Coherent Sources
S₁ and S₂ have the same frequency and a constant phase difference because both are illuminated by one source.
Wave Optics · Chapter 03
Build YDSE from coherent sources and path difference to fringe width, fringe shift, missing orders and intensity distribution.
Young's experiment demonstrates the wave nature of light by dividing one incident wavefront into two coherent secondary sources S₁ and S₂. The slits are narrow, have separation d, and illuminate a screen at distance D where D ≫ d.
S₁ and S₂ have the same frequency and a constant phase difference because both are illuminated by one source.
Monochromatic light, narrow slits, D ≫ d, small observation angle and overlapping diffracted beams.
At O, both optical paths are equal: Δ = 0. Hence the central fringe is bright.
For a point P at transverse displacement x, the rays make a small angle θ.
Path difference: Δ = S₂P − S₁P = d sinθ.
For small θ: sinθ ≈ tanθ = x/D.
Therefore: Δ = xd/D.
Phase difference: φ = (2π/λ)Δ = 2πxd/(λD).
Notation rule: Δ is used only for path difference. φ is used only for phase difference. No other symbol is used for path difference.
For constructive interference: Δ = nλ, where n = 0, 1, 2, 3, ...
Using Δ = dxₙ/D: dxₙ/D = nλ.
Hence xₙ = nλD/d = nβ.
For n = 0, x₀ = 0, giving the central bright fringe.
For destructive interference: Δ = (2n−1)λ/2, where n = 1, 2, 3, ...
Using Δ = dxₙ/D: dxₙ/D = (2n−1)λ/2.
Hence xₙ = (2n−1)λD/(2d) = (2n−1)β/2.
The first dark fringe is at x = β/2 on either side of O.
The positions of consecutive bright fringes are xₙ = nλD/d and xₙ₊₁ = (n+1)λD/d.
β = xₙ₊₁ − xₙ = λD/d.
The same separation is obtained between consecutive dark fringes.
| Change | Effect on β | Reason |
|---|---|---|
| λ increases | β increases | β ∝ λ |
| D increases | β increases | β ∝ D |
| d increases | β decreases | β ∝ 1/d |
Angular position θₙ ≈ xₙ/D.
For consecutive bright fringes, Δθ = β/D.
Using β = λD/d: Δθ = λ/d.
Bright and dark fringes move farther apart. Red light gives wider fringes than blue light.
The pattern expands linearly on the screen, although angular fringe width remains unchanged.
The pattern contracts because the path difference changes more rapidly with x.
Moving the illuminating source introduces a constant initial path difference between S₁ and S₂. The zero-path point therefore moves, shifting the entire fringe system.
The pattern shifts in the opposite sense required to restore equal total paths.
The shift reverses. Its magnitude depends on source geometry.
Source shift moves the complete pattern but does not change fringe width.
D increases, so β = λD/d increases and the fringes spread out.
D decreases, so β decreases and the fringes come closer.
A plate of thickness t and refractive index μ replaces the same thickness of air.
Additional optical path: Δp = μt − t = (μ−1)t.
A shift Δx produces compensating geometrical path dΔx/D.
Equating: dΔx/D = Δp.
Therefore Δx = DΔp/d = D(μ−1)t/d.
Since β = λD/d: Δx = β(μ−1)t/λ.
The entire fringe system shifts toward the slit containing the plate. Fringe width remains unchanged.
In a liquid of refractive index μ, wavelength becomes λ′ = λ/μ.
β′ = λ′D/d = λD/(μd).
Thus β′ = β/μ.
Frequency is unchanged on entering the liquid, but wave speed and wavelength decrease, so the fringes become narrower.
Let each slit have width a and slit separation d.
Interference maximum: d sinθ = nλ.
Single-slit diffraction minimum: a sinθ = mλ.
If both coincide, n = m(d/a).
Therefore interference orders equal to integer multiples of d/a are missing when d/a is an integer.
Example: If d = 4a, the 4th, 8th, 12th, ... interference maxima are absent.
General result: I = I₁ + I₂ + 2√(I₁I₂)cosφ.
