Interakce s tercem.pdf - FBMI

Interakce s tercem.pdf - FBMI Interakce s tercem.pdf - FBMI

11.10.2013 Views

OBJEMOVÁ POLARIZACE The bulk polarization, P, of a material is the vector sum of the dipole moments, μ i, of individual molecules per unit volume. 1 N P mi aE V V The polarizability, α, of the material can be written in terms of the electric susceptibility, χ, and the permittivity of vacuum, ε 0, and the relative permittivity of the material, ε r . ( ) a e e e - 0 0 r 1 Thus, the polarization of the material can be modeled as. 0 ( 1) Pe e - E r E P The greater the polarization, the greater the interaction between the impinging light and the material.

n = c vakuu / c materiál = = c o / c materiál c vakuum lvacuum n λ vakuu INDEX LOMU f materiál = c mat / l (c vakuu / n) / (l vakuu / n) = f vakuu n c 0 n l vakuum/n l c / f c vakuum λ vakuu

OBJEMOVÁ POLARIZACE<br />

The bulk polarization, P, of a material is the<br />

vector sum of the dipole moments, μ i, of<br />

individual molecules per unit volume.<br />

1 N<br />

P mi<br />

aE<br />

V V<br />

The polarizability, α, of the material can be<br />

written in terms of the electric susceptibility,<br />

χ, and the permittivity of vacuum, ε 0, and the<br />

relative permittivity of the material, ε r .<br />

( )<br />

a e e e -<br />

0 0 r 1<br />

Thus, the polarization of the material can be<br />

modeled as.<br />

0<br />

( 1)<br />

Pe e - E<br />

r<br />

E P<br />

The greater the polarization,<br />

the greater the interaction<br />

between the impinging light and<br />

the material.

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