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...


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

Extracted 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°

Jun 10, 2022
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