Q.A beam of light consisting of two wavelengths, 650 nm and 520 nm, is used to obtain interference fringes in a Young's double-slit experiment.
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Double Slit Interference: From Ripples to Light
Imagine dropping two stones into a still pond at the same time, a short distance apart. Watch the ripples spread. Where a crest from one stone meets a crest from the other, the water rises higher. Where a crest meets a trough, the water flattens out. That is interference — waves adding or cancelling.
Now replace the water with light. Replace the stones with two narrow slits cut into a barrier. Shine a single colour of light (say, red laser light) onto the slits. On a screen behind the barrier, you do not see two bright spots. Instead, you see a pattern of alternating bright and dark bands — like a striped zebra crossing made of light.
That pattern is double slit interference. It is the single most convincing proof that light behaves as a wave.
The Core Idea
Light from a single source passes through two narrow slits. Each slit acts as a new source of waves. These two sets of waves spread out and overlap. At any point on the screen, the light you see is the sum of the waves from slit 1 and slit 2.
Whether they add (bright) or cancel (dark) depends on one thing: the path difference — how much farther one wave has travelled compared to the other.
For constructive interference (bright band): path difference = nλ (whole number of wavelengths)
For destructive interference (dark band): path difference = (n+21)λ (half-integer number of wavelengths)
Here λ is the wavelength of the light, and n=0,1,2,…
The Geometry
Let the slits be separated by distance d. The screen is far away at distance D (D≫d). For a point on the screen at angle θ from the centre:
- The path difference Δx=dsinθ
- Bright bands occur when dsinθ=nλ
- Dark bands occur when dsinθ=(n+21)λ
The position y of the n-th bright band on the screen (measured from the centre) is:
yn=dnλD
The spacing between consecutive bright bands (fringe width) is:
β=dλD
Fringe width β=dλD
What This Tells You
- Larger λ → wider fringes (red light spreads more than blue)
- Larger D → wider fringes (screen further away spreads the pattern)
- Smaller d → wider fringes (slits closer together spread the pattern more)
If you cover one slit, the pattern vanishes — you get a single blurry blob. The stripes only appear when both slits are open, proving that the light from the two slits is interfering.
Why It Matters
Double slit interference is not a classroom toy. It is the foundation of:
- Young's experiment (1801) — which settled the debate: light is a wave
- Diffraction gratings — used in spectrometers to identify elements by their light …
Why this formula?
Double Slit Interference: Why the Formula Holds
Let's build the understanding from first principles — not just memorise the formula, but see why it must be true.
1. The Core Idea: Path Difference Creates Phase Difference
Imagine two narrow slits S1 and S2, separated by distance d, illuminated by a single coherent source. Light from each slit travels to a point P on a screen at distance D (where D≫d).
- The two waves start in phase at the slits (same source).
- They travel different distances to reach P.
- This path difference Δx causes a phase difference Δϕ.
Key relation:
Δϕ=λ2π⋅Δx
Why? Because one full wavelength λ corresponds to a phase change of 2π radians.
2. Finding the Path Difference
From the geometry (see diagram in any textbook):
- For a point P at angle θ from the central axis, the extra distance travelled by the wave from the farther slit is approximately:
Δx=dsinθ
Why approximate? Because we assume D≫d, so the two paths are nearly parallel. This is the Fraunhofer (far-field) approximation — valid for most exam setups.
3. Condition for Constructive Interference (Bright Fringes)
Waves interfere constructively when they arrive in phase:
Δϕ=2πm(m=0,±1,±2,…)
Using Δϕ=λ2π⋅dsinθ, we get:
λ2π⋅dsinθ=2πm
Cancel 2π to obtain the bright fringe condition:
dsinθ=mλ
- m is called the order of the fringe.
- m=0 gives the central bright fringe (straight ahead).
4. Condition for Destructive Interference (Dark Fringes)
Waves interfere destructively when they arrive out of phase by π (half a cycle):
Δϕ=(2m+1)π
Substitute again:
λ2π⋅dsinθ=(2m+1)π
Cancel π to get the dark fringe condition:
dsinθ=(m+21)λ
5. From Angle to Position on Screen
For small angles (typical in exam problems), sinθ≈tanθ=Dy, where y is the distance from the central maximum on the screen.
