传输扩散方程周期解问题的Petrov-Galerkin方法的稳定性

本文以下列简单问题为例,讨论Petrov-Galerkin方法的稳定性:?U/?t q?U/x=ε~2U/x~2,-∞0,U(x, t)=U(x 1.t), -∞相似文献   

关于双曲型偏微分方程u_xy=f(x,y,u,u_x,u_y)的唯一性问题

关于双曲型偏微分方程 u_(xy)=f(x,y,u,u_x,u_y),0≤x≤a,0≤y≤b,-∞相似文献   

半线性抛物型方程的双移动边界问题

本文运用Fourier方法和压缩映像不动点原理,证明了半线性抛物型方程的双移动边界问题 u_t=a~2u_(xx) F(x,t,u,u_x),(x,t)∈D_∞, u(l_1(t),t)=0,l_1(0)=0,t∈(0, ∞), u(l_2(t),t)=0,l_2(0)=l_0,t∈(0, ∞), u(x,0)=φ(x),0≤x≤l_0,φ(0)=φ(l_0)=0.解的存在唯一性,其中D_∞={(x,t)|l_1(t)相似文献   

On the Necessary and Sufficient Condition of Existence of Solution to Cauchy problem of a Class of Degenerate Equation

In this paper, we discuss the existence of the solution to the Cauchy problem: L_p~ku≡u_(xx)-x~(2k)u_(tt) Px~(k-1)u_t=f(x,t),t≥0, (1) (A_k) u(x,0)=ψ_1(x), u_t(x,0)=ψ_2(x), (2)where κ=2i 1, i=0,1,2,…,P R=(-∞, ∞), ψ_1(x),ψ_2(x)∈C~∞(R), f(x,t) ∈C~∞(R_2~ ),R_2~ ={(x, t)∈R~2|t≥0}.If κ=1, the uniqueness and existence of solution to the Cauchy problem(A_κ) was entirely solved by [1-3], if κ>1, A. Menikoff proved that the C~∞     

铁磁链方程组的两个差分格式

考虑下面的铁磁链方程组: z_t=z×z_(xx)+z×h,(1)其边界条件为 z(0,t)=z(1,t)=0,(2)初始条件为 z(x,0)=φ(x),(3)这里z=(u,v,w),h=(h_1(x,t),h_2(x,t),h_3(x,t))是定义在区域Q{0≤x≤1,     

一类非线性抛物方程的反问题

本文讨论了下述反问题 u_1-△u=β(t)f(u) γ(x,t),x∈Ω,0相似文献   

Glimm方法对于燃烧模型组的收敛性

本文对于反应速率无穷的燃烧模型组的初值问题证明了Glimm方法的收敛性,其中f′(u)>0,f″(u)≥δ>0(u≥0),常数q>O以及当u_0(x)>0时z_0(x)=0。     

含爆轰波的间断解的渐近性

<正> 在[1]中我们研究了如下的初值问题:/t(u+qz)+/zf(u)=υ ~2u/x~2,(1)z/t=-kφ(u)z,(2)u(x,0)=u_0(x),z(x,0)=z_0(x)(3)当υ=+0,K=+∞时的弱解.其中常数q>0,υ,K,q分别代表了粘性系数、化学反应速率和束缚能,u是一个综合变量,它代表了密度、速度和温度,z是未燃气体的     

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。     

一类非线性Schr dinger方程的高精度守恒数值格式

1引言本文讨论下面非线性Schr(?)dinger方程(NLS)方程的初边值问题:i(?)u/(?)t (?)~2u/(?)x~2 2|u~2|u=0,(1) u(x_l,t)=u(x_r,t)=0,t>0,(2) u(x,0)=u_0(x),x_l≤x≤x_r,(3)其中u(x,t)是复值函数,u_0(x)为已知的复值函数,i~2=-1.该问题有着如下的电荷与能量守恒关系:     

