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EM Scattering Homework assignment 1

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0<br />

<br />

h<br />

z<br />

2a<br />

y<br />

kˆ<br />

i<br />

z ˆ<br />

x<br />

0<br />

E<br />

i<br />

E ˆ 0<br />

x<br />

Problem 3:<br />

E r E exp 0<br />

ki<br />

r where k<br />

i<br />

is the<br />

i<br />

i<br />

Consider a plane wave traveling in free space with j <br />

incident wave vector with k<br />

i<br />

k 00<br />

. The wave is incident upon a certain dielectric<br />

object of arbitrary shape with a dielectric constant<br />

r generating equivalent currents inside<br />

the object. Let E , H denote the scattered field, i.e., the field induced by these equivalent<br />

s<br />

s<br />

currents. In the far field zone the scattered electric field is given by:<br />

Where,<br />

ˆs<br />

<br />

f<br />

exp jkr<br />

E ( ) <br />

ˆ , ˆ<br />

s<br />

r Q<br />

<br />

k<br />

s<br />

k<br />

i<br />

r<br />

k denotes the direction of scattering and <br />

ˆ ˆ<br />

s<br />

,<br />

i <br />

<br />

<br />

Q k k is the vector scattering amplitude<br />

(see the powerpoint slides for a description). Using the reciprocity theorem of electromagnetic<br />

theory show that<br />

i<br />

<br />

ˆ ˆ k<br />

<br />

i<br />

E0 Q , ˆ<br />

<br />

ki ki E0<br />

<br />

s <br />

exp j<br />

i<br />

dS<br />

<br />

4<br />

j<br />

<br />

n E r k r<br />

S<br />

i<br />

0<br />

<br />

ˆ exp j <br />

H H r n k r<br />

<br />

dS<br />

<br />

s i <br />

S

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