Electrodynamics of Continuous Media |
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Page 224
... discontinuity , let us consider an element of the surface and use a system of co - ordinates in which it is at rest . † First of all , the mass flux must be continuous at a surface of discontinuity : the mass of fluid entering from one ...
... discontinuity , let us consider an element of the surface and use a system of co - ordinates in which it is at rest . † First of all , the mass flux must be continuous at a surface of discontinuity : the mass of fluid entering from one ...
Page 227
... discontinuities cannot exist indefinitely , even if the conditions ( 53.13 ) are fulfilled . Although no turbu- lence occurs , the sharp discontinuity is replaced by a gradually widening transitional region , in which the velocity and ...
... discontinuities cannot exist indefinitely , even if the conditions ( 53.13 ) are fulfilled . Although no turbu- lence occurs , the sharp discontinuity is replaced by a gradually widening transitional region , in which the velocity and ...
Page 233
... discontinuities . The discon- tinuities discussed here are related in this way to shock waves also . The transition between shock waves and rotational discontinuities is formed by a discontinuity in which there is no change in density ...
... discontinuities . The discon- tinuities discussed here are related in this way to shock waves also . The transition between shock waves and rotational discontinuities is formed by a discontinuity in which there is no change in density ...
Contents
Notation X | 1 |
2 The energy of the electrostatic field of conductors | 3 |
3 Methods of solving problems in electrostatics | 9 |
Copyright | |
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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 diffraction dipole direction discontinuity distance effect electric field electromagnetic electrons electrostatic ellipsoid equation div expression external field ferroelectric ferromagnetic field H fluid flux force formula free energy frequency function given gives grad H₂ Hence incident induction integral isotropic Laplace's equation layer linear macroscopic magnetic field magnetic moment magnetisation magnitude Maxwell's equations medium metal normal obtain optical particle perpendicular piezoelectric plane polarisation PROBLEM propagation properties pyroelectric quantities refraction relation respect result rotation scalar scattering SOLUTION sphere suffixes superconducting surface symmetry tangential temperature theory thermodynamic potential tion unit volume values variable velocity wave vector wire z-axis zero