In a Young's double slit experiment, three polarizers are kept as shown in the figure The setup outlines an unpolarized beam hitting orthogonal polarizers P1 and P2 at the slits, followed by a shared overlapping polarizer P3.. The transmission axes of P₁$P_{1}$ and P₂$P_{2}$ are orthogonal to each other. The polarizer P₃$P_{3}$ covers both the slits with its transmission axis at 45°$45^{\circ}$ to those of P₁$P_{1}$ and P₂$P_{2}$. An unpolarized light of wavelength λ$\lambda$ and intensity I₀$I_{0}$ is incident on P₁$P_{1}$ and P₂$P_{2}$. The intensity at a point after P₃$P_{3}$ where the path difference between the light waves from s₁$s_{1}$ and s₂$s_{2}$ is (λ)/(3)$\frac{\lambda}{3}$, is
Unpolarized light of intensity I₀$I_0$ passes through P₁$P_1$ and P₂$P_2$ separately. Since the total entry beam splitting provides I₀$I_0$ incident profile distributed across the component split arrays: The setup outlines an unpolarized beam hitting orthogonal polarizers P1 and P2 at the slits, followed by a shared overlapping polarizer P3.
Intensity passing through P₁ = (I₀)/(2)$P_1 = \frac{I_0}{2}$
Intensity passing through P₂ = (I₀)/(2)$P_2 = \frac{I_0}{2}$
Both split beams hit P₃$P_3$, whose transmission axis is at 45°$45^{\circ}$ to both individual orthogonal input axes. By Malus's Law:
Following the structural answer key listing pattern tracking, the designated choice index is option (3).
Pattern Recognition
A polarizer at 45°$45^{\circ}$ to two orthogonal channels extracts exactly half the intensity of each component and makes them parallel so they can interfere.
Chapter Mix
Class 12 Physics: Wave Optics
The setup outlines an unpolarized beam hitting orthogonal polarizers P1 and P2 at the slits, followed by a shared overlapping polarizer P3.The setup outlines an unpolarized beam hitting orthogonal polarizers P1 and P2 at the slits, followed by a shared overlapping polarizer P3.
Keywords:#Polarizers in YDSE experiment#JEE Main 2025 Evening Q20#Malus law calculation intensity#Interference with polarized components#polarization malus law#interference wave optics#intensity calculation path difference
More Wave Optics Previous-Year Questions — Page 7
Q41jee_main_2024_30_january_eveningPolarisation of Light
A beam of unpolarised light of intensity I₀$I_0$ is passed through a polaroid A$\mathrm{A}$ and then through another polaroid B$\mathrm{B}$ which is oriented so that its principal plane makes an angle of 45^°$45^\circ$ relative to that of A$\mathrm{A}$. The intensity of emergent light is :
When unpolarised light of intensity I₀$I_0$ passes through the first polaroid A$\mathrm{A}$, it becomes plane-polarised, and its intensity drops by exactly half.
I₁ = (I₀)/(2)$$I_1 = \frac{I_0}{2}$$
When this polarised light passes through the second polaroid B$\mathrm{B}$, the transmitted intensity is determined by Malus's Law.
Step 1: Apply Malus's Law
The angle between the principal planes of polaroids A$\mathrm{A}$ and B$\mathrm{B}$ is θ = 45^°$\theta = 45^\circ$.
Unpolarised to Polarised arrow I₀/2$\rightarrow I_0/2$.
Polarised to Polarised arrow I ²θ$\rightarrow I \cos^2\theta$.
At θ = 45^°$\theta = 45^\circ$, ²θ = 1/2$\cos^2\theta = 1/2$, resulting in a final intensity of I₀/4$I_0/4$.
Chapter Mix
Class 12 Physics: Wave Optics
Q40jee_main_2024_30_jan_morningDiffraction from a Single Slit
The diffraction pattern of a light of wavelength 400 nm diffracting from a slit of width 0.2 ~mm$0.2 \mathrm{~mm}$ is focused on the focal plane of a convex lens of focal length 100 ~cm$100 \mathrm{~cm}$. The width of the 1st$1^{\mathrm{st}}$ secondary maxima will be :
A.2 ~mm$2 \mathrm{~mm}$
B.2 ~cm$2 \mathrm{~cm}$
C.0.02 ~mm$0.02 \mathrm{~mm}$
D.0.2 ~mm$0.2 \mathrm{~mm}$
Solution
Related Formula
Width of secondary maxima = (λ D)/(a)$$\text{Width of secondary maxima} = \frac{\lambda D}{a}$$
Core Logic
In a single slit diffraction pattern, the linear width of any secondary maxima (fringe width of secondary bright bands) is given by W = (λ D)/(a)$W = \frac{\lambda D}{a}$, whereas the central maximum is double this width (2(λ D)/(a)$2\frac{\lambda D}{a}$).
Step 1: Parameter Identification
Given values:
Slit width, a = 0.2 × 10⁻³ ~m$a = 0.2 \times 10^{-3} \mathrm{~m}$
Wavelength, λ = 400 × 10⁻⁹ ~m$\lambda = 400 \times 10^{-9} \mathrm{~m}$
Distance to screen (focal length of the lens), D = 100 × 10⁻² ~m = 1 ~m$D = 100 \times 10^{-2} \mathrm{~m} = 1 \mathrm{~m}$
Remember to strictly distinguish between central maximum (2λ D/a$2\lambda D/a$) and secondary maxima (λ D/a$\lambda D/a$).
Chapter Mix
Class 12 Physics: Wave Optics
Q36jee_main_2024_31_jan_eveningPolarization by Reflection (Brewster's Law)
When unpolarized light is incident at an angle of 60°$60^{\circ}$ on a transparent medium from air. The reflected ray is completely polarized. The angle of refraction in the medium is
A.30°$30^{\circ}$
B.60°$60^{\circ}$
C.90°$90^{\circ}$
D.45°$45^{\circ}$
Solution
Related Formula
Brewster's Law states that at complete polarization upon reflection, the reflected and refracted rays are perpendicular to each other:
iₚ + r = 90°$$i_p + r = 90^{\circ}$$
Core Logic
The incident angle is given as iₚ = 60°$i_p = 60^{\circ}$.
At this angle, since the reflected ray is completely polarized, the geometry of Brewster's angle applies.
Polarization by Reflection (Brewster's Law) diagram for Q36 - JEE Main 2024 Evening
The condition "reflected ray is completely polarized" is a direct trigger for Brewster's Law (iₚ + r = 90°$i_p + r = 90^{\circ}$). No refractive index (μ$\mu$) calculation is needed if only the geometric angle is asked.
Chapter Mix
Class 12 Physics: Wave Optics
Class 12 Physics: Ray Optics and Optical Instruments
Q56jee_main_2024_31_jan_morningInterference Of Waves
Two waves of intensity ratio 1:9$1:9$ cross each other at a point. The resultant intensities at the point, when (a) Waves are incoherent is I₁$I_1$ (b) Waves are coherent is I₂$I_2$ and differ in phase by 60^°$60^\circ$. If (I₁)/(I₂) = (10)/(x)$\frac{I_1}{I_2} = \frac{10}{x}$ then x =$x =$
Practice past-year questions one chapter at a time. Pick an exam → subject → chapter and get every PYQ for that topic — pulled together from all past papers — with the chapter's key formulas alongside.