A Critique of the Variational Method in Scattering Problems

Cover A Critique of the Variational Method in Scattering Problems
A Critique of the Variational Method in Scattering Problems
D S Jones
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Is used, the set is also required to be complete. Now try an approximation G to g given by (8) G . N c^G^ n where the sum may involve either a finite or infinite number of terms and the constants c are to determined. We shall now prove the following - 5 - Theorem 1 The necessary and sufficient conditions for the express- ion in (7) to be stationary for small variations of G are (9) (^» V ' (°n' ^^ (n-0, 1, ... ).
G then satisfies (f, G) = (G, LG) and A - (f, G).
The importance of this theorem l
...ies in the fact that equations (9) are precisely those obtained by substituting the expansion (8) in (1) and taking the inner product of both sides with G, which is Galerkin's process.
Then A may be calculated directly from its original definition (2) because the approximation satisfies the reciprocity theorem. Obviously this direct method of setting up the equations is to be preferred to determining them via the variation principle. It should be remarked that, if we make a one -terra approximation so that G » c G, the reciprocity theorem is satisfied if 00 (f, G^) « c^(G^, LG^) and (f, G) becomes (f, Gq)^/(Gq, UG ) which is the same as would be calculated from (7).


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