A wave field E incident on a 2-polarized short-dipole at the origin. The fields arrives from 0 = 45 and = 0 direction, and, therefore, the available power at the dipole will be proportional to A(45)=G(45). Unit vector i describes the polarization of the field the dipole would radiate in and = 0 direction. = 45 E = ( 2)ej*(x+)/ V/m. 54 Short dipole E = (2-)*(+)/ The power received P, by the short-dipole in mW is: (a) 0.4 (b) 0.5 (c) 0.6 (d) 0.7 (e) None of the above