For I₁ = I₂ = I₀: I = 2I₀(1+cosφ).
Using 1+cosφ = 2cos²(φ/2): I = 4I₀cos²(φ/2).
At φ = 2nπ, Imax = 4I₀. At φ = (2n−1)π, Imin = 0.
Visibility V = (Imax−Imin)/(Imax+Imin).
For λ = 500 nm, D = 1 m and d = 0.5 mm, find β.
Answer: 1.000 mm
Step-by-step solution: β = λD/d = (500×10⁻⁹×1)/(0.5×10⁻³) = 1.000e-3 m = 1.000 mm.
If β = 1.10 mm, find the position of the 2nd bright fringe.
Answer: 2.20 mm
Step-by-step solution: xₙ = nβ = 2 × 1.10 = 2.20 mm.
For β = 1.20 mm, find the 3rd dark fringe from the center.
Answer: 3.00 mm
Step-by-step solution: xₙ = (2n−1)β/2 = 5×1.20/2 = 3.00 mm.
A sheet of μ = 1.55 and thickness 5 μm is inserted. D = 2.5 m, d = 0.5 mm. Find Δx.
Answer: 13.750 mm
Step-by-step solution: Δp = (μ−1)t. Therefore Δx = D(μ−1)t/d = 13.750 mm.
The apparatus is immersed in a liquid of refractive index 1.40. Find β′/β.
Answer: 0.714
Step-by-step solution: β′ = β/μ, so β′/β = 1/1.40 = 0.714.
Interference slit separation is 3 times the slit width. Which interference orders are missing?
Answer: Multiples of 3
Step-by-step solution: Diffraction minimum a sinθ = mλ coincides with interference maximum d sinθ = nλ. Thus n = m(d/a) = 3m; orders 3, 6, 9, ... are missing.
Two slit intensities are 4 and 1 units. Find Imax and Imin.
Answer: Imax = 9, Imin = 1
Step-by-step solution: Imax = (√I₁+√I₂)² and Imin = (√I₁−√I₂)². Substitution gives the stated values.
At a point, path difference Δ = 0.75λ. Find phase difference φ.
Answer: 1.50π rad
Step-by-step solution: φ = (2π/λ)Δ = 2π(0.75) = 1.50π rad.
For λ = 650 nm, D = 1 m and d = 1 mm, find β.
Answer: 0.650 mm
Step-by-step solution: β = λD/d = (650×10⁻⁹×1)/(1×10⁻³) = 6.500e-4 m = 0.650 mm.
If β = 2.10 mm, find the position of the 5th bright fringe.
Answer: 10.50 mm
Step-by-step solution: xₙ = nβ = 5 × 2.10 = 10.50 mm.
For β = 1.33 mm, find the 3rd dark fringe from the center.
Answer: 3.33 mm
Step-by-step solution: xₙ = (2n−1)β/2 = 5×1.33/2 = 3.33 mm.
A sheet of μ = 1.55 and thickness 3 μm is inserted. D = 2.5 m, d = 1 mm. Find Δx.
Answer: 4.125 mm
Step-by-step solution: Δp = (μ−1)t. Therefore Δx = D(μ−1)t/d = 4.125 mm.
The apparatus is immersed in a liquid of refractive index 1.40. Find β′/β.
Answer: 0.714
Step-by-step solution: β′ = β/μ, so β′/β = 1/1.40 = 0.714.
Interference slit separation is 3 times the slit width. Which interference orders are missing?
Answer: Multiples of 3
Step-by-step solution: Diffraction minimum a sinθ = mλ coincides with interference maximum d sinθ = nλ. Thus n = m(d/a) = 3m; orders 3, 6, 9, ... are missing.
Two slit intensities are 25 and 9 units. Find Imax and Imin.
Answer: Imax = 64, Imin = 4
Step-by-step solution: Imax = (√I₁+√I₂)² and Imin = (√I₁−√I₂)². Substitution gives the stated values.
At a point, path difference Δ = 0.25λ. Find phase difference φ.
