Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
Dentro del libro
Resultados 1-3 de 42
Página 128
... coordinates . 10.2 Conduction of Heat in an Infinite Insulated Plate . Cartesian Coordinates Consider the conduction of heat in an infinite insulated plate lying in the x , y coordinate plane . Let c represent the specific heat , p the ...
... coordinates . 10.2 Conduction of Heat in an Infinite Insulated Plate . Cartesian Coordinates Consider the conduction of heat in an infinite insulated plate lying in the x , y coordinate plane . Let c represent the specific heat , p the ...
Página 131
... Coordinates In a large number of problems on the conduction of heat in an infinite insulated plate the initial temperature distribution is a function only of the distance r from the origin of coordinates . In such cases it is much more ...
... Coordinates In a large number of problems on the conduction of heat in an infinite insulated plate the initial temperature distribution is a function only of the distance r from the origin of coordinates . In such cases it is much more ...
Página 132
Gerald Goertzel, Nunzio Tralli. more convenient to use polar coordinates than cartesian coordinates . In general , two methods of procedure are available , namely : 1. Transform the original problem , Eq . ( 10.1 ) , to polar coordinates ...
Gerald Goertzel, Nunzio Tralli. more convenient to use polar coordinates than cartesian coordinates . In general , two methods of procedure are available , namely : 1. Transform the original problem , Eq . ( 10.1 ) , to polar coordinates ...
Contenido
Perturbation of Eigenvalues | 14 |
The Laplacian v2 in One Dimension | 18 |
Solution for Diagonalizable Matrices | 21 |
Derechos de autor | |
Otras 19 secciones no mostradas
Otras ediciones - Ver todas
Términos y frases comunes
approximate arbitrary ax² basis Bessel function boundary conditions chap coefficients column consider constant continuous systems contour coordinates corresponding cylindrical functions d²/dx² defined denoted determinant diagonal differential equation Dirac notation domain eigen eigencolumns eigenfunctions eigenvalue equation eigenvector eikr evaluate expansion finite number follows Fourier given Green's function Hence Hermitian Hermitian matrix Hermitian operator infinite integral inverse Laplace transform Laplacian linear operator linearly independent lowest eigenvalue matrix membrane method multiplication nonsingular normal obtained orthonormality conditions plane problem procedure relations representation result satisfies the boundary scattering sinh solve spherical spherical harmonics string Substitution theorem trial functions vanish variable vector space Verify wave write written y₁ yields York zero ηπχ πο ποχ ди ду дх