Some Mathematical Methods of Physics |
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Página 80
Thus , the matrix M has been eliminated , and instead the difference operator d2 with boundary conditions ( 6.9 ) and ( 6.10 ) has been intro- duced . i Such a procedure , of writing a difference equation y1 = Dx , and boundary ...
Thus , the matrix M has been eliminated , and instead the difference operator d2 with boundary conditions ( 6.9 ) and ( 6.10 ) has been intro- duced . i Such a procedure , of writing a difference equation y1 = Dx , and boundary ...
Página 97
... boundary conditions ( 8.4 ) is Hermitian . It is incorrect to omit the italic phrase . The boundary conditions are part of the definition of the operator . When an operator L is defined by ( 8.6 ) OPERATORS IN CONTINUOUS SYSTEMS 97.
... boundary conditions ( 8.4 ) is Hermitian . It is incorrect to omit the italic phrase . The boundary conditions are part of the definition of the operator . When an operator L is defined by ( 8.6 ) OPERATORS IN CONTINUOUS SYSTEMS 97.
Página 144
[ In the case of the circular membrane 2 = n = · 0 , ± 1 , ± 2 , ... because of the single - valuedness condition on ƒx , n ( r , 0 ) . ] λ is now determined from the boundary conditions = fx.a ( r , 0 ) Ja ( kr ) ( A cos 0 + B sin 0 ) ...
[ In the case of the circular membrane 2 = n = · 0 , ± 1 , ± 2 , ... because of the single - valuedness condition on ƒx , n ( r , 0 ) . ] λ is now determined from the boundary conditions = fx.a ( r , 0 ) Ja ( kr ) ( A cos 0 + B sin 0 ) ...
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Contenido
Solution for Diagonalizable Matrices | 21 |
The Evaluation of a Function of a Matrix for an Arbitrary Matrix | 38 |
13 | 44 |
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applied approaches approximate arbitrary basis becomes Bessel boundary conditions called chap chapter Clearly coefficients column complete consider constant continuous contour coordinates corresponding defined definition demonstrated denoted derived determinant difference differential equation direction discussed eigencolumn eigenfunctions eigenvalue element equal equation evaluate example exists expansion expression finite follows Fourier function given Green's function Hence independent infinite integral introduce known limit linear lowest matrix method multiplication normalized notation Note obtained operator orthonormality path Physics plane positive problem procedure reduces relations replaced representation represented result satisfies scattering solution solve space string Substitution Suppose theorem transformation unique vanish variable vector verified wave write written yields York zero ду