线性微分追捕对策

本文研究线性微分对策的追捕问题,给出一些结束追捕的条件.我们研究方程(?)=C_z-u+v(1)描述的线性微分对策,其中 z∈R~n,C 是 n×n 常阵,u∈P,v∈Q.控制域 P 和 Q 是 n维欧氏空间 R~(?)中的紧凸集合.作为时间的函数 u=u(t),v=v(t)对 t 是可测的.设 M 是 R~n 中的全维数闭凸集合.定义 给定 z_0∈R~n,如果对于任意的可测函数 v(t)∈Q,t≥0,都可以构造出一个可测函数 u(t)∈P,t≥0,使得方程(?)(t)=Cz(t)-u(t)+v(t),z(0)=z_0的解 z(t),t≥0,在不超过数τ的时间内落到集合 M 上:z(t|ˉ)∈M,(t|ˉ)∈[0,τ],则称     

具粘性拟线性波方程的能量衰减估计

给出下列具粘性拟线性波方程初边值问题解的能量衰减估计u_(tt)(t,x)-div{σ(|▽u(t,x)|~2)▽u(t,x)}-△u(t,x)-△ut(t,x)+δ|u_t(t,x)|~(p-1)u_t(t,x)=μ|u(t,x)|~(q-1)u(t,x),x∈Ω,t∈(0,T),u(t,x)|■Ω=0,t∈(0,T),u(0,x)=u_0(x),u_t(0,x)=u_1(x),x∈Ω,其中Ω是R~N(N≥1)中具有光滑边界■Ω的区域,p≥1,q1,δ0,μ0,△表示Laplace算子,▽表示梯度算子和σ(s)是一给定的非线性函数.证明的思想是应用一已知的积分不等式,证明以上初边值问题解的能量衰减估计.     

高阶广义 Korteweg-de Vries 型方程组的周期边界问题与初值问题

<正> §1.引言近年来有很多作者从物理学的角度研究了所谓 Korteweg-de Vries 方程或简称为 KdV方程u_(?)+αuu_x+βu_(xxx)=0 (1)的解的性质.也有不少工作从数学的角度讨论这类方程及其推广的问题的提法.在[8—9]中提出了更广泛的一类高阶 KdV 方程.在[10]中研究了形式为z_t+α(|z|~2z)_x+z_(xxx)=0 (2)的复函数 z(x,t)=u(x,t)+iv(x,t)的复 KdV 方程的问题.复函数方程(2)可以写成实函数 u(x,t)与 v(x,t)所满足的方程组u_t+α((u~2+v~2)u)_x+u_(xxx)=0,v_t+α((u~2+v~2)v)_x+v_(xxx)=0 (3)的形式.     

亚纯函数的级的估计

设f(z)为一亚纯函数,其级p< ∞。re~(iω_1),re~(iω_2),…,re~(iω_q)(r≥0)为q条射线,其中0≤ω_1<ω_2<…<ω_q<2π,q≥1。本文证明了若方程:f(z)=0,f(z)=∞,f~((l))(z)=1(l≥0,f~((0))≡f)的根均分布在包含上述q条射线的q个窄形区域中,又δ(0,f) δ(∞,f) δ(1,f~((l))>0,则     

具有阻尼的半线性波动方程解的衰减估计

研究具有阻尼的半线性波动方程的初边值问题u_(tt)-△u+βu_t=|u|~(p-1)u,x∈Ω,t>0u(x,0)=u_0(x),u_t(x,0)=u_1(x),x∈Ωu|_((?)Ω)=0,t≥0其中γ为正常数,Ω■R~n为有界域,当n≥3时,1相似文献   

非线性梁振动方程的周期解

一、引言考虑下述问题Ku″ A~2u M(‖A~1/2u‖~2)Au Au′=f(x,t),t>0,x∈Ω,(1.1)u|_t=0~=u_0(x),x∈Ω,(1.2)Ku′|_(t=0)=u_1(x),x∈Ω,(1.3)u=0,x∈(?)Ω,t≥0 (1.4)的ω-周期解的存在性.其中 Ω(?)R~n 为一有界光滑区域,u′=((?)u)/((?)t),u_″=((?)u)/((?)t)~2,K 为有界线性对称算子且满足(Ku,u)≥0,M∈C~1[0,∞),M(ξ)≥-β,ξ≥0.此模型最初由Woinowsky 和 Krieger 提出,方程形式为     

