WOLFRAM NOTEBOOK

WOLFRAM|DEMONSTRATIONS PROJECT

Polarization of an Electromagnetic Wave

E
x
2
E
y
2
Δφ
0
E
(x, y, z,
t
0
)
(
E
x
,
E
y
)
The polarization of an electromagnetic wave describes the orientation of the oscillating electric field. The wave is transverse and travels in the positive
z
direction. There is also a magnetic field in phase with the electric field and perpendicular to both the electric field and the direction of propagation. The electric field may be divided into two perpendicular components labeled
E
x
and
E
y
, such that
E
=
E
x
cos(kz-ωt)
x
+
E
y
cos(kz-ωt+Δφ)
y
, where
Δφ
is the phase difference between the two components. When
Δφ=0
or
Δφ=π
, the wave is said to be linearly polarized. If
Δφ=π/2
and
E
x
has the same magnitude as
E
y
, then the wave is said to be circularly polarized; in all other cases, the wave is elliptically polarized.
Wolfram Cloud

You are using a browser not supported by the Wolfram Cloud

Supported browsers include recent versions of Chrome, Edge, Firefox and Safari.


I understand and wish to continue anyway »

You are using a browser not supported by the Wolfram Cloud. Supported browsers include recent versions of Chrome, Edge, Firefox and Safari.