非线性对流-扩散方程初边值问题的特征-差分解法

[1]讨论了线性方程c(x)((?u)/(?t))+b(x)(((?u)/(?x))-?/(?x))(a(x)(?u/?x))=f(x,t)初值问题的特征-有限元及特征-差分方法,[2]讨论了非线性方程 c(x)((?u)/(?t))+b(x,u)((?u)/(?x))-(?/(?x))(a(x,u)((?u)/(?x)))-f(x,u) (1.1)第一边值问题的特征-差分方法,并改善了[1]中某些重要结果。本文着重讨论非线性方程     

FINITE ELEMENT ANALYSIS OF A LOCAL EXPONENTIALLY FITTED SCHEME FOR TIME-DEPENDENTCONVECTION-DIFFUSION PROBLEMS

1.IntroductionConsiderthetime-dependentconvection-diffusionproblemat--Euzx a(x,t)u. b(x,t)u~f(x,t),(x,t)E[0,1]x[0,T](1.1)u(0,t)=u(1,t)~0,tE[0,T].(1.2)u(x,0)=u000,xE[0,1],(1.3)a(x,t)2or>0,(1.4)b(x,t)--a.(x,t)/220>0,(1.5)where0SE<<1'(1.1)-(1.5)canbereg...     

抛物型差分方程的符号稳定性

对于热传导方程的初边值问题 ut=(p(x)u_x)_x-q(x)u t>0 u(t,a)=u(t,b)=0(1.1) u(0,x)=u~0(x),polya [3]曾证明过,对于所有t>0,解u(i,x)在[a,b]上的变号次数不大于给定的初值函数u~0(k)在[a,b]上的变号次数.Nickel在[2]中讨论了更广泛的情况,得到了类似的更深入的结果.     

有限不变测度与一维扩散过程

<正> 本文沿用[2]或[3]中的记号. 对于微分算符Ω: Ωu=(a(x)u′)′+b(x)u′+c(x)u(1) a(x)>0,c(x)≤0,a(x),b(x)连续可微,c(x)连续以及它的形式共轭算符Ω: Ωv=(a(x)v′)′-(b(x)v)′+c(x)v(2)我们将说明:在c(x)0时Ω导出的满足局部边值条件的马氏过程P(t,x,Γ)(确切含义见[2]或[3]中定义4.5.1,4.5.4及4.5.5)不存在有限不变测度;在c(x)≡0时Ω导出的满足局部边值条件的马氏过程P(t,x,Γ)如果存在有限不变测度,则必是绝对连续的且其密度满足共轭方程.     

R~N空间中退化的logistic型拟线性椭圆方程正解存在唯一性

本文研究下列退化的logistic型p-Laplacian方程:-△Apu=a(x)|u|p-2u- b(x)|u|q-1u,x∈RN(N≥2)．在对系数a(x),b(x)在无穷远处的性质加以一般限制,得出了正解唯一存在性定理．我们的结果改进了文[1]和[2]中的相应结果．     

一类二阶四点边值问题正解的存在性

讨论二阶四点微分方程组边值问题u″+p(t)f(t,u(t),v(t))=0,0 t 1,v″+q(t)g(t,u(t),v(t))=0,0 t 1,u(0)=a1x(ξ1),u(1)=b1x(η1)v(0)=a2x(ξ2),v(1)=b2x(η2)如果函数f,g:[0,1]×[0,∞)×[0,∞)→[0,∞)是连续的,并赋予f、g一定的增长条件,利用Leggett-Williama不动点定理,证明了上述边值问题至少存在三对正解.     

求解奇异摄动转向点问题的高精度方法

1.引言 本文考察以下奇异摄动转向点问题: Lu≡ε~2u″+xa(x)u′-b(x)u=f(x),x∈I=[-1,1], u(-1)=A,u(1)=B, (1.1)其中参数ε是(0,1]中的常数,函数a(x)∈C~3[I],b(x),f(x)∈C~4[I]且满足a(x)≥a_*>0,b(x)≥b_*>0.在以上假设下,由[1]知,方程(1.1)存在唯一解u_8∈C~5[I]且     

关于拟线性抛物型方程b(u)u_t=[a(u)u_x]_x反问题拟解的存在性问题

本文在 [1 ]中“ut=[a(u) ux]x的一个反问题”的基础上 ,解决了 b(u) ut=[a(u) ux]x 反问题拟解的存在性问题     

关于非线性蜕化抛物型方程解的唯一性(英文)

本文证明,在条件a(s)>0(s>0),a(0)=0,b(s)=0(a(s)~λ)(s≥0,0≤λ≤1、2),s~μ=0(a(s))(a>0,μ>0)之下,混合问题 μ_t=(a(u)u_x)_x+b(u)u_x, (x, t)∈R={(x, t)|-11时,解为唯一的,这改善了[1,2]的结果。     

