## Course of theoretical physics: Electrodynemics of continuous media |

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Page 34

The electric field in

field in another class of substances, ... (6.2) Let us suppose that no charges are

brought into the

The electric field in

**dielectrics**WE SHALL now go on to consider a static electricfield in another class of substances, ... (6.2) Let us suppose that no charges are

brought into the

**dielectric**from outside, which is the most usual and important ...Page 36

The linear relation between them is therefore a simple proportionalityzi D = t~:E. (

7.1) The coefficient s is the permittivity or

constant of the substance and is a function of its thermodynamic state. As well as

the ...

The linear relation between them is therefore a simple proportionalityzi D = t~:E. (

7.1) The coefficient s is the permittivity or

**dielectric**penneabilit y or**dielectric**constant of the substance and is a function of its thermodynamic state. As well as

the ...

Page 456

Current (continued) in a moving conductor 217-22 steady (Ill) 8611'. magnetic

field of 107-13 superconductivity I82-5 surface I07 Curvilinear coordinates 452-3

Cylinder conducting 14, 15-16, 17, I12, 206-7

Current (continued) in a moving conductor 217-22 steady (Ill) 8611'. magnetic

field of 107-13 superconductivity I82-5 surface I07 Curvilinear coordinates 452-3

Cylinder conducting 14, 15-16, 17, I12, 206-7

**dielectric**40, 53 Debye relaxation ...### What people are saying - Write a review

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angle anisotropy anisotropy energy antiferromagnetic atoms axes axis body boundary conditions calculation charge circuit coefﬁcient coefficients components conductor constant coordinates corresponding cross-section crystal Curie point curl H deﬁned deﬁnition denote dependence derivatives determined dielectric diffraction direction discontinuity dissipation domains electric ﬁeld electromagnetic ﬁeld electrons ellipsoid energy ﬂux expression external ﬁeld external magnetic ﬁeld ferroelectric ferromagnet ﬁeld H ﬁnd ﬁnite ﬁrst ﬁrst term ﬂow ﬂuctuations ﬂuid formula free energy frequency function given gives grad Hence incident induction inﬁnite integral isotropic Landau theory layer linear magnetic ﬁeld magnetohydrodynamics magnetostriction magnitude medium normal obtain optical particle permittivity perpendicular perturbation phase plane polarization PROBLEM propagated properties pyroelectric quantities reﬂection refraction relation respect result rotation satisﬁed scattering shock wave signiﬁcance solution sphere superconducting surface symmetry tangential temperature tensor theory thermodynamic potential transition uniaxial upper half-plane values variable velocity volume wave vector z-axis zero