λ > 0, there exists α0 > 0 such that for α ≥ α0, the above equation does not have a solution of energy less than or equal to Λ.  相似文献   

18.
We are concerned with the nonexistence of positive solutions of the nonlinear parabolic partial differential equations in a cylinder Ω × (0, T) with initial condition u(., 0) = u0(.) ? 0 and vanishing on the boundary ?Ω × (0, T), given by where $\Omega \in \mathbf {R}^NWe are concerned with the nonexistence of positive solutions of the nonlinear parabolic partial differential equations in a cylinder Ω × (0, T) with initial condition u(., 0) = u0(.) ? 0 and vanishing on the boundary ?Ω × (0, T), given by where $\Omega \in \mathbf {R}^N$ (resp. a Carnot Carathéodory metric ball in $\mathbf {R}^{2N+1})$ with smooth boundary and the time dependent singular potential function V(x, t) ∈ L1loc(Ω × (0, T)), $\alpha , \beta \in \mathbf {R}$, 1 < p < N, p ? 1 + α + β > 0. We find the best lower bounds for p + β and provide proofs for the nonexistence of positive solutions. © 2011 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim  相似文献   

19.
We prove that if q = p h , p a prime, do not exist sets U í AG(n,q){U {\subseteq} AG(n,q)}, with |U| = q k and 1 < k < n, determining N directions where
\fracqk - 1p - 1 < N £ \fracq+32 q k-1+ qk-2 +...+q2 + q \frac{{q^k} - 1}{p - 1} < N \le \frac{q+3}{2} q ^{k-1}+ q^{k-2} +\dots+q{^2} + q  相似文献   

20.
Let A 0, ... , A n−1 be operators on a separable complex Hilbert space , and let α0,..., α n−1 be positive real numbers such that 1. We prove that for every unitarily invariant norm,
for 2 ≤ p < ∞, and the reverse inequality holds for 0 < p ≤ 2. Moreover, we prove that if ω0,..., ω n−1 are the n roots of unity with ω j = e ij/n , 0 ≤ jn − 1, then for every unitarily invariant norm,
for 2 ≤ p < ∞, and the reverse inequalities hold for 0 < p ≤ 2. These inequalities, which involve n-tuples of operators, lead to natural generalizations and refinements of some of the classical Clarkson inequalities in the Schatten p-norms. Extensions of these inequalities to certain convex and concave functions, including the power functions, are olso optained.   相似文献   

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