三维可压核废料污染问题的交替方向特征有限元格式的敛速分析

1　引　　言三维可压核废料污染问题的数学模型为[1 ] :(a)　φ1 p t+ .u =-q +R′s(c)(b)　φ c t+u . c- .(Ec c) =g(c)(c)　φKi ci t+u . ci - .(Ec ci) +d3(ci) p t=fi(c,c1 ,c2 ,… ,c Nc) ,(i =1 ,… ,Nc)(d)　 d2 T t+cpu . T - .(EH T) +d1 (p) p t=Q(u,T,c,p) (1 .1 )其中 :u=-a(c) p=-k(x)μ(c) p.(x,t)∈Ω×J,Ω=I×I×I,I=(0 ,1 ) ,J=(0 ,T] .假设问题 (1 .1 )满足周期边界条件 ,p(x,t) .c(x,t) .ci(x,t) .T(x,t)的初始条件分别取为 p0 (x) ,c0 (x) ,c0i(x) ,T0 (x) ,(i=1 ,… ,Nc) .假设 (1 .1 )的系数可关…     

INJECTIVE MAPS ON PRIMITIVE SEQUENCES OVER Z/（p^e）

Let Z/(pe) be the integer residue ring modulo pe with p an odd prime and integer e ≥ 3. For a sequence (a) over Z/(pe), there is a unique p-adic decomposition (a) = (a)0 (a)1·p … (a)e-1 ·pe-1, where each (a)i can be regarded as a sequence over Z/(p), 0 ≤ i ≤ e - 1. Let f(x) be a primitive polynomial over Z/(pe) and G' (f(x), pe) the set of all primitive sequences generated by f(x) over Z/(pe). For μ(x) ∈ Z/(p)[x] with deg(μ(x)) ≥ 2 and gcd(1 deg(μ(x)),p- 1) = 1,set ψe-1 (x0, x1,…, xe-1) = xe-1·[ μ(xe-2) ηe-3 (x0, x1,…, xe-3)] ηe-2 (x0, x1,…, xe-2),which is a function of e variables over Z/(p). Then the compressing map ψe-1: G'(f(x),pe) → (Z/(p))∞,(a) (→)ψe-1((a)0, (a)1,… ,(a)e-1) is injective. That is, for (a), (b) ∈ G' (f(x), pe), (a) = (b) if and only if ψe - 1 ((a)0, (a)1,… , (a)e - 1) =ψe - 1 ((b)0,(b)1,… ,(b)e-1). As for the case of e = 2, similar result is also given. Furthermore, if functions ψe-1 and ψe-1 over Z/(p) are both of the above form and satisfy ψe-1((a)0,(a)1,… ,(a)e-1) = ψe-1((b)0,(b)1,… ,(b)e-1) for (a),(b) ∈ G'(f(x),pe), the relations between (a) and (b), ψe-1 and ψe-1 are discussed.     

不定常耦合型偏微分方程组非协调元方法的稳定性和收敛性

(1)a_(ij)~(k)(x)充分光滑,A~(k)(x)对x∈Ω为一致正定、有界的对称矩阵。 (2)对(x,p)∈Ω×R~2,D_1(x,p),一致有界且关于p满足Lipschitz条件。对(x,t,p)∈Ω×[0,T]×R~2,F(x,t,p)对P满足Lipschitz条件,F(x,t,0)∈L~∞([0,T];L~2(Ω)×L~2(Ω))。     

关于一类二阶非线性双曲型方程全离散有限元方法的稳定性和收敛性估计

1　引　　言考虑如下混合问题 :φ( x,u) utt- di,j=1 xi( aij( x,u) u xj) - di=1bi( x,u) uxi =f( x,u)　　　　　　　　　　　　　　　 ( x,t)∈Ω× [0 ,T]u( x,0 ) =0 ,　 ut( x,0 ) =0　　 x∈Ωu( x,t) =0　 ( x,t)∈ Ω× [0 ,T]( 1 .1 )这里 utt= 2 u t2 ,uxi= u xi;Ω是 Rd 中充分光滑的有界开域 ,边界 Ω光滑 .对于 φ( x,u)中仅含有 x,或 φ( x,u)≡ 1的线性或非线性双曲型方程的半离散或全离散有限元方法的研究已有 [1 ] -[4 ] .这些文献定义了线性[1 ] [4] 或非线性[2 ] 或预测—校正[4] 全离散有限元格式 ,然后将原方…     

