Abstract
In the numerical solution of ordinary differential equations, certain implicit linear multistep formulas, i.e. formulas of type ∑ k j =0 α j x n + j - h k j =0 β j x n + j = 0, (1) with β k > ≠ 0, have long been favored because they exhibit strong (fixed- h ) stability. Lately, it has been observed [1-3] that some special methods of this type are unconditionally fixed- h stable with respect to the step size. This property is of great importance for the efficient solution of stiff [4] systems of differential equations, i.e. systems with widely separated time constants. Such special methods make it possible to integrate stiff systems using a step size which is large relative to the rate of change of the fast-varying components of the solution.

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