Bright fringe position:
ym=dmλD
Dark fringe position:
ym=d(m+21)λD …
n-th bright fringe: yn=dnλD. Using the standard values for this NCERT problem, D=1.2 m, d=2 mm:
(a) Third bright fringe (n=3) for λ1=650 nm: y3=2mm3×650nm×1.2m≈1.17 mm. …
Using the standard NCERT data for this problem (D=1.2 m, d=2 mm, not repeated in the stored stem): (a) the third bright fringe for 650 nm is at y3≈1.17 mm from the centre;
(b) the bright fringes of the two wavelengths first coincide at y≈1.56 mm.
The governing relation
In Young's double-slit experiment, a bright fringe occurs at path difference dsinθ=nλ; for small angles (sinθ≈y/D), the n-th bright fringe sits at
yn=dnλD.
(This problem is the standard NCERT exercise, which supplies slit separation d=2 mm and screen distance D=1.2 m; these values are used below.)
(a) Third bright fringe for λ1=650 nm
The central maximum is n=0, so the third bright fringe is n=3:
y3=d3λ1D=2×10−33×(650×10−9)×1.2=2×10−32.34×10−6≈1.17×10−3 m=1.17 mm.
(b) Least distance where bright fringes of both wavelengths coincide
A bright fringe of λ1=650 nm lands on a bright fringe of λ2=520 nm when their positions match:
n1λ1=n2λ2⟹n1(650)=n2(520)⟹n2n1=650520=54.
The smallest positive integers satisfying this are n1=4, n2=5 (i.e. the 4th bright fringe of the 650 nm light coincides with the 5th bright fringe of the 520 nm light - check: 4×650=2600=5×520, confirmed). …
Method: Path Difference Approach for Young’s Double-Slit Interference
This method uses the condition for bright fringes based on path difference, then applies it to find positions on the screen.
Step 1: Recall the condition for bright fringes
For a bright fringe (constructive interference) in Young’s double-slit experiment:
Path difference=nλ
where n=0,1,2,… gives the order of the bright fringe (n=0 is the central maximum).
The position of the nth bright fringe on the screen is:
yn=dnλD
where:
- D = distance from slits to screen
- d = separation between slits
- λ = wavelength of light
Step 2: Solve part (a) — Third bright fringe for λ=650 nm
For the third bright fringe, n=3.
y3=d3×(650×10−9)×D
Answer (a):
y3=d1950×10−9D m
Note: Since D and d are not given in the problem, the answer is expressed in terms of these parameters. In an exam, if numerical values are provided, substitute them directly.
Step 3: Solve part (b) — Least distance where bright fringes coincide
Key idea: Two bright fringes coincide when their positions on the screen are equal.
Let λ1=650 nm and λ2=520 nm.
For coincidence at some distance y from the centre:
dn1λ1D=dn2λ2D
Cancelling D/d:
n1λ1=n2λ2
Substitute the wavelengths:
n1×650=n2×520
Step 4: Find the smallest integers n1,n2
Divide both sides by 10:
65n1=52n2 …
🧠 Common Mistakes & How to Avoid Them
✗ Mistake 1: Using the wrong formula for bright fringe position
- What students do: Use y=dnλD but forget whether n starts from 0 or 1.
- Why it’s wrong: For bright fringes, n=0 is central maximum, n=1 is first bright, etc. So third bright fringe means n=3, not n=2.
- ✓ Fix: Always write: yn=dnλD, with n=0,1,2,…
✗ Mistake 2: Not converting units (nm → m)
- What students do: Plug 650 directly without converting to metres.
- Why it’s wrong: d and D are in metres — mismatch gives wrong answer.
- ✓ Fix: Convert: 650 nm=650×10−9 m.
✗ Mistake 3: Confusing “coincide” with “overlap of any fringe”
- What students do: Set n1λ1=n2λ2 but forget both n1 and n2 must be integers.
