Electrodynamics of Continuous Media: Volume 8Covers the theory of electromagnetic fields in matter, and the theory of macroscopic electric and magnetic properties of matter. There is a considerable amount of new material particularly on the theory of the magnetic properties of matter and the theory of optical phenomena with new chapters on spatial dispersion and non-linear optics. |
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Page 15
... problem for the whole field . For example , for a very sharp wedge in the field of a point charge e , the passage to the limit of small r in ( 3.21 ) confirms that = constant × √r sin 10 , the constant being [ 4e√ / a / n ( a2 + z2 ) ...
... problem for the whole field . For example , for a very sharp wedge in the field of a point charge e , the passage to the limit of small r in ( 3.21 ) confirms that = constant × √r sin 10 , the constant being [ 4e√ / a / n ( a2 + z2 ) ...
Page 32
... PROBLEMS PROBLEM 1. A small conductor with capacitance c ( equal in order of magnitude to its dimension ) is at a distance r from the centre of a spherical conductor with large radius a ( c ) . The distance r — a from the conductor to ...
... PROBLEMS PROBLEM 1. A small conductor with capacitance c ( equal in order of magnitude to its dimension ) is at a distance r from the centre of a spherical conductor with large radius a ( c ) . The distance r — a from the conductor to ...
Page 206
... PROBLEM 2. The same as Problem 1 , but for a conducting cylinder ( with radius a ) in a uniform periodic mangnetic field perpendicular to its axis . SOLUTION . This problem is the " two - dimensional analogue ” of Problem 1. In what ...
... PROBLEM 2. The same as Problem 1 , but for a conducting cylinder ( with radius a ) in a uniform periodic mangnetic field perpendicular to its axis . SOLUTION . This problem is the " two - dimensional analogue ” of Problem 1. In what ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
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angle anisotropy anisotropy energy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge coefficient components conductor constant coordinates corresponding cross-section crystal Curie point curl H denote depends derivative determined dielectric diffraction direction discontinuity dispersion E₁ E₂ electric field electromagnetic electrons ellipsoid equation expression external field ferroelectric ferromagnet field H fluctuations fluid flux formula free energy frequency function given gives grad H₁ H₂ Hence incident induction integral isotropic Laplace's equation linear magnetic field magnetic moment Maxwell's equations medium normal obtain optical particle permittivity perpendicular perturbation phase plane polarization PROBLEM propagated properties pyroelectric quantities refraction relation respect result rotation scattering sin² SOLUTION sphere suffixes superconducting surface symmetry temperature tensor theory thermodynamic potential transition uniaxial values variable velocity volume wave vector z-axis zero Απ