Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
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Página 121
... string , take the string as lying along the x axis from x = 0 to x = L and denote by y ( x , t ) the displacement at right angles to the axis at any point x at any time t . The equation of motion is 22 If y ( x , 1 ) 22 y ( x , t ) = c2 ...
... string , take the string as lying along the x axis from x = 0 to x = L and denote by y ( x , t ) the displacement at right angles to the axis at any point x at any time t . The equation of motion is 22 If y ( x , 1 ) 22 y ( x , t ) = c2 ...
Página 206
... String As an application of the procedure described above , consider the variation in frequency and shape of a string whose mass per unit length is varied from its original condition of uniformity . The string is taken as extending ...
... String As an application of the procedure described above , consider the variation in frequency and shape of a string whose mass per unit length is varied from its original condition of uniformity . The string is taken as extending ...
Página 237
... string lie along the x axis in the region 0 ≤ x ≤a , and let the density distribution be denoted by p ( x ) . Then , the actual string might be approximated by a weightless string loaded with n masses m , at the points x ; = ih i = 0 ...
... string lie along the x axis in the region 0 ≤ x ≤a , and let the density distribution be denoted by p ( x ) . Then , the actual string might be approximated by a weightless string loaded with n masses m , at the points x ; = ih i = 0 ...
Contenido
Solution for Diagonalizable Matrices | 21 |
The Evaluation of a Function of a Matrix for an Arbitrary Matrix | 38 |
13 | 44 |
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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