A beam of unpolarised light of intensity \( I_0 \) is passed through a polaroid A and then through another polaroid B which is oriented so that its principal plane makes an angle of 45° relative to that of A. The intensity of emergent light is:
\(\frac{I_0}{2}\)
\(\frac{I_0}{2\sqrt2}\)
\(\frac{I_0}{4}\)
\(\frac{I_0}{8}\)
When unpolarised light passes through a polaroid, the intensity of the transmitted light \( I \) is given by:
\[ I = \frac{I_0}{2}, \]
where \( I_0 \) is the intensity of the incident unpolarised light.
Passing through Polaroid A: After passing through polaroid A, the intensity becomes:
\[ I_A = \frac{I_0}{2}. \]
Passing through Polaroid B: When the light passes through the second polaroid B at an angle \( \theta = 45^\circ \) relative to the first:
\[ I_B = I_A \cos^2(45^\circ) = \left( \frac{I_0}{2} \right) \cos^2(45^\circ). \]
Since \( \cos(45^\circ) = \frac{1}{\sqrt{2}} \):
\[ I_B = \left( \frac{I_0}{2} \right) \left( \frac{1}{\sqrt{2}} \right)^2 = \left( \frac{I_0}{2} \right) \left( \frac{1}{2} \right) = \frac{I_0}{4}. \]
Thus, the intensity of emergent light after passing through both polaroids is:
\[ \frac{I_0}{4}. \]
A body of mass 1000 kg is moving horizontally with a velocity of 6 m/s. If 200 kg extra mass is added, the final velocity (in m/s) is:
Light travels in form of transverse EM waves. The underlying oscillation is along directions perpendicular to the propagation direction, in this example, oscillating electric and magnetic fields. Process of restricting the vibration of light waves to one direction is known as Polarisation.
There are three types of polarisation such as:
The few methods of polarisation of Light are: