Amplitude
The electric-field amplitudes add with phase. They may reinforce or oppose one another.
Wave Optics · Chapter 02
Master superposition, coherent sources, path and phase difference, intensity distribution and Young's Double Slit Experiment for board and competitive examinations.
When two or more light waves overlap in a linear medium, the instantaneous resultant displacement equals the algebraic sum of their individual displacements. The waves continue through one another; interference changes the observed intensity distribution, not the identity of the component waves.
The electric-field amplitudes add with phase. They may reinforce or oppose one another.
Brightness is proportional to the square of resultant amplitude. Therefore I₁/I₂ = a²/b².
Interference redistributes energy between bright and dark regions; total energy remains conserved.
Contrast ratio: Imax/Imin = (a+b)²/(a−b)². If a = b, then Imax = 4a² and Imin = 0.
Let y₁ = a sinωt and y₂ = b sin(ωt + φ).
By superposition: y = y₁ + y₂.
y = a sinωt + b sin(ωt + φ).
y = a sinωt + b sinωt cosφ + b cosωt sinφ.
y = (a + b cosφ) sinωt + (b sinφ) cosωt.
Let R cosθ = a + b cosφ and R sinθ = b sinφ.
Squaring and adding: R² = a² + b² + 2ab cosφ.
Since intensity is proportional to amplitude squared: I = a² + b² + 2ab cosφ.
If I₁ ∝ a² and I₂ ∝ b²: I = I₁ + I₂ + 2√(I₁I₂) cosφ.
If a = b and each beam has intensity I₀:
I = 2I₀(1+cosφ) = 4I₀cos²(φ/2)In amplitude units: I = 4a²cos²(φ/2).
Imax = (a+b)²
Imin = (a−b)²
V = (Imax−Imin)/(Imax+Imin) = 2ab/(a²+b²)
A wave leads if it reaches the same phase earlier; it lags if it reaches that phase later. The sign depends on the chosen reference wave.
The overlapping circular wavefronts from S₁ and S₂ reach the screen with different path differences. At O and P₂-type points the waves reinforce; at P₁-type points they oppose, giving alternating bright and dark fringes.
S₁ and S₂ are separated by d. The screen is at distance D, with D ≫ d.
At the screen center, Δx = 0, so the waves arrive in phase and form the central bright fringe.
Successive bright or dark fringes are separated by β = λD/d.
Colors arise because reflected beams acquire wavelength-dependent phase differences.
A coating creates destructive interference between reflected beams.
Split beams recombine to reveal tiny optical path changes.
Known fringe shifts allow accurate wavelength determination.
Introducing a sample changes optical path and shifts fringes.
Fringe distortion reveals very small surface irregularities.
Two waves have amplitudes 2 and 3. Find Imax in proportional units.
Answer: 25
Detailed solution: Imax = (a+b)² = (2+3)² = 25.
Two waves have amplitudes 3 and 5. Find Imax in proportional units.
Answer: 64
Detailed solution: Imax = (a+b)² = (3+5)² = 64.
Two waves have amplitudes 4 and 1. Find Imax in proportional units.
Answer: 25
Detailed solution: Imax = (a+b)² = (4+1)² = 25.
Two waves have amplitudes 5 and 2. Find Imax in proportional units.
Answer: 49
Detailed solution: Imax = (a+b)² = (5+2)² = 49.
Two waves have amplitudes 6 and 4. Find Imax in proportional units.
Answer: 100
Detailed solution: Imax = (a+b)² = (6+4)² = 100.
Two waves have amplitudes 5 and 2. Find Imin.
Answer: 9
Detailed solution: Imin = (a−b)² = (5−2)² = 9.
Two waves have amplitudes 7 and 3. Find Imin.
Answer: 16
Detailed solution: Imin = (a−b)² = (7−3)² = 16.
Two waves have amplitudes 8 and 5. Find Imin.
Answer: 9
Detailed solution: Imin = (a−b)² = (8−5)² = 9.
Two waves have amplitudes 6 and 1. Find Imin.
Answer: 25
Detailed solution: Imin = (a−b)² = (6−1)² = 25.
Two waves have amplitudes 9 and 4. Find Imin.
