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radiated power dipole antenna. H j. E q. I D L. z. . r. y. j. x. far field. far field. The teacher remembers some calculus. H j. z. 1. E q. I D L 2. I D L 1. q. r. 2. y. j. x. x. linear media ==> superposition holds. z. r 1. E q. q 1. I D L 1. r. h. q.
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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 =