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Generalized Lorentz-Lorenz law

The dimension of the problem can be reduced by using the properties of determinants and the final result is [Pg.159]

In the low frequency limit, the size of the particle is considered to be very small compared to the incident wavelength. It is then sufficient to take only the lowest-order coefficients in the fields expansions, and in this limit, the elements of the T matrix can be obtained in closed form for simple shapes. For spherical particles, we have [Pg.159]

As a result, the long-wavelength equation for the effective wave number takes the form [Pg.160]

For an ensemble of spheres of radius R and small fractional concentrations c, [Pg.160]


See other pages where Generalized Lorentz-Lorenz law is mentioned: [Pg.150]    [Pg.158]    [Pg.159]    [Pg.159]    [Pg.150]    [Pg.158]    [Pg.159]    [Pg.159]    [Pg.15]   
See also in sourсe #XX -- [ Pg.158 ]




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