The functions φ1, φ2,…, φn are always chosen to be simple and are called trial functions. The success of the method is due in part to choosing these functions to be low-degree splines. This in turn generally leads to a system of equations for the coefficients c1, c2,…, cn that involves the treatment of sparse matrices, i.e. matrices in which a large proportion of the elements are zero; very efficient software can then be used.
In Galerkin's method the criterion for choosing the coefficients is that the amount by which u(x) fails to satisfy the equation is in a certain sense small. The Rayleigh–Ritz method is a variational method. The finite-element method can in general be regarded as a process in which a solution in an infinite-dimensional space is replaced by an approximation that lies in a finite-dimensional subspace. The whole process is referred to as finite-element analysis.
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