Some least-squares Galerkin procedures for first-order time-dependent convection–diffusion system

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Abstract

Four least-squares Galerkin finite element schemes are formulated to solve first-order time-dependent convection–diffusion systems and the convergence of these schemes is analyzed.

Introduction

The purpose of this paper is to analyze the least-squares Galerkin finite element methods for solving first-order time-dependent convection–diffusion systems. Let Ω be an open bounded domain Rd, 1⩽d⩽3, with a Lipschitz continuous boundary Γ. We consider the following initial-boundary value problem of a first-order time-dependent convection–diffusion systemc(x)u(x,t)t+divσ(x,t)+q(x,t)u(x,t)=f(x,t),x∈Ω,0<t⩽T,σ(x,t)+A(x)∇u(x,t)+b(x,t)u(x,t)=0,x∈Ω,0<t⩽T,u(x,t)=0,x∈ΓD,σ(x,t)·ν(x)=0,x∈ΓN,0⩽t⩽T,u(x,0)=u0(x),x∈Ω,where div is the divergence operator and ∇ the gradient operator, flow field b=(b1(x,t),…,bd(x,t))T, source term q=q(x,t)⩾0 and exterior flow function f=f(x,t) in (1.1) are some given functions, the coefficient c=c(x) is a positive function and the diffusion coefficient matrix A=(aij(x))d×d is a symmetric uniformly positive definite matrix, i.e., there exist some positive constants c and a such thatai=1dξ2ii,j=1daij(x)ξiξj,c⩽c(x),∀ξ∈Rd,x∈Ω,and Γ=ΓDΓN and ν is the unit vector normal to ΓN.

Much research on least-squares finite element schemes and their applications to various boundary value problems of elliptic equations or systems has been done and some systematic theory on the ellipticity of schemes and convergence of approximate solutions have also been established, e.g., see Refs. [2], [6], [7], [8], [9], [10], [11], [15], [17], [21], [22]. In recent years, the least-squares finite element methods have been extended to unstationary problems, e.g., see Refs. [12], [14], [16], [20], [24], in which some very effective numerical results were shown. However, the theory on the convergence of least-squares finite element methods for evolutionary problems has not been clarified.

Our main results in this paper are that four least-squares Galerkin finite element procedures are formulated to solve the first-order time-dependent convection–diffusion problems (1.1) in Section 2 and the convergence theory on these algorithms is established in Section 3.

Section snippets

Least-squares Galerkin finite element procedures

Throughout this paper we use usual definitions and notations of Sobolev spaces as in Ref. [1]. Let Wk,p(Ω)(k⩾0,1⩽p⩽∞) be Sobolev spaces defined on Ω with usual norms ∥·∥Wk,p(Ω) and Hk(Ω)=Wk,2(Ω). Define inner products as follows:(u,v)=∫Ωu(x)v(x)dx∀u,v∈L2(Ω),(σ,ω)=i=1dii)∀σ,ω∈(L2(Ω))d.Introduce the spaces H={ω∈(L2(Ω))d; divω∈L2(Ω), ω·ν=0 on ΓN} and S={v∈H1(Ω);v=0 on ΓD}. Make a time partition 0=t0<t1<⋯<tn<⋯<tM−1<tM=T and set τn=tntn−1 and τ=max1⩽nMτn. Let wn(x)=w(x,tn) and wn−1/2(x)=w(x,tn

Convergence analysis

In this section, we denote by K and δ some general constants and small positive constants independent of the mesh parameters hu,hσ and τ, which may be different at different occurrences. We assume that the finite element spaces Hhσ and Shu have approximate properties [3], [4], [5], [13], [18], [19] that there exist some integers k1k⩾0 and m⩾1 such thatinfωh∈Hhσ∥ω−ωh(L2(Ω))d⩽Khσk+1∥ω∥(Hk+1(Ω))d,infωh∈Hhσdiv(ω−ωh)∥L2(Ω)⩽Khk1σ∥ω∥(Hk1+1(Ω))d,infvhShu{∥v−vhL2(Ω)+hu∥∇(v−vh)∥(L2(Ω))d}⩽K1hm+1u∥v∥H

Acknowledgements

This work was supported in part by China State Major Key Project for Basic Researches, by the Research Fund for Doctoral Program of High Education and TCTPF of China State Education Commission.

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