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a) Show that the Maxwell Garnett mixing formula for metallic inclusions (i

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Applications of electrodynamics, spring 2005

Exercise 4(Thursday 17.2., return answers until 16:00 on Monday 14.2.) 1. Determine the polarization and the total cross section of a perfectly con-

ducting sphere whose radius is much smaller than the wavelength of the incident electromagnetic field.

2. a) Show that the Maxwell Garnett mixing formula for metallic inclusions (i → ∞) is

ef f =h

1 + 2f 1−f

b) The Maxwell Garnett formula is accurate at low volume fractions f. One attempt to improve its validity at larger f is to consider the following iterative process:

i) Start with a uniform host material of volume V0 and permittivity h. ii) Add a small amount ∆V V0 of metallic spheres and calculate the effective permittivity of this mixture.

iii) Consider the medium of the previous step as a uniform host material and add again inclusions of an amount ∆V. Continue this procedure several times.

Show that after N iterations ef f =h

N

Y

n=1

1 + V 2∆V

0+n∆V

1− V0+n∆V∆V

Show that at the limit N → ∞

ef f = h (1−f)3

There is experimental evidence that this result is fairly accurate at least for 0≤f ≤0.5.

(2)

3. Above a uniform earth, there is a horizontal electric dipole whose current density is J(r, t) = ILδ(x)δ(y)δ(z −h)e−iωtex. The electromagnetic pa- rameters of the air are µ0, 0, σ0 and in the earth µ1, 1, σ1. The earth’s surface is the xy-plane.

a) Show that the vector potential can be expressed as Ax0 = C

Z 0 db b

K0

(e−K0|z−h|+R(b)e−K0(z+h))J0(bρ), z > 0 Az0 = C ∂

∂x

Z

0 db S(b)e−K0(z+h)J0(bρ), z > 0 Ax1 = C

Z

0 db P(b)eK1zJ0(bρ), z < 0 Az1 = C ∂

∂x

Z

0 db Q(b)eK1J0(bρ), z <0 where C is a constant to be determined later and

K =√

b2−k2, ρ=qx2+y2 b) Express B and E using only the vector potential.

c) Apply boundary conditions to solve P, Q, R, S.

d) Construct a line current of amplitude I of successive dipoles. Calculate Ax1 and Az1 (set µ1o).

e) Calculate B1 for a line current. Determine the constant C by studying a time-independent current.

Reminder: there is still time to consider the extra problem no. 5 of exercise 3.

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