“…Following Lawson [7] and Swayne [9], the vector yj/ The development of numerical methods will be based on making appropriate approximations to the exponentials in this recurrence relation. Higher-order Pade approximants [8] are popularly employed (see, for instance, [4,5,11]) for such exponentials. Methods based on the use of these approximants are of high accuracy in time and, in the case of the subdiagonal Pades, have good stability properties.…”
A parallel algorithm is developed for the numerical solution of the diffusion equation u, = u,,, 0 < * < X, 0 < / < 7\ subject to u(x, 0) = / ( * ) , u x (X, t) = g(t) and the specification of mass f a u(x,t)dx = M(t), 0 < b < X.
“…Following Lawson [7] and Swayne [9], the vector yj/ The development of numerical methods will be based on making appropriate approximations to the exponentials in this recurrence relation. Higher-order Pade approximants [8] are popularly employed (see, for instance, [4,5,11]) for such exponentials. Methods based on the use of these approximants are of high accuracy in time and, in the case of the subdiagonal Pades, have good stability properties.…”
A parallel algorithm is developed for the numerical solution of the diffusion equation u, = u,,, 0 < * < X, 0 < / < 7\ subject to u(x, 0) = / ( * ) , u x (X, t) = g(t) and the specification of mass f a u(x,t)dx = M(t), 0 < b < X.
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