Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
Dentro del libro
Resultados 1-3 de 74
Página 33
... consider the new variables y = x1 x2 z = x1 + x2 which correspond to the masses of Fig . 1.2 moving together ( y = 0 implies that x1 = x2 ) or oppositely ( z = 0 ) . Each of these motions may be expected to exist independently . ( The ...
... consider the new variables y = x1 x2 z = x1 + x2 which correspond to the masses of Fig . 1.2 moving together ( y = 0 implies that x1 = x2 ) or oppositely ( z = 0 ) . Each of these motions may be expected to exist independently . ( The ...
Página 94
... considering a discrete system with three interior points . 4. Solve Exercise 2 approximately by considering a discrete system with three interior points . 5. Consider the system shown below : Pin joint W 94 SYSTEMS WITH AN INFINITE ...
... considering a discrete system with three interior points . 4. Solve Exercise 2 approximately by considering a discrete system with three interior points . 5. Consider the system shown below : Pin joint W 94 SYSTEMS WITH AN INFINITE ...
Página 220
... consider the various & for which λ = f * Hf 打 was stationary for N f = Σaili i = 1 For an orthonormal set . , it was found that the a , satisfied the equation Σ q1 * Hq , a1 = λa , Now write the N solutions as jo σ = 1 , 2 , 3 ...
... consider the various & for which λ = f * Hf 打 was stationary for N f = Σaili i = 1 For an orthonormal set . , it was found that the a , satisfied the equation Σ q1 * Hq , a1 = λa , Now write the N solutions as jo σ = 1 , 2 , 3 ...
Contenido
34 | 12 |
The Laplacian V² in One Dimension | 18 |
Solution for Diagonalizable Matrices | 21 |
Derechos de autor | |
Otras 31 secciones no mostradas
Otras ediciones - Ver todas
Términos y frases comunes
approximate arbitrary asymptotic ax² base vectors basis Bessel functions boundary conditions Chap coefficients consider constant continuous systems contour corresponding cylindrical functions d²/dx² defined definition denoted determinant diagonal diagonalizable differential equation Dirac notation eigen eigencolumns eigenfunctions eigenvalue problem eigenvectors elements evaluate expansion finite number follows formula given Green's function Hence Hermitian matrix Hermitian operator infinite integral representation integral theorem inverse Laplace transform linear operator linearly independent lowest eigenvalue matrix McGraw-Hill Book Company method multiplication nonsingular normal matrix obtained orthonormality conditions perturbation procedure relations result Ritz method satisfies scattering sinh solution solve spherical substitution transformation functions trial functions vanish variable vector space Verify wave whence write written x₁ y₁ yields York zero ηπχ παχ ди ду дх