首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 31 毫秒
1.
We consider the boundary value problem
. Hereu ∈ ℝ2,D = diag{d 1,d 2},d 1,d 2 > 0, and the functionF is jointly smooth in (u, μ) and satisfies the following condition: for 0 <μ ≪ 1 the boundary value problem has a homogeneous (independent ofx) cycle bifurcating from a loop of the separatrix of a saddle. We establish conditions for stability and instability of this cycle and give a geometric interpretation of these conditions. Translated fromMatematicheskie Zametki, Vol. 63, No. 5, pp. 697–708, May, 1998. This research was supported by the Russian Foundation for Basic Research under grant No. 96-01-00207.  相似文献   

2.
We prove certain properties of solutions of the equation
in a domain ω ⊂R 3, which are similar to the properties of harmonic functions. By using the potential method, we investigate basic boundary-value problems for this equation. Lvov University, Lvov. Translated from Ukrainskii Matematicheskii Zhurnal, Vol. 51, No. 1, pp. 48–59, January, 1999.  相似文献   

3.
The paper is devoted to the study of the behavior of the following mixed problem for large values of time:
where Ω is an unbounded region of ℝ n with, generally speaking, noncompact boundary ; the surface Γ is star-shaped (relative to the origin), ν is the unit outer normal to ∂Ω; and the initial functionsf andg are assumed to be sufficiently smooth and finite. Under certain restrictions on the part of the boundary Γ2 constrained by the impedance condition, we establish that one can match the impedanceg≥0 (characterizing the absorption of energy by the surface Γ2) to the geometric properties of this surface so that the energy on an arbitrary compact set will decay at a rate characteristic for the first mixed problem. Translated fromMatematicheskie Zametki, Vol. 66, No. 3, pp. 393–400, September, 1999.  相似文献   

4.
The regular solutions of generalized axisymmetric potential equation , a>−1/2 are called generalized axisymmetric potentials. In this paper, the characterizations of lower order and lower type of entire GASP in terms of their approximation error {En} have been obtained.  相似文献   

5.
The paper deals with localization properties of solutions to the Cauchy problem with the initial data u0(x) ∈ L2(ℝn) for a wide class of equations in the divergence form. This class contains, e.g., the following equation:
, Restrictions are obtained, sharp in a sense, on the behavior of the function ensuring the instantaneous compactification of the support of an arbitrary energy solution to the problem as well as the compactification of the support after a finite waiting-time. Translated from Trudy Seminara imeni l. G. Petrovskogo, No. 20, pp. 121–154, 1997.  相似文献   

6.
This paper is devoted to studying the initial value problems of the nonlinear Kaup Kupershmidt equations δu/δt + α1 uδ^2u/δx^2 + βδ^3u/δx^3 + γδ^5u/δx^5 = 0, (x,t)∈ E R^2, and δu/δt + α2 δu/δx δ^2u/δx^2 + βδ^3u/δx^3 + γδ^5u/δx^5 = 0, (x, t) ∈R^2. Several important Strichartz type estimates for the fundamental solution of the corresponding linear problem are established. Then we apply such estimates to prove the local and global existence of solutions for the initial value problems of the nonlinear Kaup- Kupershmidt equations. The results show that a local solution exists if the initial function u0(x) ∈ H^s(R), and s ≥ 5/4 for the first equation and s≥301/108 for the second equation.  相似文献   

7.
For an equation of the form $$\begin{gathered} \frac{{\partial u}}{{\partial t}} - \sum\nolimits_{ij = 1}^n {{\text{ }}\alpha ^{ij} } \frac{{\partial ^2 u}}{{\partial x^i \partial x^j }} + \sum\nolimits_{ij = 1}^n {\beta _j^i x^i } \frac{{\partial u}}{{\partial x^i }} = 0, \hfill \\ {\text{ }}x \in R^n ,{\text{ }}t \in R^1 , \hfill \\ \end{gathered}$$ where α=(αij) is a constant nonnegative matrix andΒ=(Β i i ) is a constant matrix, subject to certain conditions, we construct a fundamental solution, similar in its structure to the fundamental solution of the heat conduction equation; we prove a mean value theorem and show that u(x0, t0) can be represented in the form of the mean value of u(x, t) with a nonnegative density over a level surface of the fundamental solution of the adjoint equation passing through the point (x0, t0); finally, we prove a parabolic maximum principle.  相似文献   

8.
This paper is devoted to studying the initial value problem of the modified nonlinear Kawahara equation the first partial dervative of u to t ,the second the third +α the second partial dervative of u to x ,the second the third +β the third partial dervative of u to x ,the second the thire +γ the fifth partial dervative of u to x = 0,(x,t)∈R^2.We first establish several Strichartz type estimates for the fundamental solution of the corresponding linear problem. Then we apply such estimates to prove local and global existence of solutions for the initial value problem of the modified nonlinear Karahara equation. The results show that a local solution exists if the initial function uo(x) ∈ H^s(R) with s ≥ 1/4, and a global solution exists if s ≥ 2.  相似文献   

9.
Résumé  Dans un célèbre papier ([3]), B. GIDAS et J.SPRUCK ont utilisé-sous des hypothèses adéquates- la technique du “blow up” pour montrer que les solutionsuC 0C 1 (Ω) du problème admettent une estimation a priori dansC 0 . Dans ce travail, on montre que, si les solutionsu sont juste supposéesC 0 , une telle estimation a priori n’existe plus. In a famous paper ([3]), B. GIDAS and J. SPRUCK used a “blow-up” argument to show that, under appropriate assumptions, all the solutionsuC 0C 1 (Ω) of the problem admit an a priori estimate inC 0 . In this work, we show that, if one supposes the solutions are only inC 0 , such an a priori estimate does not hold.  相似文献   