Answer: 25
Detailed solution: Imin = (a−b)² = (9−4)² = 25.
Equal beams each have intensity 4. Find resultant intensity at φ = 0°.
Answer: 16.00
Detailed solution: I = 2I₀(1+cosφ) = 8(1+cos0°) = 16.00.
Equal beams each have intensity 4. Find resultant intensity at φ = 60°.
Answer: 12.00
Detailed solution: I = 2I₀(1+cosφ) = 8(1+cos60°) = 12.00.
Equal beams each have intensity 5. Find resultant intensity at φ = 90°.
Answer: 10.00
Detailed solution: I = 2I₀(1+cosφ) = 10(1+cos90°) = 10.00.
Equal beams each have intensity 3. Find resultant intensity at φ = 120°.
Answer: 3.00
Detailed solution: I = 2I₀(1+cosφ) = 6(1+cos120°) = 3.00.
Equal beams each have intensity 6. Find resultant intensity at φ = 180°.
Answer: 0.00
Detailed solution: I = 2I₀(1+cosφ) = 12(1+cos180°) = 0.00.
For path difference 0.25λ, find phase difference.
Answer: 0.50π rad
Detailed solution: φ = 2πΔx/λ = 2π(0.25) = 0.50π rad.
For path difference 0.5λ, find phase difference.
Answer: 1.00π rad
Detailed solution: φ = 2πΔx/λ = 2π(0.5) = 1.00π rad.
For path difference 0.75λ, find phase difference.
Answer: 1.50π rad
Detailed solution: φ = 2πΔx/λ = 2π(0.75) = 1.50π rad.
For path difference 1.5λ, find phase difference.
Answer: 3.00π rad
Detailed solution: φ = 2πΔx/λ = 2π(1.5) = 3.00π rad.
For path difference 2.25λ, find phase difference.
Answer: 4.50π rad
Detailed solution: φ = 2πΔx/λ = 2π(2.25) = 4.50π rad.
For phase difference 0.5π rad, find path difference.
Answer: 0.25λ
Detailed solution: Δx = φλ/(2π) = 0.5πλ/(2π) = 0.25λ.
For phase difference 1π rad, find path difference.
Answer: 0.50λ
Detailed solution: Δx = φλ/(2π) = 1πλ/(2π) = 0.50λ.
For phase difference 1.5π rad, find path difference.
Answer: 0.75λ
Detailed solution: Δx = φλ/(2π) = 1.5πλ/(2π) = 0.75λ.
For phase difference 0.25π rad, find path difference.
Answer: 0.13λ
Detailed solution: Δx = φλ/(2π) = 0.25πλ/(2π) = 0.13λ.
For phase difference 1.75π rad, find path difference.
Answer: 0.88λ
Detailed solution: Δx = φλ/(2π) = 1.75πλ/(2π) = 0.88λ.
The interfering intensities are 9 and 4. Find visibility.
Answer: 0.923
Detailed solution: V = 2√(I₁I₂)/(I₁+I₂) = 0.923.
The interfering intensities are 16 and 4. Find visibility.
Answer: 0.800
Detailed solution: V = 2√(I₁I₂)/(I₁+I₂) = 0.800.
The interfering intensities are 25 and 9. Find visibility.
Answer: 0.882
Detailed solution: V = 2√(I₁I₂)/(I₁+I₂) = 0.882.
The interfering intensities are 10 and 2.5. Find visibility.
Answer: 0.800
Detailed solution: V = 2√(I₁I₂)/(I₁+I₂) = 0.800.
The interfering intensities are 12 and 3. Find visibility.
Answer: 0.800
Detailed solution: V = 2√(I₁I₂)/(I₁+I₂) = 0.800.
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not correctly explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
Case: White light reflects from the upper and lower surfaces of a thin oil film.
Detailed solution: Different wavelengths satisfy constructive or destructive conditions at different angles, producing colors.
Key result: Thin-film interference redistributes wavelengths spatially.
Case: A second sound is generated opposite in phase to ambient noise.
Detailed solution: At the ear, similar amplitudes with phase difference π give destructive interference.
Key result: The cancellation is best when amplitudes match.
Case: A coating is selected so two reflected beams cancel.