Answer: 0.50π rad
Step-by-step solution: φ = (2π/λ)Δ = 2π(0.25) = 0.50π rad.
For λ = 550 nm, D = 1 m and d = 0.75 mm, find β.
Answer: 0.733 mm
Step-by-step solution: β = λD/d = (550×10⁻⁹×1)/(0.75×10⁻³) = 7.333e-4 m = 0.733 mm.
If β = 0.90 mm, find the position of the 3rd bright fringe.
Answer: 2.70 mm
Step-by-step solution: xₙ = nβ = 3 × 0.90 = 2.70 mm.
For β = 2.60 mm, find the 3rd dark fringe from the center.
Answer: 6.50 mm
Step-by-step solution: xₙ = (2n−1)β/2 = 5×2.60/2 = 6.50 mm.
A sheet of μ = 1.55 and thickness 6 μm is inserted. D = 2.5 m, d = 0.75 mm. Find Δx.
Answer: 11.000 mm
Step-by-step solution: Δp = (μ−1)t. Therefore Δx = D(μ−1)t/d = 11.000 mm.
The apparatus is immersed in a liquid of refractive index 1.40. Find β′/β.
Answer: 0.714
Step-by-step solution: β′ = β/μ, so β′/β = 1/1.40 = 0.714.
Interference slit separation is 3 times the slit width. Which interference orders are missing?
Answer: Multiples of 3
Step-by-step solution: Diffraction minimum a sinθ = mλ coincides with interference maximum d sinθ = nλ. Thus n = m(d/a) = 3m; orders 3, 6, 9, ... are missing.
Two slit intensities are 9 and 4 units. Find Imax and Imin.
Answer: Imax = 25, Imin = 1
Step-by-step solution: Imax = (√I₁+√I₂)² and Imin = (√I₁−√I₂)². Substitution gives the stated values.
At a point, path difference Δ = 1λ. Find phase difference φ.
Answer: 2.00π rad
Step-by-step solution: φ = (2π/λ)Δ = 2π(1) = 2.00π rad.
For λ = 700 nm, D = 1 m and d = 0.5 mm, find β.
Answer: 1.400 mm
Step-by-step solution: β = λD/d = (700×10⁻⁹×1)/(0.5×10⁻³) = 1.400e-3 m = 1.400 mm.
If β = 1.00 mm, find the position of the 1st bright fringe.
Answer: 1.00 mm
Step-by-step solution: xₙ = nβ = 1 × 1.00 = 1.00 mm.
For β = 1.10 mm, find the 3rd dark fringe from the center.
Answer: 2.75 mm
Step-by-step solution: xₙ = (2n−1)β/2 = 5×1.10/2 = 2.75 mm.
A sheet of μ = 1.55 and thickness 4 μm is inserted. D = 2.5 m, d = 0.5 mm. Find Δx.
Answer: 11.000 mm
Step-by-step solution: Δp = (μ−1)t. Therefore Δx = D(μ−1)t/d = 11.000 mm.
The apparatus is immersed in a liquid of refractive index 1.40. Find β′/β.
Answer: 0.714
Step-by-step solution: β′ = β/μ, so β′/β = 1/1.40 = 0.714.
Interference slit separation is 3 times the slit width. Which interference orders are missing?
Answer: Multiples of 3
Step-by-step solution: Diffraction minimum a sinθ = mλ coincides with interference maximum d sinθ = nλ. Thus n = m(d/a) = 3m; orders 3, 6, 9, ... are missing.
Two slit intensities are 1 and 1 units. Find Imax and Imin.
Answer: Imax = 4, Imin = 0
Step-by-step solution: Imax = (√I₁+√I₂)² and Imin = (√I₁−√I₂)². Substitution gives the stated values.
At a point, path difference Δ = 0.5λ. Find phase difference φ.
Answer: 1.00π rad
Step-by-step solution: φ = (2π/λ)Δ = 2π(0.5) = 1.00π rad.
For λ = 600 nm, D = 1 m and d = 1 mm, find β.
