
doi: 10.1002/fld.2493
AbstractThe MHD Falkner–Skan equation arises in the study of laminar boundary layers exhibiting similarity on the semi‐infinite domain. The proposed approach is equipped by the orthogonal Sinc functions that have perfect properties. This method solves the problem on the semi‐infinite domain without truncating it to a finite domain and transforming domain of the problem to a finite domain. In addition, the governing partial differential equations are transformed into a system of ordinary differential equations using similarity variables, and then they are solved numerically by the Sinc‐collocation method. It is shown that the Sinc‐collocation method converges to the solution at an exponential rate. Copyright © 2010 John Wiley & Sons, Ltd.
semi-infinite, collocation method, Other numerical methods (fluid mechanics), MHD Falkner-Skan equation, Magnetohydrodynamics and electrohydrodynamics, Spectral, collocation and related methods for boundary value problems involving PDEs, Boundary-layer theory, separation and reattachment, higher-order effects, sinc functions, nonlinear ODE
semi-infinite, collocation method, Other numerical methods (fluid mechanics), MHD Falkner-Skan equation, Magnetohydrodynamics and electrohydrodynamics, Spectral, collocation and related methods for boundary value problems involving PDEs, Boundary-layer theory, separation and reattachment, higher-order effects, sinc functions, nonlinear ODE
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