Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
Dentro del libro
Resultados 1-3 de 16
Página 22
... desired . Such a method of evaluation will be determined in this chapter . 2.2 Eigenvalues and Eigencolumns If there exist a number λ and a column u such that Au = λι ( 2.7 ) then 2 is said to be an eigenvalue of A , u is said to be an ...
... desired . Such a method of evaluation will be determined in this chapter . 2.2 Eigenvalues and Eigencolumns If there exist a number λ and a column u such that Au = λι ( 2.7 ) then 2 is said to be an eigenvalue of A , u is said to be an ...
Página 73
... desired . In Part Two this circumstance will be used in order to extend many of the considera- tions of Part One to systems with infinite numbers of degrees of freedom , i.e. , to continuous systems . Specifically , meaning will be ...
... desired . In Part Two this circumstance will be used in order to extend many of the considera- tions of Part One to systems with infinite numbers of degrees of freedom , i.e. , to continuous systems . Specifically , meaning will be ...
Página 275
... desired to expand a function between -L and + L , ( 2B.37 ) can be used only if the function is odd , ( 2B.40 ) when it is even . However , any function can be represented as the sum of an even and an odd one . Hence , if an arbitrary ...
... desired to expand a function between -L and + L , ( 2B.37 ) can be used only if the function is odd , ( 2B.40 ) when it is even . However , any function can be represented as the sum of an even and an odd one . Hence , if an arbitrary ...
Contenido
34 | 12 |
Solution for Diagonalizable Matrices | 21 |
The Evaluation of a Function of a Matrix for an Arbitrary Matrix | 38 |
Derechos de autor | |
Otras 29 secciones no mostradas
Otras ediciones - Ver todas
Términos y frases comunes
approximation arbitrary ax² basis Bessel functions boundary conditions Chap coefficients column consider constant continuous systems contour coordinates corresponding cylindrical functions d²/dx² defined definition denoted determinant diagonal differential equation Dirac notation domain eigencolumns eigenfunctions eigenvectors elements evaluate expansion F₁ finite number follows formula Fourier given Green's function Hence Hermitian Hermitian matrix Hermitian operator infinite integral inverse Laplacian linear operator linearly independent lowest eigenvalue Mathematical matrix McGraw-Hill Book Company method multiplication nonsingular normal number of degrees obtained orthonormality conditions Physics problem relations representation result Ritz method scattering sinh solution solve spherical spherical harmonics string Substitution theorem transform trial functions vanish variable vector space Verify w₁ wave write written x₁ Y₁ yields York zero ηπχ ди ду дх