Some new methods for stiff differential equations
1979; Taylor & Francis; Volume: 7; Issue: 1 Linguagem: Inglês
10.1080/00207167908803156
ISSN1029-0265
Autores Tópico(s)Electromagnetic Simulation and Numerical Methods
ResumoA numerical method applied to the differential equation y′=λy can lead to a solution of the form , where z and w = λh satisfy an equation P(w, z) = 0. In general P(w,z) is a polynomial in both w and z, of degree M in w and N in z. Existing multistep and Runge-Kuta methods correspond to the cases M = 1 and N = 1 respectively. New methods are fottd by taking MS≧2N≧2. The approach here is first to find a suitable polynomial P(w,z) with the desired stability properties, and then to find a process which leads to this polynomial. Third- and fourth-order A- and L-stable processes are given of the semi-explicit arid linearly implicit types.
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