In: Physics
Not only are the electric and magnetic field waves in the far-field
traveling at the speed of light, but they always have a special
restricted orientation and proportional magnitudes,
,
which can be seen immediately from the Poynting
vector. The electric field, magnetic field, and direction of
wave propagation are all orthogonal, and the wave propagates in the
same direction as
.
Also, E and B far-fields
in free space, which as wave solutions depend primarily on these
two Maxwell equations, are always in-phase with each other. This is
guaranteed since the generic wave solution is first order in both
space and time, and the curl
operator on one side of these equations results in first-order
spacial derivatives of the wave solution, while the time-derivative
on the other side of the equations, which gives the other field, is
first order in time, resulting in the same phase shift for both
fields in each mathematical operation.
From the viewpoint of an electromagnetic wave traveling forward, the electric field might be oscillating up and down, while the magnetic field oscillates right and left; but this picture can be rotated with the electric field oscillating right and left and the magnetic field oscillating down and up. This is a different solution that is traveling in the same direction. This arbitrariness in the orientation with respect to propagation direction is known as polarization. On a quantum level, it is described as photon polarization. The direction of the polarization is defined as the direction of the electric field.