Detailed solution: Optical thickness and reflection phase shifts are chosen for odd-π relative phase.
Key result: Reduced reflection increases transmission.
Case: The observation point is equidistant from S₁ and S₂.
Detailed solution: Path difference is zero and the coherent waves arrive in phase.
Key result: A central bright fringe appears.
Case: One slit receives four times the intensity of the other.
Detailed solution: Amplitudes are in ratio 2:1; Imax = 9 units and Imin = 1 unit on a common scale.
Key result: Visibility becomes 8/10 = 0.8.
Case: A narrow spectral line is used instead of white light.
Detailed solution: A single wavelength gives a regular fixed phase-to-path relation.
Key result: Fringes are sharp and evenly interpretable.
Case: The source slit is widened substantially.
Detailed solution: Different source points form shifted fringe systems that overlap.
Key result: Spatial coherence falls and visibility decreases.
Case: A thin transparent plate is placed in front of one slit.
Detailed solution: It adds optical path (μ−1)t and shifts the entire fringe pattern.
Key result: Fringe spacing stays essentially unchanged.
Case: Two synchronized antennas radiate at the same frequency.
Detailed solution: Their fields add constructively and destructively depending on path difference.
Key result: Directional maxima and minima form.
Case: A beam is split, sent along two paths and recombined.
Detailed solution: A tiny path change creates a measurable phase shift.
Key result: Interference enables precision length and refractive-index measurements.
Academic note: These are original PYQ-pattern and exam-style questions, not verbatim reproductions of copyrighted past papers.
A. resultant displacement equals the algebraic sum of component displacements
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. coherent sources have equal frequency and constant phase difference
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Δx = nλ and φ = 2nπ
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. Δx = (2n−1)λ/2 and φ = (2n−1)π
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. I = I₁+I₂+2√(I₁I₂)cosφ
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. I = 4I₀cos²(φ/2)
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Imax = (a+b)²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. Imin = (a−b)²
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. φ = 2πΔx/λ
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. V = (Imax−Imin)/(Imax+Imin)
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. I₁/I₂ = a²/b²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. equal paths give a bright central fringe
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. interference redistributes energy rather than creating or destroying it
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. one primary source illuminating two slits provides coherence
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. visibility is maximum when the two intensities are equal
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. resultant displacement equals the algebraic sum of component displacements
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. coherent sources have equal frequency and constant phase difference
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. Δx = nλ and φ = 2nπ
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Δx = (2n−1)λ/2 and φ = (2n−1)π
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. I = I₁+I₂+2√(I₁I₂)cosφ
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. I = 4I₀cos²(φ/2)
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. Imax = (a+b)²
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Imin = (a−b)²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. φ = 2πΔx/λ
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. V = (Imax−Imin)/(Imax+Imin)
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. I₁/I₂ = a²/b²
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. equal paths give a bright central fringe
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. interference redistributes energy rather than creating or destroying it
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. one primary source illuminating two slits provides coherence
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. visibility is maximum when the two intensities are equal
A. resultant displacement equals the algebraic sum of component displacements
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. coherent sources have equal frequency and constant phase difference
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Δx = nλ and φ = 2nπ
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. Δx = (2n−1)λ/2 and φ = (2n−1)π
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. I = I₁+I₂+2√(I₁I₂)cosφ
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. I = 4I₀cos²(φ/2)
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Imax = (a+b)²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. Imin = (a−b)²
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. φ = 2πΔx/λ
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. V = (Imax−Imin)/(Imax+Imin)
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. I₁/I₂ = a²/b²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. equal paths give a bright central fringe
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. interference redistributes energy rather than creating or destroying it
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. one primary source illuminating two slits provides coherence
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. visibility is maximum when the two intensities are equal
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. resultant displacement equals the algebraic sum of component displacements
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. coherent sources have equal frequency and constant phase difference
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. Δx = nλ and φ = 2nπ
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Δx = (2n−1)λ/2 and φ = (2n−1)π
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. I = I₁+I₂+2√(I₁I₂)cosφ
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. I = 4I₀cos²(φ/2)
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. Imax = (a+b)²
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Imin = (a−b)²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. φ = 2πΔx/λ
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. V = (Imax−Imin)/(Imax+Imin)
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. I₁/I₂ = a²/b²
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. equal paths give a bright central fringe
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. interference redistributes energy rather than creating or destroying it
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. one primary source illuminating two slits provides coherence
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. visibility is maximum when the two intensities are equal