Answer: 0.600 mm
Step-by-step solution: β = λD/d = (600×10⁻⁹×1)/(1×10⁻³) = 6.000e-4 m = 0.600 mm.
If β = 1.95 mm, find the position of the 4th bright fringe.
Answer: 7.80 mm
Step-by-step solution: xₙ = nβ = 4 × 1.95 = 7.80 mm.
For β = 1.87 mm, find the 3rd dark fringe from the center.
Answer: 4.67 mm
Step-by-step solution: xₙ = (2n−1)β/2 = 5×1.87/2 = 4.67 mm.
A sheet of μ = 1.55 and thickness 2 μm is inserted. D = 2.5 m, d = 1 mm. Find Δx.
Answer: 2.750 mm
Step-by-step solution: Δp = (μ−1)t. Therefore Δx = D(μ−1)t/d = 2.750 mm.
The apparatus is immersed in a liquid of refractive index 1.40. Find β′/β.
Answer: 0.714
Step-by-step solution: β′ = β/μ, so β′/β = 1/1.40 = 0.714.
Interference slit separation is 3 times the slit width. Which interference orders are missing?
Answer: Multiples of 3
Step-by-step solution: Diffraction minimum a sinθ = mλ coincides with interference maximum d sinθ = nλ. Thus n = m(d/a) = 3m; orders 3, 6, 9, ... are missing.
Two slit intensities are 16 and 9 units. Find Imax and Imin.
Answer: Imax = 49, Imin = 1
Step-by-step solution: Imax = (√I₁+√I₂)² and Imin = (√I₁−√I₂)². Substitution gives the stated values.
At a point, path difference Δ = 1.25λ. Find phase difference φ.
Answer: 2.50π rad
Step-by-step solution: φ = (2π/λ)Δ = 2π(1.25) = 2.50π rad.
For λ = 500 nm, D = 1 m and d = 0.75 mm, find β.
Answer: 0.667 mm
Step-by-step solution: β = λD/d = (500×10⁻⁹×1)/(0.75×10⁻³) = 6.667e-4 m = 0.667 mm.
If β = 0.82 mm, find the position of the 2nd bright fringe.
Answer: 1.65 mm
Step-by-step solution: xₙ = nβ = 2 × 0.82 = 1.65 mm.
For β = 2.40 mm, find the 3rd dark fringe from the center.
Answer: 6.00 mm
Step-by-step solution: xₙ = (2n−1)β/2 = 5×2.40/2 = 6.00 mm.
A sheet of μ = 1.55 and thickness 5 μm is inserted. D = 2.5 m, d = 0.75 mm. Find Δx.
Answer: 9.167 mm
Step-by-step solution: Δp = (μ−1)t. Therefore Δx = D(μ−1)t/d = 9.167 mm.
The apparatus is immersed in a liquid of refractive index 1.40. Find β′/β.
Answer: 0.714
Step-by-step solution: β′ = β/μ, so β′/β = 1/1.40 = 0.714.
Interference slit separation is 3 times the slit width. Which interference orders are missing?
Answer: Multiples of 3
Step-by-step solution: Diffraction minimum a sinθ = mλ coincides with interference maximum d sinθ = nλ. Thus n = m(d/a) = 3m; orders 3, 6, 9, ... are missing.
Two slit intensities are 4 and 4 units. Find Imax and Imin.
Answer: Imax = 16, Imin = 0
Step-by-step solution: Imax = (√I₁+√I₂)² and Imin = (√I₁−√I₂)². Substitution gives the stated values.
At a point, path difference Δ = 0.75λ. Find phase difference φ.
Answer: 1.50π rad
Step-by-step solution: φ = (2π/λ)Δ = 2π(0.75) = 1.50π rad.
For λ = 650 nm, D = 1 m and d = 0.5 mm, find β.
Answer: 1.300 mm
Step-by-step solution: β = λD/d = (650×10⁻⁹×1)/(0.5×10⁻³) = 1.300e-3 m = 1.300 mm.
If β = 1.40 mm, find the position of the 5th bright fringe.
