![]() |
VOOZH | about |
Malus Law, also known as Malus Law of Polarization, is a fundamental principle in optics that describes how the intensity of polarized light changes as it passes through a polarizer. It is named after Étienne-Louis Malus, a French physicist who formulated the law in 1808.
In this article, we will discuss the concept of Malus Law which describes the intensity of change in the intensity of polarized light.
Table of Content
According to Malus's rule, the square of the cosine of the angle formed between the polarizer's plane and the analyzer's transmission axes determines how much plane-polarized light changes in intensity as it passes through the device.
Malus's Law is significant in optics and helps in understanding how polarized sunglasses work, how stress patterns in transparent materials can be studied, and in various other applications where control of light polarization is required.
Étienne-Louis Malus was a mathematician, physicist, engineer, and commander from France. Malus was born in France's Paris. He served at the Institut d'Égypte's mathematics department and took part in Napoleon's invasion of Egypt.
Read More about Polarization of Light.
Malus noticed that when the crystal spun, the intensity changed from highest to minimum. Consequently, he suggested that A = A cosθ must be the amplitude of the reflected beam. Malus calculated the intensity by square-rooting the amplitude relation i.e. Io = Ao2.
I(θ) = Io cos2 θ
Where
This equation is known as Malus’s Law.
Assume the light source emits unpolarized light, which means the electric field vector oscillates randomly in all directions perpendicular to the direction of propagation.
When this light encounters a polarizing filter, the filter only allows the component of the electric field parallel to its polarization axis to pass through.
The electric field vector of the incoming light can be represented as = E0cos(ωt−kx) , where:
When the light hits the polarizer, the electric field vector can be decomposed into two components: parallel (E∥) and perpendicular (E⊥) to the axis of the polarizer. Since the perpendicular component is blocked, only E∥ passes through.
If θ is the angle between the light's initial polarization direction and the axis of the filter, the parallel component is given by E∥=E0cos(θ).
The intensity of light is proportional to the square of the amplitude of its electric field. If I0 is the intensity of the incident light, the intensity I of the transmitted light is proportional to E∥2.
Therefore, the intensity of the light after passing through the polarizer is I = Io cos2 θ.
According to Malus' law, the polarizer's angle affects how much-polarized light can flow through it.
Malus Law Experiment. The goals of this experiment are to determine the connection between the intensity of light passed through the analyzer and the angle '′ between the polarizer and analyzer axes. The following equipment was used: The following are the experiment's requirements: A laser diode.
To perform the experiment we can use the following setup and procedure for experiment.
In above mentioned experiment we can observe the following things.
Using these observations, we can calculate the value of required intensity.
There are some limitations of this law in real life:
Read More,
Ordinary (or unpolarized) light and plane polarized light vary in that the former oscillates in a single plane alone, while the latter has vibrations occurring inside it at random angles without any plane. Using an organic filter is another way to polarize light.
A light beam without polarization travels through two consecutive polaroid.
We are aware that the intensity of unpolarized light decreases to half as it travels through a Polaroid. In the event that it traverses any further polaroid, the intensity determined by Malus law .The angle θ in this case is between the polaroid's intensity variation axis and 0 to 2π. The curve is nothing (cos2 θ).
You must first measure the distance between the light source and the spot in order to determine the intensity of the light. Decide on the S.I. units for the distance.
For instance, the unit should be 0.56 m if the point of application is 56 cm from the light source.