A wave field E incident on a 2-polarized short-dipole at the origin. The fields arrives from...

 

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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 = 0º direction. = 45° E = ( − 2)ej*(x+²)/√² V/m. 54 Short dipole E = (2-²)*(+)/√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 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 = 0º direction. = 45° E = ( − 2)ej*(x+²)/√² V/m. 54 Short dipole E = (2-²)*(+)/√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