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. |
From inside the book
Results 1-3 of 85
Page 54
... crystals . The majority of the types of crystal symmetry do not admit this constant vector ( see below ) , and we then have simply i D1 = & ik Ek⋅ ( 13.2 ) The tensor & is symmetrical : Eik = Eki . ( 13.3 ) In order to prove this , it ...
... crystals . The majority of the types of crystal symmetry do not admit this constant vector ( see below ) , and we then have simply i D1 = & ik Ek⋅ ( 13.2 ) The tensor & is symmetrical : Eik = Eki . ( 13.3 ) In order to prove this , it ...
Page 56
... crystal symmetry . Since , in any symmetry transformation , all the properties of the crystal must remain unchanged , it is clear that the only crystals which can be pyro- electric are those in which there is a direction which is ...
... crystal symmetry . Since , in any symmetry transformation , all the properties of the crystal must remain unchanged , it is clear that the only crystals which can be pyro- electric are those in which there is a direction which is ...
Page 70
... crystal , the components of the tensor Yi , kl must remain unaltered in value . Hence it follows at once that no piezoelectric body can have a centre of symmetry or , in particular , be isotropic . For , on reflection in the centre ...
... crystal , the components of the tensor Yi , kl must remain unaltered in value . Hence it follows at once that no piezoelectric body can have a centre of symmetry or , in particular , be isotropic . For , on reflection in the centre ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
Copyright | |
102 other sections not shown
Other editions - View all
Common terms and phrases
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