Boltzmann-Poisson方程组初边值问题的整体弱解

§ 1.　Introduction　　LetΩ R3beasmoothboundedopenset,f(t,x ,v)bethedistributionfunctionofcar riersattimet >0 ,positionvectorx∈Ωandvelocityvectorv∈R3.Theforcefieldactingonthecarriersisdenotedbythe3 dimensionalvectorfunctionE(t,x) ,thepotentialcorespondingtoE(t,x)isdenotedbyu(t,x) ,then (f,E)satisfythefollowingBoltzmann Poissonsystem tf +v· xf +E· vf =Q(f) ,　 (t,x ,v)∈R+ ×Ω×R3,(1 .1 )E =- xu ,-Δxu =ρ ,　 (t,x) ∈R+ ×Ω ,(1 .2 )whereρ(t,x) =∫R3 f(t,x ,v)dvisthecarriernum…     

THE FINITE ELEMENT METHODS FOR A CLASS OF NONLINEAR PARABOLIC EQUATIONS

1　IntroductionConsider the nonlinear parabolic initial-boundary problem:φ( x,u) ut- di,j=1 xj( aij( x,u) u xi) - di=1bi( x,u) uxi =f ( x,u)　　　　 ( x,t)∈Ω× ( 0 ,T]u( x,0 ) =u0 ( x)　　 x∈Ωu( x,t) =0　　 ( x,t)∈ Ω× ( 0 ,T]( 1 .1 )where ut= u t,uxi= u xi.Ω is a bounded domain in Rd with a smooth boundary Ω.Supposeφ( x,u) =1 ,bi( x,u) =0 in( 1 .1 ) ,Douglas and Dupont[1 ] formulated severalGalerkin procedures in 1 970 called Crank-Nicolson-Galerkin approximation,predictor-co…     

一类随机微分方程的解法

设(Ω,,p)是一个完备的概率空间,(_t)_(t≤T)是的非降子σ代数族,W=(W_t,_t),t≤T 是 Wiener 过程。a(t,x),b(t,x)均是关于[0,T]×R 可测函数,并且假定 a(t,ξ_t)∈L_W~1[0,T],b(t,ξ_t)∈L_W~2[0,T](参考[5])。称 p—a.s 连续的随机过程ξ=(ξ_t,_t),t≤T 为随机微分方程     

两相不定常连续铸钢问题有限元逼近的收敛性分析

记Ω=(0,1)×(0.τ)为钢锭区域,Ω_τ=(0,T)×Ω,Ω_τ=Ω_1(t)∪Ω_2(t),t∈(0,T),其中Ω_1(t)与Ω_2(t)分别表示液态与固态区域。时刻t时的自由界面由F(t)={(x,z)∈Ω,s(X,Z,t)=0}表示,F=(?)F(t)。 设u=u(X,Z,t)表示温度。作变换后不妨设Ω,(t)上     

一类拟线性退化抛物方程Dirichlet问题粘性解的正则性

本文考虑下面的Dirichlet问题ut一Tr[a(x,t)D2u]+H(x,t,u,Du)=0,(x,t)∈QT=Ω×(0,T),u(x,t)=ψ(x,t), (x,t)∈ГT. (DP)利用粘性解理论证明了当H,Г满足一定条件时,(DP)的粘性解u(x,t)满足如果ψ∈Ca2,则u(x,t)∈Cα,羞;若ψ=0,则u(x,t)是Lpschitz连续的.     

线性抛物型积分微分方程的扩展混合体积元方法

1 引言 考虑线性抛物型积分微分方程初边值问题: {pt(x,t)-▽.{A(x,t)▽p(x,t) +∫t0 B(x,t,τ)▽p(x,τ)dτ}=f(x,t),(x,t)∈Ω×(0,T],(1.1) p(x,0):p0(x), x∈Ω, p(x,t)=0, (x,t)∈(a)Ω×(0,T]. 这里x=(x,y),Ω=(a,b)×(c,d),(e)Ω是区域Ω的边界,p为未知函数,A=(aij)2×2为已知的对称正定矩阵,B=(bij)2×2为已知矩阵,而且aij,bij,(aij)t(i,j=1,2)光滑有界,f∈L2(Ω).     

三维热传导型半导体问题的特征有限元方法和分析

本文研究三维热传导型半导体瞬态问题的特征有限元方法及其理论分析,其数学模型是一类非线性偏微分方程的初边值问题,对电子位势方程提出Ｇａｌｅｒｋｉｎ逼近;对电子,空穴浓度方程采用特征有限元逼近;对热传导方程采用对时间向后差分的Ｇａｌｅｒｋｉｎ逼近．应用微分方程先验估计理论和技巧得到了最优阶Ｌ＾２误差估计。     

裂缝-孔隙介质中地下水污染问题的Galerkin交替方向有限元方法

考虑裂缝 孔隙介质中地下水污染问题均匀化模型的数值模拟．对压力方程采用混合元方法,对浓度方程采用Ｇａｌｅｒｋｉｎ交替方向有限元方法,对吸附浓度方程采用标准Ｇａｌｅｒｋｉｎ方法,证明了交替方向有限元格式具有最优犔２ 和犎１ 模误差估计．     

High accuracy A.D.I. methods for parabolic equations with variable coefficients

Summary High accuracy alternating direction implicit (A.D.I.) methods are derived for solving the heat conduction equation with variable coefficients in two and three space dimensions. These methods are shown to be unconditionally stable.     

