Some Mathematical Methods of Physics |
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Página 126
... us how to study the wave in a finite string as a superposition of waves traveling to the right and to the left . Thus the wave traveling to the right ( increasing x ) may be written as x - ct · A + 1 y ( x — ct , 0 ) — 1 ̄ý ( u ...
... us how to study the wave in a finite string as a superposition of waves traveling to the right and to the left . Thus the wave traveling to the right ( increasing x ) may be written as x - ct · A + 1 y ( x — ct , 0 ) — 1 ̄ý ( u ...
Página 176
CHAPTER 13 Radiation and Scattering Problems 13.1 The Outgoing Wave Condition Consider the propagation of waves outward from a given source . Let c represent the velocity of propagation . Then , the amplitude of the wave ( r , t ) at ...
CHAPTER 13 Radiation and Scattering Problems 13.1 The Outgoing Wave Condition Consider the propagation of waves outward from a given source . Let c represent the velocity of propagation . Then , the amplitude of the wave ( r , t ) at ...
Página 185
The incident wave of ( 13.39 ) has a density of | inc | 2 = leikz | 2 = 1 , so that it corresponds to an incident current density of clinc2 = c . According to ( 13.40 ) , the outgoing wave at large r corresponds to a radial outward ...
The incident wave of ( 13.39 ) has a density of | inc | 2 = leikz | 2 = 1 , so that it corresponds to an incident current density of clinc2 = c . According to ( 13.40 ) , the outgoing wave at large r corresponds to a radial outward ...
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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