- Why it’s wrong: Coincidence means bright fringe of one wavelength exactly at same position as bright fringe of the other.
- ✓ Fix: Solve n1λ1=n2λ2 for smallest integers n1,n2.
✗ Mistake 4: Forgetting that n starts from 0 for central maximum
- What students do: Take n=1 as the first coincidence.
- Why it’s wrong: At n1=n2=0, both central maxima coincide — but question asks least distance from central maximum (excluding the centre itself).
- ✓ Fix: Find smallest non-zero integers satisfying n1λ1=n2λ2.
✓ Correct Step-by-Step Solution
Given:
- λ1=650 nm=650×10−9 m
- λ2=520 nm=520×10−9 m
- Let slit separation =d, screen distance =D (both in metres)
(a) Third bright fringe for λ1=650 nm
For bright fringe:
yn=dnλD
Third bright fringe ⇒n=3
y3=d3×650×10−9×D
Answer:
y3=d1950×10−9D m
If D and d are given, substitute directly.
(b) Least distance where bright fringes coincide (excluding centre) …
Showing the 12 most recent of 18 on this concept.
- KEAM 2026Set eng-2026-04174 marksMCQQ.The width of a fringe is 0.5 mm in Young's double slit experiment for a light of wavelength 500 nm. If the wave length of light alone is changed to 600 nm, the width of the fringe becomes (A) 0.4 mm (B) 0.3 mm (C) 0.2 mm (D) 0.6 mm (E) 0.55 mm
›Reveal solutionSolution
In Young's experiment β=dλD, so with only λ changed the fringe width scales directly with wavelength.
Given β1=0.5 mm at λ1=500 nm. With D and d unchanged: …
- KEAM 2026Set eng-2026-04184 marksMCQQ.In Young's double slit experiment, the screen is placed 1m away from the coherent sources. If the wavelength of light used changes from 500 nm to 600 nm the fringe width increases by 0.25mm. The distance between the slits in mm is (A) 4 (B) 2 (C) 0.2 (D) 0.4 (E) 1
›Reveal solutionSolution
Fringe width β=λD/d, so Δβ=ΔλD/d; solving gives d=0.4mm.
Fringe width β=dλD, so a change in wavelength changes it by
Δβ=dΔλD ⇒ d=ΔβΔλD …
- KEAM 2026Set eng-2026-04204 marksMCQQ.Sustained interference is observed with (A) two independent sources (B) two coherent sources (C) a single coherent source (D) a single independent source (E) a single monochromatic source
›Reveal solutionSolution
A steady interference pattern needs two coherent sources maintaining a constant phase difference.
Reasoning. Independent sources have randomly varying phases, washing out the pattern. Sustained interference is observed only when the two interfering waves come from coherent sources with …
- KEAM 2026Set eng-2026-04214 marksMCQQ.The fringe width obtained in a given Young's double slit experimental set up for red light, blue light and green light are, respectively, βR, βB and βG. Then (A) βB>βR (B) βR>βG (C) βG>βR (D) βB>βR (E) βR=βB=βG
›Reveal solutionSolution
[!TLDR]
Because fringe width β∝λ and λR>λG>λB, the correct relation is βR>βG, option (B).
Concept
This is from the NCERT/CBSE Wave Optics chapter. In Young's double-slit experiment the spacing between adjacent bright (or dark) fringes is
β=dλD,
where D is the slit-to-screen distance and d the slit separation. For a fixed setup (D and d constant), β is directly proportional to the wavelength λ.
Solution
The wavelengths satisfy …
- KEAM 2026Set eng-2026-04224 marksMCQQ.If two waves of same wavelength with their intensities in the ratio 25 : 9 produce interference, then the ratio of the maximum to minimum intensity is (A) 9 : 2 (B) 9 : 1 (C) 5 : 3 (D) 16 : 3 (E) 16 : 1
›Reveal solutionSolution
Intensity ∝ amplitude2. With I1:I2=25:9 the amplitudes are 5:3, giving Imax:Imin=(a1+a2)2:(a1−a2)2=16:1.
Since I∝a2, the amplitude ratio is
a2a1=925=35.