A. resultant displacement equals the algebraic sum of component displacements
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. coherent sources have equal frequency and constant phase difference
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Δx = nλ and φ = 2nπ
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. Δx = (2n−1)λ/2 and φ = (2n−1)π
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. I = I₁+I₂+2√(I₁I₂)cosφ
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. I = 4I₀cos²(φ/2)
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Imax = (a+b)²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. Imin = (a−b)²
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. φ = 2πΔx/λ
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. V = (Imax−Imin)/(Imax+Imin)
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. I₁/I₂ = a²/b²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. equal paths give a bright central fringe
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. interference redistributes energy rather than creating or destroying it
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. one primary source illuminating two slits provides coherence
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. visibility is maximum when the two intensities are equal
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. resultant displacement equals the algebraic sum of component displacements
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. coherent sources have equal frequency and constant phase difference
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. Δx = nλ and φ = 2nπ
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Δx = (2n−1)λ/2 and φ = (2n−1)π
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. I = I₁+I₂+2√(I₁I₂)cosφ
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. I = 4I₀cos²(φ/2)
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. Imax = (a+b)²
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Imin = (a−b)²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. φ = 2πΔx/λ
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. V = (Imax−Imin)/(Imax+Imin)
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. I₁/I₂ = a²/b²
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. equal paths give a bright central fringe
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. interference redistributes energy rather than creating or destroying it
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. one primary source illuminating two slits provides coherence
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. visibility is maximum when the two intensities are equal
A. resultant displacement equals the algebraic sum of component displacements
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. coherent sources have equal frequency and constant phase difference
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Δx = nλ and φ = 2nπ
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. Δx = (2n−1)λ/2 and φ = (2n−1)π
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. I = I₁+I₂+2√(I₁I₂)cosφ
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. I = 4I₀cos²(φ/2)
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Imax = (a+b)²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. Imin = (a−b)²
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. φ = 2πΔx/λ
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. V = (Imax−Imin)/(Imax+Imin)
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. I₁/I₂ = a²/b²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. equal paths give a bright central fringe
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. interference redistributes energy rather than creating or destroying it
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. one primary source illuminating two slits provides coherence
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. visibility is maximum when the two intensities are equal
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. resultant displacement equals the algebraic sum of component displacements
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. coherent sources have equal frequency and constant phase difference
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. Δx = nλ and φ = 2nπ
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Δx = (2n−1)λ/2 and φ = (2n−1)π
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. I = I₁+I₂+2√(I₁I₂)cosφ
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. I = 4I₀cos²(φ/2)
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. Imax = (a+b)²
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Imin = (a−b)²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. φ = 2πΔx/λ
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. V = (Imax−Imin)/(Imax+Imin)
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. I₁/I₂ = a²/b²
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. equal paths give a bright central fringe
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. interference redistributes energy rather than creating or destroying it
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. one primary source illuminating two slits provides coherence
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. visibility is maximum when the two intensities are equal
A. resultant displacement equals the algebraic sum of component displacements
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. coherent sources have equal frequency and constant phase difference
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Δx = nλ and φ = 2nπ
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. Δx = (2n−1)λ/2 and φ = (2n−1)π
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. I = I₁+I₂+2√(I₁I₂)cosφ
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. I = 4I₀cos²(φ/2)
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Imax = (a+b)²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. Imin = (a−b)²
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. φ = 2πΔx/λ
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. V = (Imax−Imin)/(Imax+Imin)
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. I₁/I₂ = a²/b²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. equal paths give a bright central fringe
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. interference redistributes energy rather than creating or destroying it
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. one primary source illuminating two slits provides coherence
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. visibility is maximum when the two intensities are equal
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. resultant displacement equals the algebraic sum of component displacements
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. coherent sources have equal frequency and constant phase difference
