A finite element collocation method for quasilinear parabolic equations

Author:

Douglas Jim,Dupont Todd

Abstract

Let the parabolic problem c ( x , t , u ) u t = a ( x , t , u ) u x x + b ( x , t , u , u x ) , 0 > x > 1 , 0 > t T , u ( x , 0 ) = f ( x ) , u ( 0 , t ) = g 0 ( t ) , u ( 1 , t ) = g 1 ( t ) c(x,t,u){u_t} = a(x,t,u){u_{xx}} + b(x,t,u,{u_x}),0 > x > 1,0 > t \leqq T,u(x,0) = f(x),u(0,t) = {g_0}(t),u(1,t) = {g_1}(t) , be solved approximately by the continuous-time collocation process based on having the differential equation satisfied at Gaussian points ξ i , 1 {\xi _{i,1}} and ξ i , 2 {\xi _{i,2}} in subintervals ( x i 1 , x i ) ({x_{i - 1}},{x_i}) for a function U : [ 0 , T ] H 3 U:[0,T] \to {\mathcal {H}_3} , the class of Hermite piecewise-cubic polynomial functions with knots 0 = x 0 > x 1 > > x n = 1 0 = {x_0} > {x_1} > \cdots > {x_n} = 1 . It is shown that u U = O ( h 4 ) u - U = O({h^4}) uniformly in x and t, where h = max ( x i x i 1 ) h = \max ({x_i} - {x_{i - 1}}) .

Publisher

American Mathematical Society (AMS)

Subject

Applied Mathematics,Computational Mathematics,Algebra and Number Theory

Reference5 articles.

1. The effect of interpolating the coefficients in nonlinear parabolic Galerkin procedures;Douglas, Jim, Jr.;Math. Comput.,1975

2. Travaux et Recherches Math\'{e}matiques, No. 17;Lions, J.-L.,1968

3. B. Wendroff, First Principles of Numerical Analysis, Addison-Wesley, Reading, Mass., 1969.

4. M. F. Wheeler, Thesis, Rice University, Houston, Texas, 1971; SIAM J. Numer. Anal. (To appear.)

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