Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
Dentro del libro
Resultados 1-3 de 21
Página 38
... applied to any matrix A for which S - 1 existed and indeed yielded f ( A ) = Sƒ ( A ) S - 1 An alternate method of expressing f ( A ) is by means of the Cauchy - integral formula from complex variable theory.1 f ( A ) = 1 f ( Z ) dz 2πi ...
... applied to any matrix A for which S - 1 existed and indeed yielded f ( A ) = Sƒ ( A ) S - 1 An alternate method of expressing f ( A ) is by means of the Cauchy - integral formula from complex variable theory.1 f ( A ) = 1 f ( Z ) dz 2πi ...
Página 49
... applied . Find the = 10. Consider the circuit of Exercise 9. At time t sin wt is applied . Find the current at any time t > 0 . References = · 0 , an emf ɛ = Carslaw , H. S. and J. C. Jaeger : " Operational Methods in Applied ...
... applied . Find the = 10. Consider the circuit of Exercise 9. At time t sin wt is applied . Find the current at any time t > 0 . References = · 0 , an emf ɛ = Carslaw , H. S. and J. C. Jaeger : " Operational Methods in Applied ...
Página 232
... Applied Mathematics , ” Prentice - Hall , Inc. , Englewood Cliffs , N.J. , 1952 . Morse , P. M. , and H. Feshbach : " Methods of Theoretical Physics , " chap . 9 , McGraw - Hill Book Company , Inc. , New York , 1953 . CHAPTER 17 ...
... Applied Mathematics , ” Prentice - Hall , Inc. , Englewood Cliffs , N.J. , 1952 . Morse , P. M. , and H. Feshbach : " Methods of Theoretical Physics , " chap . 9 , McGraw - Hill Book Company , Inc. , New York , 1953 . CHAPTER 17 ...
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