An infinitesimal electric dipole of length l and constant current /, is placed along the xz-plane and symmetrically about the origin, but oriented 45° from the x-axis (as shown below). Drive the electric field (E,, Eg, E4) radiated by the dipole. Also, compute the time-average power density radiated by the dipole. A, (sin 0 cos sin 0 sin ø cos 0 Ag = ( cos0 cos cos 0 sin o -sin 0 ) Ay cos o - sin o Az 45°

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An infinitesimal electric dipole of length l and constant current l, is placed along the xz-plane
and symmetrically about the origin, but oriented 45° from the x-axis (as shown below). Drive
the electric field (E,, Eg, E4) radiated by the dipole. Also, compute the time-average power
density radiated by the dipole.
(sin0 cos sin 0 sin cos e
= ( cos 0 cos o cos 0 sin o -sin e A,
- sin o
(A,
Ag
A
cos o
\42)
45°
Transcribed Image Text:An infinitesimal electric dipole of length l and constant current l, is placed along the xz-plane and symmetrically about the origin, but oriented 45° from the x-axis (as shown below). Drive the electric field (E,, Eg, E4) radiated by the dipole. Also, compute the time-average power density radiated by the dipole. (sin0 cos sin 0 sin cos e = ( cos 0 cos o cos 0 sin o -sin e A, - sin o (A, Ag A cos o \42) 45°
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