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The new technique involved substituting trial functions of unknown amplitude into the variational functional, which is then rendered stationary as an algebraic function of the amplitude coefficients.
A suitable set of trial functions is proposed.
Shannon's delta kernel is used for trial functions.
Timoshenko beam functions were used as the trial functions.
Legendre orthogonal polynomials are used as trial functions.
The following result relies on a construction of trial functions.
And w 1 and w 2 are trial functions.
Kato next picked the subspace, W, of trial functions.
The Ritz method, based on highly stable trigonometric trial functions, is used as solution technique.
In order to avoid long computational run times, physically pertinent trial functions are utilized.
The Rayleigh Ritz method was used applying beam functions as the trial functions.
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