Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
Dentro del libro
Resultados 1-3 de 9
Página 283
... path of integration W , is equal to W1 + W2 . 1 -4π 3π π 2π 3π 4π مدد Figure 2C.1 . Allowed regions in the w plane . Expression ( 2C.10 ) for the integral representation of the cylindrical functions Z , may now be written Z , ( ( p ) ...
... path of integration W , is equal to W1 + W2 . 1 -4π 3π π 2π 3π 4π مدد Figure 2C.1 . Allowed regions in the w plane . Expression ( 2C.10 ) for the integral representation of the cylindrical functions Z , may now be written Z , ( ( p ) ...
Página 288
... path of integration does not pass through a singularity of the integrand . Let z = xiy and _f ( z ) = u ( x , y ) + ... path as possible we must avoid the mountains and keep to the valleys as much as possible . In the interesting case ...
... path of integration does not pass through a singularity of the integrand . Let z = xiy and _f ( z ) = u ( x , y ) + ... path as possible we must avoid the mountains and keep to the valleys as much as possible . In the interesting case ...
Página 289
... path . Such a path is called a line of steepest ascent and descent . There will be one into each valley . If zo is a saddle point , f ( z ) near it can be expanded in the form Zo ƒ ( z ) = ƒ ( z ) + 1⁄2 ( z − zo ) 2ƒ ̋ ( zo ) + ...
... path . Such a path is called a line of steepest ascent and descent . There will be one into each valley . If zo is a saddle point , f ( z ) near it can be expanded in the form Zo ƒ ( z ) = ƒ ( z ) + 1⁄2 ( z − zo ) 2ƒ ̋ ( zo ) + ...
Contenido
Solution for Diagonalizable Matrices | 21 |
The Evaluation of a Function of a Matrix for an Arbitrary Matrix | 38 |
13 | 44 |
Derechos de autor | |
Otras 25 secciones no mostradas
Otras ediciones - Ver todas
Términos y frases comunes
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