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Learn about the far field radiated power and superposition principle in antenna design using Hj Eq. I DL z r y j x theory. Explore how small changes impact big changes in linear media. Educated guesses and methods of moments explained.
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radiated power dipole antenna
Hj Eq I DL z r y j x
The teacher remembers some calculus.
Hj z 1 Eq I DL2 I DL1 q r 2 y j x x linear media ==> superposition holds
z r1 Eq q1 I DL1 r h q r2 h h q2 I DL2 linear media ==> superposition holds
h z r1 Eq q1 h I DL1 r q r2 q2 I DL2 small changes big changes
h z r1 Eq q1 h I DL1 r q r2 q2 I DL2
Hj z 1 Eq I DL1 q r 2 y j I DL2 x x linear media ==> superposition holds
z r1 Eq q1 I DL1 r h q r2 h h q2 I DL2 linear media ==> superposition holds
h z r1 Eq q1 h I DL2 I DL1 r q r2 q2 small changes big changes
h z r1 Eq q1 h I DL2 I DL1 r q r2 q2
educated guess list What is this? far field
educated guess list I(z) confined to length of antenna h Imaxat z = 0 Integrable function
q q’ r r’ z’ z method of moments can be used
nonuniform current antenna arrays
z q r
even function
z r1 Eq q1 I(0) DL1 r h q phase r2 h q2 I()DL2 phased array
r1 z Eq q1 r I(0) DL1 h q small changes h r2 q2 I()DL2 phased array
Movie to illustrate the radiation pattern of a phased array antenna – mpg movie.
x =