10.
We considerC 2-solutionsf=u+iv+jw of the system
calledH-solutions introduced by H. Leutwiler. Iff is anH-solution in ω, thenf | Ω∩ℂ is holomorphic. SinceH-solutions are real analytic, a non-zeroH-solution cannot vanish in an open subdomain of ℝ3. Our object is, by the way of examples, to show that there are many kinds of null-sets ofH-solutions in ℝ3. This is in sharp contrast to a holomorphic functionf in ℂ, where the setf −1 ({0}) consists of discrete points only unlessf≡0. This research is supported by the Academy of Finland  相似文献   

11.
Suppose a, b, and are reals witha<b and consider the following diffusion equation
  相似文献   

12.
In [2], [6], [7], methods are discussed for solving initial value problems
in certain scales of Banach spaces. The crucial point is to use suitable interior estimates for the complex valued functionu=u 0+iu 1. For holomorphic functionsu these estimates follow from Cauchy’s integral formula or from equivalent estimates for the harmonic partsu 0 andu 1. In this paper we consider the (linear) case for quaternionic-valued functionsu=u 0 e 0+u 1 e 1+u 1 e 2+u 3 e 3,u i=u i (t,x 0,x 1,x 2,x 3), by transferring the real-valued 4×4 system to an equivalent quaternionic equation and dealing with monogenic solutions. Finally we consider a special Dirac system for a certain non-monogenic case.  相似文献   

13.
A direct construction is given of a functionf(x1, x2) ∈ C°, such that the equation $$\frac{{\partial u}}{{\partial x_1 }} + ix_1^{2k - 1} \frac{{\partial u}}{{\partial x_2 }} = f$$ has no solution in any neighborhood of the origin; the functionf and all its derivatives vanish for x1=0.  相似文献   

14.
Explicit inversion formulas of Balakrishnan–Rubin type and a characterization of Bessel potentials associated with the Laplace–Bessel differential operator are obtained. As an auxiliary tool the B-metaharmonic semigroup is introduced and some of its properties are investigated.  相似文献   

15.
The results of dispersion analysis of the equation and relevant computer-assisted experiments are presented. The existence of solutions with sharpenings (collapses) and solutions of oscillatory type is discovered. Bibliography: 6 titles. Translated fromObchyslyuval’na ta Prykladna Matematyka, No. 76, 1992, pp. 13–18.  相似文献   

16.
In the first section of this article a new method for computing the densities of integrals of motion for the KdV equation is given. In the second section the variation with respect to q of the functional ∫ 0 π w (x,t,x,;q)dx (t is fixed) is computed, where W(x, t, s; q) is the Riemann function of the problem $$\begin{gathered} \frac{{\partial ^z u}}{{\partial x^2 }} - q(x)u = \frac{{\partial ^2 u}}{{\partial t^2 }} ( - \infty< x< \infty ), \hfill \\ u|_{t = 0} = f(x), \left. {\frac{{\partial u}}{{\partial t}}} \right|_{t = 0} = 0. \hfill \\ \end{gathered} $$   相似文献   

17.
At first Cauchy-problem for the equation: \(L[u(X,t)] \equiv \sum\limits_{i = 1}^n {\frac{{\partial ^2 u}}{{\partial x_1^2 }} + \frac{{2v}}{{\left| X \right|^2 }}} \sum\limits_{i = 1}^n {x_i \frac{{\partial u}}{{\partial x_i }} - \frac{{\partial u}}{{\partial t}} = 0} \) wheren≥1,v—an arbitrary constant,t>0,X=(x 1, …, xn)∈E n/{0}, |X|= =(x 1 2 +…+x n 2 )1/2, with 0 being a centre of coordinate system, is studied. Basing on the above, the solution of Cauchy-Nicolescu problem is given which consist in finding a solution of the equationL p [u (X, t)]=0, withp∈N subject the initial conditions \(\mathop {\lim }\limits_{t \to \infty } L^k [u(X,t)] = \varphi _k (X)\) ,k=0, 1,…,p?1 and ?k(X) are given functions.  相似文献   

18.
Sunto Si studia il problema della determinazione di una soluzione dell'equazione ak(x)∂ku/∂xk=f(x, y) entro la semistriscia a≤x≤b, y≥0, che assuma assegnati valori per y=0 e per x=a, x1, x2, b (a<x1<x2<b). Analogamente si studia il problema della determinazione di una soluzione dell' equazione ak(x)∂ku/∂xk+b(x)∂u/∂y=f(x,y), entro la medesima semistriscia, cha assuma assegnati valori per y=0 e per x=a, x1, x2, b e la cui ∂/∂y assuma assegnati valori per y=0. A Giovanni Sansone nel suo 70mo compleanno.  相似文献   

19.
It is proved that the Dirichlet problem is correct in the characteristic rectangle D ab = [0, a] × [0, b] for the linear hyperbolic equation
with the summable in D ab coefficients p 0, p 1, p 2, p 3 and q if and only if the corresponding homogeneous problem has only the trivial solution. The effective and optimal in some sense restrictions on p 0, p 1, p 2 and p 3 guaranteeing the correctness of the Dirichlet problem are established.  相似文献   

20.
In this paper we apply the method of potentials for studying the Dirichlet and Neumann boundary-value problems for a B-elliptic equation in the form
$ \Delta _{x'} u + B_{x_{p - 1} } u + x_p^{ - \alpha } \frac{\partial } {{\partial x_p }}\left( {x_p^\alpha \frac{{\partial u}} {{\partial x_p }}} \right) = 0 $ \Delta _{x'} u + B_{x_{p - 1} } u + x_p^{ - \alpha } \frac{\partial } {{\partial x_p }}\left( {x_p^\alpha \frac{{\partial u}} {{\partial x_p }}} \right) = 0   相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号