Answer: 7.00 mm
Step-by-step solution: xₙ = nβ = 5 × 1.40 = 7.00 mm.
Academic note: These are original questions in the requested examination patterns, not verbatim reproductions of copyrighted papers.
A. Δ
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. φ
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δ = xd/D
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ = nλ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. Δ = (2n−1)λ/2
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. xₙ = nλD/d
A. frequency changes at every fringe
B. β is independent of wavelength
C. xₙ = (2n−1)λD/(2d)
D. fringe width equals λd/D
A. β is independent of wavelength
B. β = λD/d
C. fringe width equals λd/D
D. frequency changes at every fringe
A. λ/d
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δp = (μ−1)t
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δx = D(μ−1)t/d
D. fringe width equals λd/D
A. β is independent of wavelength
B. β′ = β/μ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. I = 4I₀cos²(φ/2)
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. bright
A. frequency changes at every fringe
B. β is independent of wavelength
C. pattern shifts but β stays unchanged
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. φ
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δ = xd/D
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δ = nλ
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ = (2n−1)λ/2
C. fringe width equals λd/D
D. frequency changes at every fringe
A. xₙ = nλD/d
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. xₙ = (2n−1)λD/(2d)
A. frequency changes at every fringe
B. β is independent of wavelength
C. β = λD/d
D. fringe width equals λd/D
A. β is independent of wavelength
B. λ/d
C. fringe width equals λd/D
D. frequency changes at every fringe
A. Δp = (μ−1)t
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δx = D(μ−1)t/d
A. frequency changes at every fringe
B. β is independent of wavelength
C. β′ = β/μ
D. fringe width equals λd/D
A. β is independent of wavelength
B. I = 4I₀cos²(φ/2)
C. fringe width equals λd/D
D. frequency changes at every fringe
A. bright
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. pattern shifts but β stays unchanged
A. Δ
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. φ
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δ = xd/D
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ = nλ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. Δ = (2n−1)λ/2
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. xₙ = nλD/d
A. frequency changes at every fringe
B. β is independent of wavelength
C. xₙ = (2n−1)λD/(2d)
D. fringe width equals λd/D
A. β is independent of wavelength
B. β = λD/d
C. fringe width equals λd/D
D. frequency changes at every fringe
A. λ/d
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δp = (μ−1)t
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δx = D(μ−1)t/d
D. fringe width equals λd/D
A. β is independent of wavelength
B. β′ = β/μ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. I = 4I₀cos²(φ/2)
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. bright
A. frequency changes at every fringe
B. β is independent of wavelength
C. pattern shifts but β stays unchanged
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. φ
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δ = xd/D
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δ = nλ
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ = (2n−1)λ/2
C. fringe width equals λd/D
D. frequency changes at every fringe
A. xₙ = nλD/d
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. xₙ = (2n−1)λD/(2d)
A. frequency changes at every fringe
B. β is independent of wavelength
C. β = λD/d
D. fringe width equals λd/D
A. β is independent of wavelength
B. λ/d
C. fringe width equals λd/D
D. frequency changes at every fringe
A. Δp = (μ−1)t
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δx = D(μ−1)t/d
A. frequency changes at every fringe
B. β is independent of wavelength
C. β′ = β/μ
D. fringe width equals λd/D
A. β is independent of wavelength
B. I = 4I₀cos²(φ/2)
C. fringe width equals λd/D
D. frequency changes at every fringe
A. bright
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. pattern shifts but β stays unchanged
A. Δ
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. φ
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δ = xd/D
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ = nλ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. Δ = (2n−1)λ/2
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. xₙ = nλD/d
A. frequency changes at every fringe
B. β is independent of wavelength
C. xₙ = (2n−1)λD/(2d)
D. fringe width equals λd/D
A. β is independent of wavelength
B. β = λD/d
C. fringe width equals λd/D
D. frequency changes at every fringe
A. λ/d
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δp = (μ−1)t
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δx = D(μ−1)t/d
