Interference and Coherence · Vidya720
Physics · Class 12 Wave Optics · NEET

Interference, from a wedding sound check to I = 4I₀ cos²(φ/2)

A full lesson: a cartoon movie at a wedding hall, then superposition in a ripple tank, path and phase difference, the intensity formula built from two waves, why ordinary lamps never show fringes, Young's clever trick, NEET shortcuts, problems to solve yourself, and 12 MCQs.

NCERT Class 12 Physics Part II · Ch 10 Wave Optics · §10.4 Coherent and incoherent addition of waves · pp. 262–265 · about 60 min

Voice
About 6 minutes. The animations start by themselves as the teacher explains them. Each stage's Listen button uses the same language.

Two speakers playing the same steady tone make fixed loud and soft spots in the hall. Where the two paths differ by half a wavelength, the waves cancel. Light does the same, but only if both waves come from one source.

Stage 1 · The hook (5 min)

Loud, soft, loud: the wedding sound check

Level

Before a wedding sangeet, Rohan uncle tests the sound system: both speakers on the stage play one steady "hmmmm" tone. Priya walks across the empty hall and notices something strange: in some places the tone is loud, a few steps later it almost disappears, then it is loud again. The speakers did not change. Only her position did.

At each spot two waves arrive, one from each speaker. If crest meets crest they add up; if crest meets trough they cancel. Which one happens depends on how much farther one speaker is than the other: the path difference. This is interference, and light does exactly the same thing, as Thomas Young showed in 1801.

Try at home

Put two phone speakers (or two earphones) half a metre apart playing the same steady tone from one tone-generator app with a split cable. Close one ear and move your head slowly sideways. Do you hear loud and soft places? Now play two different songs from two phones. What changes?

Answer

With one tone fed to both, you hear fixed loud and soft spots: the sources are coherent. Two different songs (or two separate phones) have no fixed phase relation, so there are no steady quiet spots: the sounds just add up.

Teacher says

"Two waves, one place. Crest on crest: louder. Crest on trough: silence. The secret is a steady phase difference."

Stage 2 · The concept (10 min)

Superposition and coherent sources: a ripple tank

Level

Two needles dip into water, moving up and down exactly alike. This picture is computed live by adding the two circular waves at every point. Change the separation, switch between the instant ripples and the average brightness, and drag the probe P.

Superposition principle

y = y₁ + y₂

The resultant displacement at any point is the (vector) sum of the displacements of the individual waves.

Coherent sources

φ₁ − φ₂ = constant in time

Not "equal brightness" or "same colour". Only a phase difference that does not change.

Nodal and antinodal lines

still water / big ripples

With coherent sources the pattern stays fixed. More separation d gives more lines, packed closer together.

Teacher says

"Look at the average view. With coherent sources, the bright and dark lines stay put. Switch to incoherent and they smear into a flat grey: no interference pattern."

Stage 3 · The law (10 min)

Path difference decides: add or cancel

Level

Two in-phase sources S₁ and S₂ send waves of equal amplitude a to a point P. One path is longer by Δ = S₂P − S₁P. Slide Δ and watch wave 1 (blue), wave 2 (purple) and their sum (green).

  1. Path difference to phase difference

    φ = (2π/λ) Δ

    One whole wavelength of extra path is one whole cycle, 2π, of phase.

  2. Constructive interference (bright)

    Δ = nλ ⇔ φ = 2nπ,   n = 0, 1, 2, …

    Crest meets crest. Resultant amplitude 2a, intensity 4I₀.

  3. Destructive interference (dark)

    Δ = (n + ½)λ ⇔ φ = (2n + 1)π

    Crest meets trough. For equal amplitudes the resultant is zero.

Teacher says

"Whole number of wavelengths: bright. Half-odd number: dark. On the perpendicular bisector Δ = 0, so that line is always bright."

Pause and predict

"What if S₂ vibrates exactly opposite to S₁ (phase difference π at the source)? Is the bisector still bright?"

Answer

No, it becomes dark. Add the source phase difference to (2π/λ)Δ. With an extra π, every bright place becomes dark and every dark place bright.

Stage 4 · Maths (10 min)

Intensity at any point: I = 4I₀ cos²(φ/2)

Level

Between "fully bright" and "fully dark" there is everything in between. Add the two waves as arrows (phasors), and read the intensity on the graph. Drag the marker on the graph or use the sliders.

