Classical Electrodynamics |
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Page 4
From the definitions above it is evident that , for an arbitrary function f ( x ) , ( 3 ) f (
x ) 8 ( x – a ) dx = f ( a ) , and ( – a ) dx = - f ' ( a ) , where a prime denotes
differentiation with respect to the argument . If the delta function has as argument
a ...
From the definitions above it is evident that , for an arbitrary function f ( x ) , ( 3 ) f (
x ) 8 ( x – a ) dx = f ( a ) , and ( – a ) dx = - f ' ( a ) , where a prime denotes
differentiation with respect to the argument . If the delta function has as argument
a ...
Page 18
10 Formal Solution of Electrostatic Boundary - Value Problem with Green ' s
Function Da The solution of Poisson ' s or Laplace ' s equation in a finite volume
V with either Dirichlet or Neumann boundary conditions on the bounding surface
S ...
10 Formal Solution of Electrostatic Boundary - Value Problem with Green ' s
Function Da The solution of Poisson ' s or Laplace ' s equation in a finite volume
V with either Dirichlet or Neumann boundary conditions on the bounding surface
S ...
Page 78
Then it is convenient to express the Green ' s function as a series of products of
the functions appropriate to the coordinates in question . We first illustrate the
type of expansion involved by considering spherical coordinates . For the case of
no ...
Then it is convenient to express the Green ' s function as a series of products of
the functions appropriate to the coordinates in question . We first illustrate the
type of expansion involved by considering spherical coordinates . For the case of
no ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
RelativisticParticle Kinematics and Dynamics | 391 |
Copyright | |
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