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. Δx = nλ and φ = 2nπ
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Δx = (2n−1)λ/2 and φ = (2n−1)π
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. I = I₁+I₂+2√(I₁I₂)cosφ
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. I = 4I₀cos²(φ/2)
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. Imax = (a+b)²
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Imin = (a−b)²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. φ = 2πΔx/λ
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. V = (Imax−Imin)/(Imax+Imin)
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. I₁/I₂ = a²/b²
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. equal paths give a bright central fringe
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. interference redistributes energy rather than creating or destroying it
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. one primary source illuminating two slits provides coherence
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. visibility is maximum when the two intensities are equal
A. resultant displacement equals the algebraic sum of component displacements
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. coherent sources have equal frequency and constant phase difference
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Δx = nλ and φ = 2nπ
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. Δx = (2n−1)λ/2 and φ = (2n−1)π
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. I = I₁+I₂+2√(I₁I₂)cosφ
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. I = 4I₀cos²(φ/2)
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Imax = (a+b)²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. Imin = (a−b)²
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. φ = 2πΔx/λ
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. V = (Imax−Imin)/(Imax+Imin)
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. I₁/I₂ = a²/b²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. equal paths give a bright central fringe
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. interference redistributes energy rather than creating or destroying it
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. one primary source illuminating two slits provides coherence
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. visibility is maximum when the two intensities are equal
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. resultant displacement equals the algebraic sum of component displacements
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. coherent sources have equal frequency and constant phase difference
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. Δx = nλ and φ = 2nπ
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Δx = (2n−1)λ/2 and φ = (2n−1)π
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. I = I₁+I₂+2√(I₁I₂)cosφ
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. I = 4I₀cos²(φ/2)
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. Imax = (a+b)²
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Imin = (a−b)²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. φ = 2πΔx/λ
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. V = (Imax−Imin)/(Imax+Imin)
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. I₁/I₂ = a²/b²
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. equal paths give a bright central fringe
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. interference redistributes energy rather than creating or destroying it
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. one primary source illuminating two slits provides coherence
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. visibility is maximum when the two intensities are equal
A. resultant displacement equals the algebraic sum of component displacements
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. coherent sources have equal frequency and constant phase difference
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Δx = nλ and φ = 2nπ
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. Δx = (2n−1)λ/2 and φ = (2n−1)π
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. I = I₁+I₂+2√(I₁I₂)cosφ
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. I = 4I₀cos²(φ/2)
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Imax = (a+b)²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. Imin = (a−b)²
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. φ = 2πΔx/λ
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. V = (Imax−Imin)/(Imax+Imin)
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. I₁/I₂ = a²/b²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. equal paths give a bright central fringe
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. interference redistributes energy rather than creating or destroying it
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. one primary source illuminating two slits provides coherence
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. visibility is maximum when the two intensities are equal
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. resultant displacement equals the algebraic sum of component displacements
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. coherent sources have equal frequency and constant phase difference
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. Δx = nλ and φ = 2nπ
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Δx = (2n−1)λ/2 and φ = (2n−1)π
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. I = I₁+I₂+2√(I₁I₂)cosφ
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. I = 4I₀cos²(φ/2)
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. Imax = (a+b)²
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. Imin = (a−b)²
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. φ = 2πΔx/λ
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. V = (Imax−Imin)/(Imax+Imin)
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. I₁/I₂ = a²/b²
A. wave intensity is directly proportional to amplitude
B. coherence requires unequal frequencies
C. equal paths give a bright central fringe
D. frequency must change at every bright fringe
A. coherence requires unequal frequencies
B. interference redistributes energy rather than creating or destroying it
C. frequency must change at every bright fringe
D. wave intensity is directly proportional to amplitude
A. one primary source illuminating two slits provides coherence
B. frequency must change at every bright fringe
C. wave intensity is directly proportional to amplitude
D. coherence requires unequal frequencies
A. frequency must change at every bright fringe
B. wave intensity is directly proportional to amplitude
C. coherence requires unequal frequencies
D. visibility is maximum when the two intensities are equal
I = I₁+I₂+2√(I₁I₂)cosφ
φ = 2nπ; Δx = nλ
φ = (2n−1)π; Δx = (2n−1)λ/2
I = 4I₀cos²(φ/2); Imax = 4I₀; Imin = 0
I₁/I₂ = a²/b²
Coherence requires constant phase difference, not equal amplitude.