  1. Write the two waves

    y₁ = a cos ωt,   y₂ = a cos(ωt + φ)

    Equal amplitude a, phase difference φ at the point P.

  2. Add using cos A + cos B

    y = 2a cos(φ/2) · cos(ωt + φ/2)

    The resultant is a wave of the same frequency with amplitude 2a cos(φ/2).

  3. Intensity ∝ amplitude²

    I = 4 a² cos²(φ/2) = 4 I₀ cos²(φ/2)

    I₀ ∝ a² is the intensity of one wave alone. Maximum 4I₀ at φ = 0, 2π, 4π…; zero at φ = π, 3π…

  4. Unequal waves (NEET)

    I = I₁ + I₂ + 2√(I₁I₂) cos φ

    I_max = (√I₁ + √I₂)², I_min = (√I₁ − √I₂)². With I₁ = I₂ = I₀ this is the formula above.

Teacher says

"Check any formula with three numbers: φ = 0 gives 4I₀, φ = π gives 0, and the average over all φ is 2I₀. Energy is not created or lost, only moved from dark places to bright places."

Stage 5 · The big idea (10 min)

When coherence is lost, fringes vanish

Level

A real lamp changes its phase abruptly about every 10⁻¹⁰ s. Below, the top strip shows the fringe pattern at one instant; the graph shows what a detector records on average. Switch between coherent and incoherent sources.

Coherent

I = 4I₀ cos²(φ/2)

Fixed φ at each point: steady bright (4I₀) and dark (0) fringes.

Incoherent

⟨cos²(φ/2)⟩ = ½ ⇒ I = 2I₀

φ changes randomly and rapidly, so only the average is seen: uniform 2I₀, no fringes.

Intensities just add

I = I₁ + I₂

For incoherent sources add intensities. For coherent sources add amplitudes first, then square.

Teacher says

"Two candles, two bulbs, two sodium lamps: incoherent. Their intensities add, 2I₀ everywhere. That is why your room has no dark stripes on the wall."

Stage 6 · Real life (5 min)

Young's trick: one parent, two pinholes

Level

Each lamp below changes its phase at random moments (the colour change on its waves). Compare two separate lamps with Young's arrangement: one pinhole S lighting two close pinholes S₁ and S₂.

Why separate lamps fail

phase jumps every ~10⁻¹⁰ s

Each atom emits independently. The phase difference of two lamps changes billions of times a second.

Young's idea (1801)

S₁, S₂ from one S

A phase jump at S reaches S₁ and S₂ at the same moment (equal paths), so φ₁ − φ₂ stays fixed.

Seen every day

soap bubbles, oil films

Light reflected from the top and bottom of a thin film comes from the same wave: coherent. The colours are interference.

Teacher says

"Think of S as the parent and S₁, S₂ as twins. Whatever the parent does, both twins do at the same moment. That is coherence."

Stage 7 · NEET level (10 min)

Shortcuts and tricks

Level

Path to phase

φ = 2πΔ/λ

λ/4 → π/2, λ/2 → π, λ → 2π, 1.5λ → 3π.

Equal waves

I = 4I₀ cos²(φ/2)

φ = 60°: 3I₀; 90°: 2I₀; 120°: I₀; 180°: 0.

Unequal waves

I_max/I_min = ((√I₁+√I₂)/(√I₁−√I₂))²

I and 4I: 9 : 1. I and 9I: 4 : 1.

From amplitudes

I_max/I_min = ((a₁+a₂)/(a₁−a₂))²

a₁ : a₂ = 2 : 1 gives 9 : 1. Work backwards with square roots.

Coherent vs incoherent

4I₀ / 0   vs   2I₀

Average of a coherent pattern is also 2I₀: energy is conserved, only redistributed.

Fringe visibility

best when I₁ = I₂

Unequal sources: dark fringes are not fully dark (I_min ≠ 0).

Teacher says

"For any interference number, ask two questions: coherent or not? Equal intensities or not? Then pick the formula. Half the NEET questions end right there."

Stage 8 · Solve it yourself

Five worked problems

Level

Cover the solution, write the formula, and solve on paper. Open the hint only if you are stuck for more than a minute.

Problem 1 · Partial brightness

Two coherent sources each give intensity I₀ at a point. The phase difference there is π/3. Find the resultant intensity and the path difference (in terms of λ).

Hint

I = 4I₀ cos²(φ/2); Δ = (λ/2π) φ.

Full solution
I = 4I₀ cos²(π/6) = 4I₀ × (√3/2)² = 3I₀
Δ = (λ/2π) × (π/3) = λ/6
I = 3I₀, Δ = λ/6
Problem 2 · Bright or dark?

Light of wavelength 600 nm from two in-phase coherent sources reaches a point with a path difference of 1.5 μm. Is the point bright or dark? What is the phase difference?

Hint

Divide Δ by λ. Whole number: bright. Half-odd: dark.

Full solution
Δ/λ = 1.5 × 10⁻⁶ / 600 × 10⁻⁹ = 2.5
φ = 2π × 2.5 = 5π (odd multiple of π)
Dark (destructive), φ = 5π
Problem 3 · Unequal sources

Two coherent sources have intensities I and 4I. Find the maximum and minimum intensity in the interference pattern and their ratio.

Hint

I_max = (√I₁ + √I₂)², I_min = (√I₁ − √I₂)².

Full solution
√I₁ = √I, √I₂ = 2√I
I_max = (√I + 2√I)² = 9I
I_min = (2√I − √I)² = I
9I and I, ratio 9 : 1
Problem 4 · Two bulbs vs Young

Two identical bulbs each give intensity I₀ on a wall. What is the intensity on the wall? If instead two coherent sources of the same strength are used, what are the brightest, darkest and average intensities?

Hint

Incoherent: add intensities. Coherent: 4I₀ cos²(φ/2), average of cos² is ½.

Full solution
Bulbs (incoherent): I = I₀ + I₀ = 2I₀ everywhere
Coherent: I_max = 4I₀, I_min = 0
average = 4I₀ × ½ = 2I₀
2I₀ uniform; coherent: 4I₀, 0, average 2I₀ (energy conserved)
Problem 5 · Working backwards

In an interference pattern I_max : I_min = 25 : 9. Find the ratio of the amplitudes and of the intensities of the two sources.

Hint

Take square roots: (a₁ + a₂)/(a₁ − a₂) = 5/3.

Full solution
(a₁ + a₂)/(a₁ − a₂) = √(25/9) = 5/3
3a₁ + 3a₂ = 5a₁ − 5a₂ ⇒ 2a₁ = 8a₂
a₁ : a₂ = 4 : 1, so I₁ : I₂ = 16 : 1
Amplitudes 4 : 1, intensities 16 : 1
Stage 9 · Practice ladder

12 MCQs, from easy to NEET-level

Level

I₀ is the intensity of one wave alone. Write the formula first, then click.

Score: 0 / 12

Stage 10 · Exam corner

How NEET asks this

If the question says…Write this firstThe trap
"coherent sources" definedconstant phase difference in timeChoosing "same amplitude" or "same intensity"
"path difference x, find phase"φ = 2πx/λForgetting the 2π, or using λ/x
"intensity at phase difference φ"I = 4I₀ cos²(φ/2)Writing cos²φ instead of cos²(φ/2)
"maximum intensity" with I₀ each4I₀ (not 2I₀)Adding intensities for coherent waves
"two independent sources / two bulbs"incoherent: I = I₁ + I₂, no fringesAnswering 4I₀ and 0
"ratio of max to min intensity"((√I₁ + √I₂)/(√I₁ − √I₂))²Using the intensity ratio directly without square roots
"amplitude ratio a₁ : a₂"I_max/I_min = ((a₁ + a₂)/(a₁ − a₂))²Taking square roots of amplitudes
"energy in interference"conserved, redistributed"Energy is destroyed at dark fringes"

Mistakes to avoid

Where this connects next

Lesson 4 puts numbers on Young's arrangement: the path difference x d/D on a screen, the positions of bright and dark fringes, and the fringe width β = λD/d.

Notation: I₀ = intensity of one wave alone (∝ a²), φ = phase difference, Δ = path difference. NCERT §10.4 treats equal amplitudes; the unequal-intensity formulas are standard NEET extensions.

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Well done. What next?

Follow the four steps: understand it, remember it, try it, then prove it with past papers.

Lesson 4: Young's double slit ›✍️ Practise this lesson: Wave Optics Challenge Q8–10: interferenceRemember it: 5-Minute Revise‹ Previous: Lesson 2: Reflection and refraction by wavefronts‹ Back to chapter🏠 Physics Part 2 home