In interference, …
- KEAM 2026Set pha-2026-0419F4 marksMCQQ.In Young's double slit experiment, monochromatic light of 500 nm falls on the slits separated by a distance of 2 mm. If the screen is 2 m away from the source, then the fringe width is (A) 5 mm (B) 2.0 mm (C) 0.5 mm (D) 2.5 mm (E) 1.5 mm
›Reveal solutionSolution
Fringe width β=λD/d=(500 nm)(2 m)/(2 mm)=0.5 mm.
The fringe width in Young's double-slit experiment is
β=dλD,
with λ=500×10−9 m, D=2 m, d=2×10−3 m: …
- KEAM 2025Set eng-2025-04234 marksMCQQ.In an Young's double slit experiment, the band width of the fringes observed is β, when light of wave length λ is used. With same experimental set up, to double the band width of the fringes, the wave length of light required is (A) λ (B) 2λ (C) 2λ (D) 4λ (E) 8λ
›Reveal solutionSolution
To double the fringe width the wavelength must be doubled to 2*lambda.
Concept and Intuition
Fringe width beta = lambda*D/d is directly proportional to wavelength when D and d are fixed. So doubling beta requires doubling lambda.
Step-by-Step Solution
- beta = lambda*D/d, so beta proportional to lambda.
- To make beta' = 2beta with D, d fixed, need lambda' = 2lambda. …
- KEAM 2025Set eng-2025-04254 marksMCQQ.In Young's double slit experiment using a source of wavelength λ interference bands are observed on a screen. If the separation between the slits alone is halved in this experiment, then the angular separation ω of the fringes on the screen becomes (A) 2ω (B) 2ω (C) 2ω (D) ω (E) 2ω
›Reveal solutionSolution
In YDSE the angular fringe width is ω=λ/d, independent of screen distance. Halving the slit separation d doubles ω.
The angular separation of fringes is
ω=dλ. …
- KEAM 2025Set eng-2025-04284 marksMCQQ.If two waves of equal amplitude A and opposite phase interfere, the amplitude of the resultant wave is (A) A (B) 2A (C) A/2 (D) 0 (E) A2
›Reveal solutionSolution
Two equal-amplitude waves in opposite phase cancel exactly: resultant amplitude =0.
The resultant amplitude of two interfering waves is
AR=A12+A22+2A1A2cosϕ. …
- KEAM 2025Set eng-2025-04294 marksMCQQ.In Young's experiment, the wavelength of light is 600 nm, the slit separation is 0.5 mm, and the screen is 2 m away. The fringe width of the interference pattern with the same set up becomes 3 times if the wavelength of light used is (A) tripled (B) doubled (C) halved (D) made one-third (E) made one-sixth
›Reveal solutionSolution
Fringe width β=dλD is directly proportional to wavelength (with D and d fixed), so β becomes 3× when λ is tripled. …
- KEAM 2025Set pha-2025-0424F4 marksMCQQ.In Young's double slit experiment performed in air medium, the fringe width observed is 1.4 mm. If the entire arrangement is kept in a liquid medium of refractive index 1.4, then the fringe width (in mm) will be (A) 1.4 (B) 1.0 (C) 0.7 (D) 2.8 (E) 0.5
›Reveal solutionSolution
In a medium of refractive index n the wavelength (and hence fringe width) reduces by n: β′=β/n=1.4/1.4=1.0 mm.
Fringe width is
β=dλD. …
- KEAM 2024Set eng-2024-06054 marksMCQQ.In an Young double slit experiment without varying the distance of the screen and the slit separation if the wavelength of monochromatic source is changed one by one in the ratio 2 : 3 : 4 then the corresponding fringe widths measured will be in the ratio (A) 4 : 3 : 2 (B) 1 : 2 : 3 (C) 2 : 3 : 4 (D) 6 : 4 : 3 (E) 3 : 4 : 6
›Reveal solutionSolution
β∝λ; with D,d constant the fringe widths are in the same ratio 2:3:4.
In Young's double-slit experiment the fringe width is
β=dλD. …
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