Intermediate boundary corrections for split operator methods in three dimensions

This paper deals with the intermediate boundary corrections required by splittings of alternating direction methods for solving three space dimensional problems involving Laplace's equation or the heat conduction equation. In addition to considering the existing splittings of Douglas and D'Yakonov, a new splitting is introduced. The extensions of the results to multidimensional problems are briefly noted.     

半导体问题的交替方向有限元方法

该文用交替方向有限元方法求解半导体问题的Energy Trans port (ET)模型。对模型中椭圆型的电子位势方程采用交替方向迭代法，对流占优扩散的电子浓度和空穴浓度方程采用特征交替方向有限元方法，热传导方程利用Patch逼近采用交替方向有限元方法求解。利用微分方程的先验估计理论和技巧，分别得到了椭圆型方程和抛物型方程的最优H+1和L+2误差估计。     

三维热传导型半导体问题的交替方向特征有限元方法及理论分析

１．引言 三维热传导型半导体器件瞬态问题的数学模型由四个非线性偏微分方程描述 ［１,２］．工程研究中一般考虑绝流边条件,由于绝流条件可以看作一反射条件来处理、为了数值分析方便,我们在此考虑三维周期问题： 其中,　＝［０,１］３,未知函数是电子位势　;电子,空穴浓度ｅ,ｐ;温度函数Ｔ．方程（１,１）－（１.４）中出现的系数均有正的上下界,且是　周期的． ａ＝Ｑ／ε,Ｑ,ε分别表示电子负荷和介电系数,均为正常数．Ｎ（ｘ）是给定的函数．Ｄｓ（ｘ）为扩散系数,μｓ（ｘ）为迁移率,ｓ＝ｅ,Ｐ．Ｒ（ｅ,ｐ,Ｔ）…     

Long- time Convergence of Numerical Approximations for Semilinear Parabolic Equations(Ⅰ )

§ 0 .Introduction　 We consider the numerical approximations of the dynamical systems governed bysemilinear parabolic equations,which are discretized by Galerkin and nonlinear Galerkinmethods in space,and by Runge-Kutta method in time.The numerical approximationson a finite time interval have already been widely studied(see[1 ]— [5] ) .We areconcerned with the long-time convergence and error estimates.This article is composedof three parts. In part ,we provide an abstract framework. In§…     

Inverse determination of thermal conductivity using semi-discretization method

In this work a semi-discretization method is presented for the inverse determination of spatially- and temperature-dependent thermal conductivity in a one-dimensional heat conduction domain without internal temperature measurements. The temperature distribution is approximated as a polynomial function of position using boundary data. The derivatives of temperature in the differential heat conduction equation are taken derivative of the approximated temperature function, and the derivative of thermal conductivity is obtained by finite difference technique. The heat conduction equation is then converted into a system of discretized linear equations. The unknown thermal conductivity is estimated by directly solving the linear equations. The numerical procedures do not require prior information of functional form of thermal conductivity. The close agreement between estimated results and exact solutions of the illustrated examples shows the applicability of the proposed method in estimating spatially- and temperature-dependent thermal conductivity in inverse heat conduction problem.     

三维非线性抛物型积分-微分方程的A.D.I.Galerkin方法及其分析

研究三维非线性抛物型积分-微分方程的A.D.I.Galerkin方法.通过交替方向,化三维为一维,简化计算;通过Galerkin法,保持高精度.成功处理了Volterra项的影响;对所提Galerkin及A.D.I.Galerkin格式给出稳定性和收敛性分析,得到最佳H1和L2模估计.     

ALTERNATING-DIRECTION MULTISTEP PRECONDITIONED ITERATIVE METHODS FOR SEMICONDUCTOR PROBLEM WITH HEAT-CONDUCTION

The model of transient behavior of semiconductor with heat-conduction is an initial and boundary problem. Alternating-direction multistep preconditioned iterative methods and theory analyses are given in this paper. Electric potential equation is approximated by mixed finite element method, concentration and heat-conduction equations are approximated by Galerkin alternating-direction multistep methods. Error estimates of optimal order in L2 are demonstrated.