Magnetic field polarization
Radiofrequency waves in lossy media Inductive effects through a cylindrical body

Let's now consider the wave inside the cylinder presented in the dual polarization of the previous one, where the electric field E_z is matched by a magnetic field H_z. By duality, the angular magnetic field H_φ is also matched by the angular electric field E_φ. The calculations presented in this paragraph endeavor to show that the current configuration of fields inside the cylinder can only be achieved in the presence of an inducing magnetic field H_zi parallel to the cylinder axis. It follows from these properties that the cylinder shown in figure 6 reproduces magnetic polarization. The diagram contains all the physical and geometric data required to calculate the H_z(ρ) and E_φ(ρ) functions in the following...