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Mathematical Study of the Nonlinear Singular Integral Magnetic Field Equation. II

Mark J. Friedman

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Source: Crossref

Published: Aug 1, 1981

DOI: 10.1137/0718042

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Source abstract

For the numerical treatment of the nonlinear singular integral magnetic field equation RM=hM+AM=HaR{\bf M} = h{\bf M} + A{\bf M} = {\bf H}_a, which has been considered by the author in Part I [SIAM J. Appl. Math., 39 (1980), pp. 14-20]. Tucker stability is established in the case where (hM)(x)=g(M(x),x)(h{\bf M})(x) = {\bf g}({\bf M}(x),x) is a bounded, continuous, and strongly monotone operator in L2{\bf L}^2 . In the special cases g(M,x)=cM{\bf g}({\bf M},x) = c{\bf M} and g(M,x)=g(M,x)M/M{\bf g}({\bf M},x) = g(M,x){{\bf M}/M}, which are important for engineering applications, explicit perturbation estimates are obtained.

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