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The imposition of the boundary conditions is performed by a collocation method through a discrete transformation technique.
The governing integral equations are derived and solved by a collocation method combined with associated boundary conditions.
The problem is solved by a collocation method in a coordinate system which permits the surface temperature to be prescribed directly.
We numerically solve the family of integral equations under consideration by a collocation method and provide a study of reconstructions based on the regularization of the ill-posed integral operators under consideration.
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This singular boundary integral is solved in the same paper by using a collocation method.
The new unknowns (the coefficients of the series) are calculated by using a collocation method.
The singular boundary integral equation we refer to in the present work is solved in [11] by using a collocation method.
We develop a numerical method for a generalized nonlocal elastic model, which is expressed as a composition of a Riesz potential operator with a fractional differential operator, by composing a collocation method with a finite difference discretization.
In Section 3 we discuss the characteristics of different types of solution obtained by Bvp4c, which is a collocation method equivalent to the fourth order monoimplicit-Runge-Kutta method.
The exciting and scattered fields for each fiber are expressed by the eigenfunction expansion, and a collocation method is used to determine the expansion coefficients numerically.
Since (3.16 - 3.18) and (3.27 - 3.29) are coupled nonlinear boundary value problems, these equations are solved numerically by Bvp4c with MATLAB, which is a collocation method equivalent to the fourth order mono-implicit Runge-Kutta method.
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