On a system of second order differential equations with periodic impulse coefficients

A thorough investigation of the systemd~2y(x):dx~2 p(x)y(x)=0with periodic impulse coefficientsp(x)={1,0≤xx_0>0) -η, x_0≤x<2π(η>0)p(x)=p(x 2π),-∞相似文献   

SP权对的分解

如权对(u,v)∈S_p(10,f~*(x)是 f 的 Hardy-Littlewood 极大函数。     

变系数Euler-Bernoulli梁振动发展系统的存在性

讨论变系数Euler-Bernoulli梁振动系统{uu(x,t) η(t)uxxxx(x,t)=0,0＜x＜1,0≤t≤T u(0,t)=ux(0,t)=0,0≤t≤t -uxxx(1,t) muu(1,t)=-αu1(1,t) βuxxx(1,t),0≤t≤T uxt(1,t) =-γuxx(1,t),0≤t≤t u(x,0)=u1(x),u1(x,0),0≤x≤1证明了该系统产生一个发展系统．     

Oblique derivative problem for general Chaplygin-Rassias equations

The present paper deals with the oblique derivative problem for general second order equations of mixed (elliptic-hyperbolic) type with the nonsmooth parabolic degenerate line K_1(y)u_(xx) |K_2(x)|u_(yy) a(x,y)u_x b(x, y)u_y c(x,y)u=-d(x,y) in any plane domain D with the boundary D=Γ∪L_1∪L_2∪L_3∪L_4, whereΓ(■{y>0})∈C_μ~2 (0<μ<1) is a curve with the end points z=-1,1. L_1, L_2, L_3, L_4 are four characteristics with the slopes -H_2(x)/H_1(y), H_2(x)/H_1(y),-H_2(x)/H_1(y), H_2(x)/H_1(y)(H_1(y)=|k_1(y)|~(1/2), H_2(x)=|K_2(x)|~(1/2) in {y<0}) passing through the points z=x iy=-1,0,0,1 respectively. And the boundary condition possesses the form 1/2 u/v=1/H(x,y)Re[λuz]=r(z), z∈Γ∪L_1∪L_4, Im[λ(z)uz]|_(z=z_l)=b_l, l=1,2, u(-1)=b_0, u(1)=b_3, in which z_1, z_2 are the intersection points of L_1, L_2, L_3, L_4 respectively. The above equations can be called the general Chaplygin-Rassias equations, which include the Chaplygin-Rassias equations K_1(y)(M_2(x)u_x)_x M_1(x)(K_2(y)u_y)_y r(x,y)u=f(x,y), in D as their special case. The above boundary value problem includes the Tricomi problem of the Chaplygin equation: K(y)u_(xx) u_(yy)=0 with the boundary condition u(z)=φ(z) onΓ∪L_1∪L_4 as a special case. Firstly some estimates and the existence of solutions of the corresponding boundary value problems for the degenerate elliptic and hyperbolic equations of second order are discussed. Secondly, the solvability of the Tricomi problem, the oblique derivative problem and Frankl problem for the general Chaplygin- Rassias equations are proved. The used method in this paper is different from those in other papers, because the new notations W(z)=W(x iy)=u_z=[H_1(y)u_x-iH_2(x)u_y]/2 in the elliptic domain and W(z)=W(x jy)=u_z=[H_1(y)u_x-jH_2(x)u_y]/2 in the hyperbolic domain are introduced for the first time, such that the second order equations of mixed type can be reduced to the mixed complex equations of first order with singular coefficients. And thirdly, the advantage of complex analytic method is used, otherwise the complex analytic method cannot be applied.