Diffraction — NEET Physics MCQs with Solutions
Free NEET Physics Diffraction MCQs with step-by-step solutions (42 questions). Part of Interference and Diffraction of Light. Practise online on Prepizo — no login needed.
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Questions with solutions
Q1 — Diffraction · easy · theory
Diffraction of light is the phenomenon of:
A. Bending of light around the edges of an obstacle or aperture ✓ Correct
B. Rotation of the plane of vibration
C. Reflection at a polished surface
D. Splitting of white light into colours
Solution: Diffraction is the bending/spreading of light as it passes the edges of an obstacle or a narrow aperture.
Q2 — Diffraction · easy · theory
Diffraction effects become significant when the size of the aperture or obstacle is:
A. Comparable to the wavelength of light ✓ Correct
B. Very much larger than the wavelength
C. Independent of the wavelength
D. Exactly one metre
Solution: Appreciable diffraction occurs only when the obstacle/aperture is of the order of the wavelength of light.
Q3 — Diffraction · easy · theory
For a single slit of width a, the directions of the minima in the diffraction pattern are given by:
A. $a\cos\theta = n\lambda$
B. $a\sin\theta = n\lambda$ (n = 1, 2, …) ✓ Correct
C. $a\sin\theta = (2n+1)\lambda/2$
D. $a\sin\theta = n\lambda/2$
Solution: Single-slit minima occur where a sinθ = nλ, n = 1, 2, 3, …
Q4 — Diffraction · medium · theory
For a single slit, the secondary maxima occur approximately in directions given by:
A. $a\sin\theta = (2n+1)\dfrac{\lambda}{2}$ ✓ Correct
B. $a\sin\theta = n\lambda/4$
C. $a\sin\theta = 2n\lambda$
D. $a\sin\theta = n\lambda$
Solution: Secondary maxima are located roughly where a sinθ = (2n+1)λ/2 (n = 1, 2, …).
Q5 — Diffraction · easy · theory
In a single-slit diffraction pattern, the central maximum is:
A. Absent
B. The brightest and the widest ✓ Correct
C. The dimmest
D. The same width as the others
Solution: The central maximum carries most of the energy — it is the brightest and about twice as wide as the secondary maxima.
Q6 — Diffraction · medium · theory
The angular width of the central maximum in single-slit diffraction (slit width a) is:
A. $\dfrac{2\lambda}{a}$ ✓ Correct
B. $\dfrac{\lambda}{a}$
C. $\dfrac{a}{\lambda}$
D. $\dfrac{\lambda}{2a}$
Solution: The first minima are at sinθ = ±λ/a, so the full angular width of the central maximum is 2λ/a.
Q7 — Diffraction · medium · theory
The linear width of the central maximum on a screen at distance D from a slit of width a is:
A. $\dfrac{2\lambda a}{D}$
B. $\dfrac{\lambda D}{a}$
C. $\dfrac{2\lambda D}{a}$ ✓ Correct
D. $\dfrac{\lambda D}{2a}$
Solution: Linear width = 2λD/a (distance between the first minima on either side of the centre).
Q8 — Diffraction · medium · theory
In a single-slit pattern, the width of the central maximum compared with a secondary maximum is:
A. Four times as wide
B. Twice as wide ✓ Correct
C. Equal
D. Half as wide
Solution: The central maximum spans from −λ/a to +λ/a, twice the width of each secondary maximum.
Q9 — Diffraction · medium · theory
If the width a of the single slit is increased, the central maximum:
A. Stays the same
B. Becomes narrower ✓ Correct
C. Becomes wider
D. Disappears
Solution: Width ∝ 1/a, so a wider slit gives a narrower (and brighter) central maximum.
Q10 — Diffraction · medium · theory
For a single slit, using light of longer wavelength makes the central maximum:
A. Wider ✓ Correct
B. Unchanged
C. Narrower
D. Split into two
Solution: Width ∝ λ, so longer wavelength produces a wider central maximum (red spreads more than violet).
Q11 — Diffraction · medium · numerical
Light of wavelength 600 nm falls on a single slit of width 0.1 mm. The linear width of the central maximum on a screen 1 m away is:
A. 6 mm
B. 24 mm
C. 12 mm ✓ Correct
D. 1.2 mm
Solution: Width = 2λD/a = (2 × 600 × 10⁻⁹ × 1)/(0.1 × 10⁻³) = 1.2 × 10⁻² m = 12 mm.
Q12 — Diffraction · medium · numerical
Light of wavelength 600 nm passes through a slit of width 0.1 mm. The distance of the first minimum from the centre on a screen 1 m away is:
A. 0.6 mm
B. 6 mm ✓ Correct
C. 12 mm
D. 3 mm
Solution: First minimum: y = λD/a = (600 × 10⁻⁹ × 1)/(0.1 × 10⁻³) = 6 × 10⁻³ m = 6 mm.
Q13 — Diffraction · easy · theory
Diffraction of light provides direct evidence for the _____ nature of light.
A. Wave ✓ Correct
B. Particle
C. Corpuscular
D. Quantum
Solution: Diffraction is a characteristic wave phenomenon, so it demonstrates the wave nature of light.
Q14 — Diffraction · medium · theory
Which is a key difference between interference and diffraction fringes?
A. Neither shows any intensity variation
B. Both have exactly equal intensity
C. Interference fringes are equally spaced and of equal intensity; diffraction fringes are unequally spaced with decreasing intensity ✓ Correct
D. Interference fringes have decreasing intensity; diffraction fringes are equally bright
Solution: Interference gives uniform, equally spaced fringes of equal intensity, whereas diffraction gives unequally spaced fringes whose intensity falls off rapidly from the centre.