D. fringe width equals λd/D
A. β is independent of wavelength
B. β′ = β/μ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. I = 4I₀cos²(φ/2)
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. bright
A. frequency changes at every fringe
B. β is independent of wavelength
C. pattern shifts but β stays unchanged
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. φ
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δ = xd/D
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δ = nλ
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ = (2n−1)λ/2
C. fringe width equals λd/D
D. frequency changes at every fringe
A. xₙ = nλD/d
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. xₙ = (2n−1)λD/(2d)
A. frequency changes at every fringe
B. β is independent of wavelength
C. β = λD/d
D. fringe width equals λd/D
A. β is independent of wavelength
B. λ/d
C. fringe width equals λd/D
D. frequency changes at every fringe
A. Δp = (μ−1)t
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δx = D(μ−1)t/d
A. frequency changes at every fringe
B. β is independent of wavelength
C. β′ = β/μ
D. fringe width equals λd/D
A. β is independent of wavelength
B. I = 4I₀cos²(φ/2)
C. fringe width equals λd/D
D. frequency changes at every fringe
A. bright
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. pattern shifts but β stays unchanged
A. Δ
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. φ
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δ = xd/D
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ = nλ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. Δ = (2n−1)λ/2
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. xₙ = nλD/d
A. frequency changes at every fringe
B. β is independent of wavelength
C. xₙ = (2n−1)λD/(2d)
D. fringe width equals λd/D
A. β is independent of wavelength
B. β = λD/d
C. fringe width equals λd/D
D. frequency changes at every fringe
A. λ/d
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δp = (μ−1)t
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δx = D(μ−1)t/d
D. fringe width equals λd/D
A. β is independent of wavelength
B. β′ = β/μ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. I = 4I₀cos²(φ/2)
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. bright
A. frequency changes at every fringe
B. β is independent of wavelength
C. pattern shifts but β stays unchanged
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. φ
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δ = xd/D
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δ = nλ
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ = (2n−1)λ/2
C. fringe width equals λd/D
D. frequency changes at every fringe
A. xₙ = nλD/d
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. xₙ = (2n−1)λD/(2d)
A. frequency changes at every fringe
B. β is independent of wavelength
C. β = λD/d
D. fringe width equals λd/D
A. β is independent of wavelength
B. λ/d
C. fringe width equals λd/D
D. frequency changes at every fringe
A. Δp = (μ−1)t
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δx = D(μ−1)t/d
A. frequency changes at every fringe
B. β is independent of wavelength
C. β′ = β/μ
D. fringe width equals λd/D
A. β is independent of wavelength
B. I = 4I₀cos²(φ/2)
C. fringe width equals λd/D
D. frequency changes at every fringe
A. bright
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. pattern shifts but β stays unchanged
A. Δ
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. φ
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δ = xd/D
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ = nλ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. Δ = (2n−1)λ/2
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. xₙ = nλD/d
A. frequency changes at every fringe
B. β is independent of wavelength
C. xₙ = (2n−1)λD/(2d)
D. fringe width equals λd/D
A. β is independent of wavelength
B. β = λD/d
C. fringe width equals λd/D
D. frequency changes at every fringe
A. λ/d
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δp = (μ−1)t
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δx = D(μ−1)t/d
D. fringe width equals λd/D
A. β is independent of wavelength
B. β′ = β/μ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. I = 4I₀cos²(φ/2)
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. bright
A. frequency changes at every fringe
B. β is independent of wavelength
C. pattern shifts but β stays unchanged
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. φ
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δ = xd/D
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δ = nλ
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ = (2n−1)λ/2
C. fringe width equals λd/D
D. frequency changes at every fringe
A. Δ
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. φ
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δ = xd/D
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ = nλ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. Δ = (2n−1)λ/2
