This does not uniquely define either the unit vector \(\hat{\bf l}\) nor the scalar part \(l_e\), since a change in the definition of the former can be compensated by a change in the definition of the...This does not uniquely define either the unit vector \(\hat{\bf l}\) nor the scalar part \(l_e\), since a change in the definition of the former can be compensated by a change in the definition of the latter and vice-versa. The potential induced in a dipole is the co-polarized component of the incident electric field times a normalized integral of the transmit current distribution over the length of the dipole, times sine of the angle between the dipole axis and the direction of incidence.
This does not uniquely define either the unit vector \(\hat{\bf l}\) nor the scalar part \(l_e\), since a change in the definition of the former can be compensated by a change in the definition of the...This does not uniquely define either the unit vector \(\hat{\bf l}\) nor the scalar part \(l_e\), since a change in the definition of the former can be compensated by a change in the definition of the latter and vice-versa. The potential induced in a dipole is the co-polarized component of the incident electric field times a normalized integral of the transmit current distribution over the length of the dipole, times sine of the angle between the dipole axis and the direction of incidence.
