Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
From inside the book
Results 1-3 of 78
Page 25
... components by a suitable choice of axes . This is referred to as the diagonalization of the tensor or transformation to principal axes of the tensor . We shall in that case have only the components Q11 , Q22 , Q33 . In this particular ...
... components by a suitable choice of axes . This is referred to as the diagonalization of the tensor or transformation to principal axes of the tensor . We shall in that case have only the components Q11 , Q22 , Q33 . In this particular ...
Page 69
... components of the vector ) which obeys the same law of transformation as the cooridnates of a point . Now consider the nine numbers formed by multiplying three components of a vector A ; by three components of another vector B. Their ...
... components of the vector ) which obeys the same law of transformation as the cooridnates of a point . Now consider the nine numbers formed by multiplying three components of a vector A ; by three components of another vector B. Their ...
Page 316
... components of the tensor 7 " are made up of six components of the Maxwell stress tensor , the three components of the momentum vector ( the Poynting vector ) and the energy density . Lagrangian and Hamiltonian of a charged particle in ...
... components of the tensor 7 " are made up of six components of the Maxwell stress tensor , the three components of the momentum vector ( the Poynting vector ) and the energy density . Lagrangian and Hamiltonian of a charged particle in ...
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