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Page 62
... Hence x2 1.2 + + E ( Y ) E ( 2 ) ) [ E ( x ) E ( V ) = • ( @gtley 22 ( z ) In tensor notation , independent of the system of co - ordinates chosen , we have $ = e / √ ( \ e \ e ̄1ixxix k ) , where is the determinant of the tensor eik ...
... Hence x2 1.2 + + E ( Y ) E ( 2 ) ) [ E ( x ) E ( V ) = • ( @gtley 22 ( z ) In tensor notation , independent of the system of co - ordinates chosen , we have $ = e / √ ( \ e \ e ̄1ixxix k ) , where is the determinant of the tensor eik ...
Page 66
... Hence we have finally the following expression for the stress tensor : σik = [ F - p ( ƏFƏp ) E , T ] dik + E¿Dx / 4π . ( 15.7 ) In isotropic media , which are those here considered , E and D are parallel . Hence ED = ExDi , and the ...
... Hence we have finally the following expression for the stress tensor : σik = [ F - p ( ƏFƏp ) E , T ] dik + E¿Dx / 4π . ( 15.7 ) In isotropic media , which are those here considered , E and D are parallel . Hence ED = ExDi , and the ...
Page 237
... Hence the ratio v2 / λ ~ -1/3 for λ » Ao and ~ A for λo . Its greatest value is therefore reached when ~ o . Thus ( v.grad ) v λ the two terms are comparable in magnitude , we have H2 ~ Απρύλου . ~ 02/0 . Finally , if ( 55.9 ) According ...
... Hence the ratio v2 / λ ~ -1/3 for λ » Ao and ~ A for λo . Its greatest value is therefore reached when ~ o . Thus ( v.grad ) v λ the two terms are comparable in magnitude , we have H2 ~ Απρύλου . ~ 02/0 . Finally , if ( 55.9 ) According ...
Contents
ELECTROSTATICS OF CONDUCTORS 1 The electrostatic field of conductors | 1 |
2 The energy of the electrostatic field of conductors | 3 |
3 Methods of solving problems in electrostatics | 9 |
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Electrodynamics of Continuous Media: Volume 8 L D Landau,E.M. Lifshitz,L. P. Pitaevskii Snippet view - 1995 |
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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 denote depends derivative determined dielectric permeability diffraction dipole direction discontinuity distance effect electric field electromagnetic electrons electrostatic ellipsoid entropy 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