Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
From inside the book
Results 1-3 of 46
Page 26
... coordinates of the field point , besides the coefficients which are constants so far as the coordinates of the field point are concerned . Again as the variable parts appear as partial derivatives of 1 / r cach term separately is a ...
... coordinates of the field point , besides the coefficients which are constants so far as the coordinates of the field point are concerned . Again as the variable parts appear as partial derivatives of 1 / r cach term separately is a ...
Page 68
... coordinates of the point . These coordinates may be of different types but we shall restrict ourselves to orthogonal Cartesian coordinates i.e. we choose three axes which are mutually perpendicular and meet at a point , O. The coordinates ...
... coordinates of the point . These coordinates may be of different types but we shall restrict ourselves to orthogonal Cartesian coordinates i.e. we choose three axes which are mutually perpendicular and meet at a point , O. The coordinates ...
Page 69
... coordinates of a point so that it will obey the same transformation formulae as the coordinates . Thus if A , be the components of the vector in the unprimed coordinate system and A , after the transformation ( 1 ) we shall have Α = Σαμ ...
... coordinates of a point so that it will obey the same transformation formulae as the coordinates . Thus if A , be the components of the vector in the unprimed coordinate system and A , after the transformation ( 1 ) we shall have Α = Σαμ ...
Contents
The empirical basis of electrostatics | 1 |
Direct calculation of fields | 7 |
dipoles9 The Dirac 8function13 | 13 |
Copyright | |
23 other sections not shown
Other editions - View all
Common terms and phrases
angle angular axes axis B₁ boundary conditions calculate called charge density charged particle coil components conductor consider coordinates cos² cose dielectric constant dipole dipole moment direction distance E₁ electric field electromagnetic field electromotive force electron electrostatic equation 16 expression field due field point finite fluid formula frame frequency function gives Hence incident interaction Laplace's equation linear Lorentz Lorentz transformation magnetic field magnitude Maxwell's equations momentum motion normal obtain orthogonal P₁ permanent magnets perpendicular photon plane plasma point charge polarization Poynting vector R₁ radiation field radiation reaction radius refracted region scalar sin² solution spherical surface integral symmetry tensor term theorem theory of relativity transformation transverse uniform vanishes vector potential velocity wave length Απ дв дг ді дх