W_2~1(*)空间中二阶常微分边值问题的解析解

文[1]给出了W_2~1[a,b]中的再生核,[2]、[3] 、[4]在W_2~1[a,b]空间中,给出了最佳插值算子,最佳Hermite算子,第二类Fredholm积分方程解析解,但至今没有对常微分边值问题进行讨论。本文在W_2~1[a,b]空间的子空间W_2~1(*)中,讨论方程(1)的求解问题。利用W_2~1(*)空间的再生核构造方程(1)的解析解u(x),由解析解可直接得到数值解u(x),其误差随节点个数n的增加按空间范数单调下降,而且当n→∞时,能够保证u(x)一致收敛于u(x)。最后,我们给出了具体算例,所得数值结果,是很令人满意的。     

Degree of L~P Approximation by Operators of Kantorovi(?) Type Satisfying Micchelli Conditions

§1 We see symbols in article, L~∞[a,b]C[a,b], let f(t) be absolute continuous over [a,b], we denote by f∈AC[a,b], L_k~p[a,b]{f:f~(k-1)∈AC[a,b] and f~(k)(t)∈L~p[a,b]}.C_k[a,b]L_k~∞[a,b], W~kL{f:f∈L_k~p[a,b] and ‖f~(k)‖_p≤1}. Let H_n.be set of algebraic polynomials of degree≤n. Let B_n(F) be Bernstein polynomials,P_n(f) be Kantorovi polynomials. We generalize p_n(f). Let T be linear operator C[a,b]AC[a,b],for g(u)∈C[a,b] we have T(g(u),a)=g(a), T(g(u),b)=g(b), let f(t)∈L[a,b], F(u) =integral from n=0 to u(f(t)dt),     

On Applications of Vector Measure to the Optimal Control Theory for Distributed Parameter Systems

Let X and Z be two reflexive Banach spaces, U\in Z and b(\cdot,\cdot):[t_0,T]*U\rightarrow X continuous. Suppose $x(t)\equiv x(t,u(\cdot))$ is a function from [t_0, T] into X , satisfying the distrbnted parameter system $dx(t)\dt=A(t)x(t)+b(t,u(t)),t_0+\int_t_0^T {+r(t,u(t))dt}$. We have proved the following theorem. Theorem. Suppose u^*(\cdot) is the optimal control function, $x^*(t)=x(t,u^*(\cdot))$ and $\psi (t)=-U'(T,t)Q_1x^*(T)-\int_t^T{U'(\sigma,t)Q(\sigma)x^*(\sigma)d\sigma}$, then the maximum principle $<\psi(t),b(t,u^*(t))>-1/2r(t,u^*(t))=\mathop {\max }\limits_{u \in U} {\psi (t),b(t,u)>-1/2r(t,u)}$ (16) holds for almost all t on [t_0, T ].     

一类具有非局部扩散的时滞Lotka-Volterra竞争模型的行波解

本文研究一类具有非局部扩散的时滞Lotka-Volterra竞争模型{(δ)/(δ)t u1(x,t)=d1 [(J1*u1)(x,t)-u1(x,t)]+r1u1(x,t)[1 - a1u1(x,t)- b1u1(x,t-Τ1)-c1u2(x,t-Τ2)],(δ)/(δ)tu2(x,t)=d2[(J2*u2)(x,t)-u2(x,t)]+r2u2(x,t)[1 - a2u2(x,t)- b2u2(x,t -Τ3)-c2u1(x,t-Τ4)]行波解的存在性问题.通过利用交叉迭代技巧,我们可以把行波解的存在性转化为寻找一对适当的上下解,这篇文章中的结果推广了已有的一些结果.     

DECAY ESTIMATES OF PLANAR STATIONARY WAVES FOR DAMED WAVE EQUATIONS WITH NONLINEAR CONVECTION IN MULTI-DIMENSIONAL HALF SPACE

This paper is concerned with the initial-boundary value problem for damped wave equations with a nonlinear convection term in the multi-dimensional half space R n + : u tt u + u t + divf (u) = 0, t > 0, x = (x 1 , x ′ ) ∈ R n + := R + × R n 1 , u(0, x) = u 0 (x) → u + , as x 1 → + ∞ , u t (0, x) = u 1 (x), u(t, 0, x ′ ) = u b , x ′ = (x 2 , x 3 , ··· , x n ) ∈ R n 1 . (I) For the non-degenerate case f ′ 1 (u + ) < 0, it was shown in [10] that the above initialboundary value problem (I) admits a unique global solution u(t, x) which converges to the corresponding planar stationary wave φ(x 1 ) uniformly in x 1 ∈ R + as time tends to infinity provided that the initial perturbation and/or the strength of the stationary wave are sufficiently small. And in [10] Ueda, Nakamura, and Kawashima proved the algebraic decay estimates of the tangential derivatives of the solution u(t, x) for t → + ∞ by using the space-time weighted energy method initiated by Kawashima and Matsumura [5] and improved by Nishihkawa [7]. Moreover, by using the same weighted energy method, an additional algebraic convergence rate in the normal direction was obtained by assuming that the initial perturbation decays algebraically. We note, however, that the analysis in [10] relies heavily on the assumption that f ′ (u) < 0. The main purpose of this paper isdevoted to discussing the case of f ′ 1 (u b ) ≥ 0 and we show that similar results still hold for such a case. Our analysis is based on some delicate energy estimates.     

