## Electrodynamics of Continuous Media |

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Page 50

Žeašča. (10.14) We can say that the quantities without the tilde are the

thermodynamic potentials with

those with it are thermodynamic potentials with

known from ...

Žeašča. (10.14) We can say that the quantities without the tilde are the

thermodynamic potentials with

**respect**to the charges on the conductors, whilethose with it are thermodynamic potentials with

**respect**to their potentials. It isknown from ...

Page 156

The first such terms which do not vanish are linear in air, and quadratic in the

direction cosines of M because of the symmetry with

sign of the time. In general, therefore, the magnetoelastic energy is given by an ...

The first such terms which do not vanish are linear in air, and quadratic in the

direction cosines of M because of the symmetry with

**respect**to a change in thesign of the time. In general, therefore, the magnetoelastic energy is given by an ...

Page 405

The total intensity of the diffraction spot is determined by the effective cross-

section, which is obtained by multiplying the expression (97.13) by p(k) and

integrating with

)p(k) do' ...

The total intensity of the diffraction spot is determined by the effective cross-

section, which is obtained by multiplying the expression (97.13) by p(k) and

integrating with

**respect**to o' and k. or = |...)." s s s exp(-ik-k-2-borjars, × (1 + cos” 9)p(k) do' ...

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### Contents

Methods of solving problems in electrostatics | 9 |

A conducting ellipsoid | 20 |

The forces on a conductor | 31 |

Copyright | |

54 other sections not shown

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### Common terms and phrases

angle anisotropy atoms averaging axes axis body boundary condition calculated charge circuit co-ordinates coefficient components conducting conductor constant corresponding cross-section crystal Curie point curl H current density cylinder denote depends derivative determined dielectric permeability difference differentiating diffraction dipole direction discontinuity distance effect electric field electromagnetic electrons electrostatic ellipsoid entropy equation div expression external field ferroelectric ferromagnetic fluid flux force formula free energy frequency function given gives grad Hence induction integral isotropic Laplace's equation layer Let us consider linear macroscopic magnetic field magnetic moment magnetisation magnitude Maxwell's equations medium metal normal obtain optical particle perpendicular phase piezoelectric plane polarisation PROBLEM propagation properties pyroelectric quantities radius refraction relation respect result rotation scalar scattering self-inductance ſº solution sphere suffixes superconducting surface symmetry tangential temperature theory thermodynamic potential tion uniform unit volume values variable velocity wave vector wire z-axis zero