Evaluate the time-average Poynting vector, = (12) Re {E s à H s } for the Hertzian dipole, assuming the general case that involves the

Evaluate the time-average Poynting vector, = (12) Re {E_s× H^ˆ—_s} for the Hertzian dipole, assuming the general case that involves the field components as given by Eqs. (10), (13a), and (13b). Compare your result to the far-zone case, Eq. (26).

Eqs. (10)

Eqs. (13a)

Eqs. (13b)

Eqs. (26)

 

Iod Has r2 sin e e-jkr 4 n cos 0 ejkr r2 Ers Iod jkr3 ||