Asymptotic Error Expansion for the Nystrom Method of Nonlinear Volterra Integral Equation of the Second Kind

1.IntroductionConsiderthenonlinearVolterraintegraJequationofthesecondkindHere,u(x)isanunknownfunction,f(x)andK(x,t,u)aregivencontinuousfunctionsdefined,respectively,on[a,b1andD={(x,t,u):aSx5b,aSt5x)-oc相似文献   

定积分換元法則的一点改进

通常所见Riemann积分换元公式的形式是:若φ(α)=a,φ(β)=b,则在适当条件下有 integral from a to b(f(x)dx)=integral from α to β(f[φ(t)]φ′(t)dt)。在常义R(Riemann)积分时须假定:f(x)在[a,b]上连续,φ(t),φ′(t)在[α,β]上连续。这时上述等式成立。或者假定:f(x)在[a,b]上R可积,φ(t),φ′(t)在[α,β]上连续,且φ′(t)≥0(或φ′(t)≤0,即φ(t)单调)。本文证明了:若f(x)在[a,b]上有界,φ(t)可表成R可积函数φ(t)的不定积分,则f(x)在[a,b]上R可积的充要条件为f[φ(t)]φ(t)在[α,β]上R可积,并且有上述等式成立(详见下文定理1)。     

对“论广义的Канторович,Л.В.多项式及其渐近行为”一文的几点注记

在[1]中,曹家鼎讨论了用线性正算子逼近连续函数,给出一些函数类逼近上界的估计,该文中主要结果是 定理A 设A_n是一列C[a,b]C[a,b]的线性正算子,A_n(1,x)=1,则当x∈[a,b]时。 _n(w~2,x)=1/2A((t-x)~2,x), (1) 其中 如果再设A_n(t,x)=x,则     

On the Uniqueness Solutions of Nonlinear Degenerate Parabolic Equations (in English)

本文证明，在条件$a(s)>0(s>0),a(0)=0,b(s)=O(a(s)^\lambda)(s \geq 0,0 \leq \lambda \geq 1/2),s^\mu=O(a(s))(s \geq 0, \mu >0$之下，混合问题 ${u_t} = {(a(u){u_x})_x} + b(u){u_x},(x,t) \in R = \{ (x,t)| - 1 < x < 1,0 < t < T\} $ $u(x,0)=u_0(x)(\geq0),-1 \leqx \leq 1$ $u(-1,0)=\psi_1(t)(\geq0),u(1,t)=\psi _w(t)(\geq 0),0 \leq t \leq T$ 当$\mu<1,\lambda \geq0$或$\mu \geq1,2\lambda+1/ \mu>1$时，解为唯一的，这改善了[1,2]的结果。     

二阶哈密尔顿系统的对称扰动(英文)

我们研究二阶Hamiltonian系统-ü=▽F1(t,u)+ε▽F2(t,u)a.e.t∈[0,T]的多重周期解,其中ε是一个参数,T0.F1(F2)∶R×RN→R关于t是T周期的,▽F1(t,x)关于x是奇的;并且Fi(t,x)(i=1,2)对所有x∈RN关于t是可测的,对几乎所有t∈[0,T]关于x是连续可微的,而且存在a∈C(R+,R+),b∈L+(0,T;R+)使得|Fi(t,x)|≤a(|x|)b(t),|▽Fi(t,x)|≤a(|x|)b(t)对所有x∈RN及几乎所有t∈[0,T]成立.我们对F1施加适当的条件,能够证明对任意的j∈N存在εj0使得|ε|≤εj,则上述问题至少有j个不同的周期解.     

Existence and Global Asymptotic Behavior of Positive Solutions for Sublinear and Superlinear Fractional Boundary Value Problems

In this paper, the authors aim at proving two existence results of fractional differential boundary value problems of the form(P_(a,b)){D~αu(x) + f(x, u(x)) = 0, x ∈(0, 1),u(0) = u(1) = 0, D~(α-3)u(0) = a, u(1) =-b,where 3 α≤ 4, Dαis the standard Riemann-Liouville fractional derivative and a, b are nonnegative constants. First the authors suppose that f(x, t) =-p(x)t~σ, with σ∈(-1, 1)and p being a nonnegative continuous function that may be singular at x = 0 or x = 1and satisfies some conditions related to the Karamata regular variation theory. Combining sharp estimates on some potential functions and the Sch¨auder fixed point theorem, the authors prove the existence of a unique positive continuous solution to problem(P_(0,0)).Global estimates on such a solution are also obtained. To state the second existence result, the authors assume that a, b are nonnegative constants such that a + b 0 and f(x, t) = tφ(x, t), with φ(x, t) being a nonnegative continuous function in(0, 1)×[0, ∞) that is required to satisfy some suitable integrability condition. Using estimates on the Green's function and a perturbation argument, the authors prove the existence and uniqueness of a positive continuous solution u to problem(P_(a,b)), which behaves like the unique solution of the homogeneous problem corresponding to(P_(a,b)). Some examples are given to illustrate the existence results.