Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
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Página 142
... Bessel functions must satisfy the boundary condition Jn ( kp ) = 0. This condition determines the eigenvalues as follows : The Bessel function J ( 2 ) is zero only for certain values of 2 , say 21 , λn2 , .... From the properties of ...
... Bessel functions must satisfy the boundary condition Jn ( kp ) = 0. This condition determines the eigenvalues as follows : The Bessel function J ( 2 ) is zero only for certain values of 2 , say 21 , λn2 , .... From the properties of ...
Página 276
... Bessel or Hankel Transforms . Substitution of ( 2B.50 ) into ( 2B.49 ) yields the Fourier - Bessel integral ∞0 f ( = [ " [ [ " $ { r ^ , „ ( kr ) r ' dr2 ] J ( kr ) k dk ( 2B.51 ) = 0 which is the analogue of the cosine Fourier ...
... Bessel or Hankel Transforms . Substitution of ( 2B.50 ) into ( 2B.49 ) yields the Fourier - Bessel integral ∞0 f ( = [ " [ [ " $ { r ^ , „ ( kr ) r ' dr2 ] J ( kr ) k dk ( 2B.51 ) = 0 which is the analogue of the cosine Fourier ...
Página 296
... Bessel functions ) Debye , P. , 291 , 292 Degenerate matrix , 26 Delta , Kronecker , 12 Delta function , 98-100 Determinant , 14-15 , 243-251 of matrix product , 15 , 250-251 Diagonal matrix , 7 Diagonalization of matrix , 26-27 , 64 ...
... Bessel functions ) Debye , P. , 291 , 292 Degenerate matrix , 26 Delta , Kronecker , 12 Delta function , 98-100 Determinant , 14-15 , 243-251 of matrix product , 15 , 250-251 Diagonal matrix , 7 Diagonalization of matrix , 26-27 , 64 ...
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