Electrodynamics of Continuous Media |
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Page 7
... charge which causes the field , and is the potential at this charge due to the conductor . W does not include the energy of the charge e in its own field , since we are interested only in the energy of the conductor . The charge on the ...
... charge which causes the field , and is the potential at this charge due to the conductor . W does not include the energy of the charge e in its own field , since we are interested only in the energy of the conductor . The charge on the ...
Page 8
... charge e ( regarding the latter as a very small conductor ) . In one state the charge e is present , the charges on the conductors are ea , and their potentials are zero . In the other state the charge e is zero , and one of the ...
... charge e ( regarding the latter as a very small conductor ) . In one state the charge e is present , the charges on the conductors are ea , and their potentials are zero . In the other state the charge e is zero , and one of the ...
Page 10
... charge e is given by σ = 1 гаф 4π e a = 2π 13 ( 3.2 ) It is easy to see that the total charge on the plane is fodfe , as it should be . The total charge induced on an originally uncharged insulated conductor by other charges is , of ...
... charge e is given by σ = 1 гаф 4π e a = 2π 13 ( 3.2 ) It is easy to see that the total charge on the plane is fodfe , as it should be . The total charge induced on an originally uncharged insulated conductor by other charges is , of ...
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 |
Copyright | |
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Electrodynamics of Continuous Media: Volume 8 L D Landau,E.M. Lifshitz,L. P. Pitaevskii Snippet view - 1995 |
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 diffraction dipole direction discontinuity distance effect electric field electromagnetic electrons electrostatic ellipsoid entropy 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 self-inductance SOLUTION sphere suffixes superconducting surface symmetry tangential temperature theory thermodynamic potential tion uniform unit volume values variable velocity wave vector wire z-axis zero