Linear Polarization of Light: light is a transverse wave, and
therefore it may exhibit two different polarizations.
On the Youtube clips you saw that waves of two different
polarizations can be excited on a rope.
The flash animation showed how a simple “polarizer”, or
a “polarizing filter” of rope waves works: if the rope passes
through a slit, only waves with polarization parallel to the
slit can get through, while waves of perpendicular polariza-
tion cannot. Below, there is another illustration of how such
simple “polarizing filter” works:
Light is an electromagnetic wave. There is no “displacement” that
oscillates and travels forward as in the case of all mechanical wa-
ves. The oscillating things here are the electric and the magnetic
field. They oscillate in planes that are perpendicular to each other.
So, what is the polarization of the EM wave shown below?
We have to choose one of
the fields as the one that
defines the polarization
direction. By convention,
this is the electric field vector.
Because we say that “there is much analogy between the polarization
ff light waves and the polarization of waves on ropes”, students may
get the impression that slits, or arrays of many parallel slits can
also be used as polarizers of light. Such an impression may be
even strengthened by the fact that an often used graphic symbol
of a light polarizer has the form of a circle or a square filled
with many parallel lines (see the example below).
Remenber, this is a totally wrong
thinking! Slits, even very narrow,
DO NOT ACT AS LIGHT POLA-
RIZERS!
The lines on the graphs do not
symbolize an array of slits –
they only indicate the polari-
zation of the light waves that
get through the polarizer.
If not slits, what’s used for polarizing light? We’ll discuss three methods:
The most popular polarizer type is polarizing foil. It was pioneered by the
well-known Polaroid company, and therefore its often called “polaroid”.
How it works? Here is the explanation (perhaps slightly oversimplified):
The incident unpolarized beam is first “organized” by the molecular stru-
cture of the foil into two waves of perpendicular polarization – and
then the same molecules absorb
(almost completely) one
of them, while the other
gets through.
Exercise: hold one polaroid in front of your
eye. Look at a light source. Put another piece of foil in front of the first one, and
turn it at various angles.
Another nice picture explaining how polarizing foil works:
BTW, the direction
along which light is
polarized by a given
device is called the
“polarizing axis”, or
“polarization axis”
of the device.
This is what
you should
see…
…and here is the
explanation, which
is quite straightforward, right?
A considerable advantage of foil polarizers
is that they are inexpensive – so they are widely used!
Two. Polarization by reflection: the reflected and refracted waves are always
partially polarized.
But in the special case
when the angle between
the reflected and the
refracted beam is
exactly 90º (see be-
low), the reflected
wave is totally
polarized, parallel
to the reflecting
surface.
Let’s find the condition for the reflected
and refracted ray being perpendicular:
p 90 b 180
So : b 90 p
b 90 p
Then : sin b sin 90 p
But : sin(90 ) cos
( trigonomet ric identity)
So : sin b cos p
sin p
Now, recall the Snell' s Law : n This is the con-
sin b
dition for the
reflected wave
And insert what we got for sin b :
to be 100% po-
larized. The
sin p sin p
incident angle
tan p n
satisfying this
sin b cos p
condition is
called the
Brewster Angle.
Because of the “inconvenient geometry” – the polarized wave
does not travel along the same direction as the incident wave --
polarization by reflection is not very often used in practical
devices, even though it is perhaps the least expensive method!
However, in its own right polarization by reflection is an
important phenomenon. For instance, sometimes it helps
to eliminate unwanted or troublesome light reflections.
We will return to that shortly.
Three: polarization by the effect of birefringence.
Some crystals have the peculiar property, called birefringence:
A light ray incident on a birefringent
material is split into two beams,
called the ordinary (o ray) and
extraordinary ray (e ray), that
have mutually perpendicular
polarizations.
Calcite (a crystalline form of CaCO3)
is transparent, completely colorless,
and exhibits unusually strong
birefringence properties.
(calcite crystals will
be now passed around).
The so-called “Nicol prism”. It is made of two pieces of calcite
with a gap between, filled with “Canada Balsam” (a transparent
glue). Due to the different refractive indices of the ordinary and
the extraordinary waves, the ordinary undergoes a total internal
reflection and is removed from the prism, while the extraordinary
gets through.
The Nicol Prism is an extremely efficient polarizer, but very expensive.
Therefore, it is used only in apparatus in which high precision is crucial.
OK, over with the methods of polarizing light!
Now, a mini-problem, and then a practical exercise:
Suppose that you have two polarizers, but the direction of the
Polarizing axis is not marked on any of them.
HOW TO FIND THE POLARIZING
AXIS DIRECTION?
It is not difficult to find situations in which the polarizing axes
are parallel, or are crossed…
...but it still does not tell us what their exact orientation is:
? ? ?
What happens if the polarizing axes are neither parallel,
nor crossed, but they make an arbitrary angle θ ?
What is the intensity of the wave transmitted by the second?
(in such configuration, we call the first “polarizer”, but the
second is now the “analyzer”).
Recipe: the amplitude of a wave can be thought of as
a vector.
Let’s denote the amplitude after the polarizer as E.
Now, " decompose" the E vector into a
component parallel to the analyser's axis :
Epar E cos This one can go!
(green light)
and a component perpendicular to it :
This one is stopped!
Eperp E sin (red light)
What we register by eyes, or using photodetectors,
is the light intensity, which is proportional to the
square of the amplitude.
Intensity before the analyzer : I E 2
Intensity after the analyzer : I E cos E 2 cos 2
2
So, the intensity transmission coefficien t is :
I E 2 cos 2
T cos 2
I E 2
Optically active media:
Some materials and compounds have the ability of
“twisting” the polarization direction of light passing
by them. We call them “optically active”:
Saccharimetry – one of the many practical applications
of measurements of the polarization axis rotation.
One of the best known examples of optically active media
is water solution of ordinary sugar (demo).
By measuring of how much the polarization direction is rotated by a
sample of sugar-containing fluid, one can determine the sugar con-
centration in it. This method is widely used in medical analysis for
checking the sugar content in blood, urine and other body fluids.