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. xₙ = nλD/d
A. frequency changes at every fringe
B. β is independent of wavelength
C. xₙ = (2n−1)λD/(2d)
D. fringe width equals λd/D
A. β is independent of wavelength
B. β = λD/d
C. fringe width equals λd/D
D. frequency changes at every fringe
A. λ/d
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δp = (μ−1)t
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δx = D(μ−1)t/d
D. fringe width equals λd/D
A. β is independent of wavelength
B. β′ = β/μ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. I = 4I₀cos²(φ/2)
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. bright
A. frequency changes at every fringe
B. β is independent of wavelength
C. pattern shifts but β stays unchanged
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. φ
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δ = xd/D
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δ = nλ
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ = (2n−1)λ/2
C. fringe width equals λd/D
D. frequency changes at every fringe
A. Δ
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. φ
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δ = xd/D
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ = nλ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. Δ = (2n−1)λ/2
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. xₙ = nλD/d
A. frequency changes at every fringe
B. β is independent of wavelength
C. xₙ = (2n−1)λD/(2d)
D. fringe width equals λd/D
A. β is independent of wavelength
B. β = λD/d
C. fringe width equals λd/D
D. frequency changes at every fringe
A. λ/d
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δp = (μ−1)t
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δx = D(μ−1)t/d
D. fringe width equals λd/D
A. β is independent of wavelength
B. β′ = β/μ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. I = 4I₀cos²(φ/2)
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. bright
A. frequency changes at every fringe
B. β is independent of wavelength
C. pattern shifts but β stays unchanged
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ
C. fringe width equals λd/D
D. frequency changes at every fringe
A. φ
B. fringe width equals λd/D
C. frequency changes at every fringe
D. β is independent of wavelength
A. fringe width equals λd/D
B. frequency changes at every fringe
C. β is independent of wavelength
D. Δ = xd/D
A. frequency changes at every fringe
B. β is independent of wavelength
C. Δ = nλ
D. fringe width equals λd/D
A. β is independent of wavelength
B. Δ = (2n−1)λ/2
C. fringe width equals λd/D
D. frequency changes at every fringe
Case: A red laser illuminates two narrow slits and clear equally spaced fringes appear.
Complete solution: The laser supplies a nearly monochromatic coherent wavefront; β = λD/d determines the spacing.
Case: A glass plate is inserted before S₁.
Complete solution: Additional path Δp = (μ−1)t shifts the pattern toward S₁; β is unchanged.
Case: The whole apparatus is immersed in water.
Complete solution: Wavelength becomes λ/μ, so β′ = β/μ.
Case: The screen distance is doubled.
Complete solution: β doubles because β = λD/d; angular spacing stays λ/d.
Case: The illuminating source is moved upward.
Complete solution: A constant initial path difference shifts the full pattern; β remains unchanged.
Case: Slit separation is five times slit width.
Complete solution: Every fifth interference maximum coincides with a diffraction minimum.
Case: One slit has four times the intensity of the other.
Complete solution: Amplitude ratio is 2:1, so minima are not completely dark and visibility is 0.8.
Case: White light replaces monochromatic light.
Complete solution: At Δ = 0 every wavelength is constructive, producing a white central fringe.
Case: Fringe width, D and d are measured.
Complete solution: Use λ = βd/D to determine the wavelength.
Case: A sheet of known thickness produces a measured shift.
Complete solution: From Δx = D(μ−1)t/d, calculate μ.
Case: A film causes N fringe shifts.
Complete solution: Optical path change equals Nλ, so t = Nλ/(μ−1).
Case: Red and blue light illuminate the slits.
Complete solution: Each wavelength creates its own fringe spacing; red fringes are wider.
Case: One slit plate vibrates slightly.
Complete solution: Changing path difference moves fringes and reduces time-averaged contrast.
Case: Two separated apertures observe a star.
Complete solution: Fringe visibility and spacing reveal angular size or separation.
Case: A central maximum is monitored while a plate is rotated.
Complete solution: Changing optical thickness changes Δ and shifts the pattern precisely.
A. Both true; Reason correctly explains Assertion
B. Both true; Reason does not 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 explain Assertion
C. Assertion true; Reason false
D. Assertion false; Reason true
Δ = nλ
Δ = (2n−1)λ/2
β = λD/d
Δx = β(μ−1)t/λ
β′ = β/μ
Δ = path difference; φ = phase difference.