Q15 — Diffraction · medium · theory
Interference arises from the superposition of waves from _____, while diffraction arises from the superposition of secondary wavelets from _____.
A. the same wavefront; two coherent sources
B. one source; one point
C. two incoherent sources; a single ray
D. two coherent sources; different parts of the same wavefront ✓ Correct
Solution: Interference is the superposition of waves from two coherent sources; diffraction is the superposition of secondary wavelets originating from different parts of the same wavefront.
Q16 — Diffraction · medium · theory
Compared with the central maximum, the intensity of the first secondary maximum in single-slit diffraction is:
A. Equal
B. Much smaller (only a few percent) ✓ Correct
C. Exactly half
D. Slightly greater
Solution: The first secondary maximum has only about 4–5% of the central maximum's intensity; the maxima fade rapidly away from the centre.
Q17 — Diffraction · medium · theory
The Fresnel distance z_F for a beam of width a and wavelength λ is:
A. $\dfrac{a}{\lambda}$
B. $\dfrac{\lambda^2}{a}$
C. $\dfrac{a^2}{\lambda}$ ✓ Correct
D. $\dfrac{\lambda}{a^2}$
Solution: The Fresnel distance is z_F = a²/λ — the distance up to which a beam of width a stays approximately collimated before diffraction spreading dominates.
Q18 — Diffraction · medium · theory
The physical significance of the Fresnel distance is that it is the distance:
A. At which the light becomes polarised
B. Up to which ray (geometric) optics is a good approximation before diffraction spreading becomes appreciable ✓ Correct
C. At which interference stops
D. At which the wavelength doubles
Solution: Beyond the Fresnel distance the diffraction spread of the beam becomes comparable to its size, so ray optics is valid only up to about z_F.
Q19 — Diffraction · medium · theory
For an aperture of 3 mm and light of wavelength 500 nm, the Fresnel distance is:
A. 180 m
B. 1.8 m
C. 18 m ✓ Correct
D. 0.18 m
Solution: z_F = a²/λ = (3 × 10⁻³)²/(500 × 10⁻⁹) = (9 × 10⁻⁶)/(5 × 10⁻⁷) = 18 m.
Q20 — Diffraction · medium · theory
If the slit width is doubled, the width of the central diffraction maximum:
A. Stays the same
B. Doubles
C. Halves ✓ Correct
D. Becomes four times
Solution: Central-maximum width ∝ 1/a, so doubling a halves the width.
Q21 — Diffraction · medium · theory
Sound waves bend around large obstacles far more readily than light waves because:
A. Light cannot diffract at all
B. Sound travels faster
C. Sound is a transverse wave
D. Sound has a much larger wavelength, comparable to everyday obstacles ✓ Correct
Solution: Diffraction is significant when the wavelength is comparable to the obstacle. Sound wavelengths (~metres) match everyday objects, while light's tiny wavelength does not.
Q22 — Diffraction · medium · theory
The angular position of the nth minimum in single-slit diffraction is given by sinθ =
A. $\dfrac{n\lambda}{a}$ ✓ Correct
B. $\dfrac{n\lambda}{2a}$
C. $\dfrac{(2n+1)\lambda}{2a}$
D. $\dfrac{a}{n\lambda}$
Solution: Minima occur at sinθ = nλ/a (n = 1, 2, 3, …).
Q23 — Diffraction · medium · theory
According to the Rayleigh criterion, two point objects are just resolved by an aperture of diameter D when their angular separation is:
A. $\dfrac{1.22\lambda}{D}$ ✓ Correct
B. $\dfrac{2\lambda}{D}$
C. $\dfrac{0.61\lambda}{D}$
D. $\dfrac{\lambda}{D}$
Solution: The Rayleigh criterion gives the limit of resolution (minimum resolvable angular separation) as θ = 1.22λ/D.
Q24 — Diffraction · medium · theory
The resolving power of a telescope (its ability to distinguish two close objects) increases when:
A. The aperture is decreased
B. The aperture (objective diameter) is increased ✓ Correct
C. A longer wavelength is used
D. The eyepiece focal length is increased
Solution: Since the limit of resolution θ = 1.22λ/D, a larger aperture D gives a smaller θ, i.e. higher resolving power.
Q25 — Diffraction · medium · theory
The limit of resolution of an optical instrument improves (gets smaller) if:
A. A longer wavelength of light is used
B. The aperture is made smaller
C. A shorter wavelength of light is used ✓ Correct
D. The intensity is reduced
Solution: θ = 1.22λ/D decreases with smaller λ (and larger D), so shorter wavelengths give finer resolution.
Q26 — Diffraction · medium · numerical
Light of wavelength 500 nm passes through a slit of width 0.2 mm. The angular width of the central maximum is:
A. $1 \times 10^{-2}$ rad
B. $5 \times 10^{-4}$ rad
C. $2.5 \times 10^{-3}$ rad
D. $5 \times 10^{-3}$ rad ✓ Correct
Solution: Angular width = 2λ/a = (2 × 500 × 10⁻⁹)/(0.2 × 10⁻³) = (1 × 10⁻⁶)/(2 × 10⁻⁴) = 5 × 10⁻³ rad.
Q27 — Diffraction · medium · theory
The coloured appearance of the surface of a compact disc (CD) in white light is chiefly due to:
A. Polarisation
B. Simple reflection
C. Diffraction of light by the closely spaced tracks ✓ Correct
D. Total internal reflection
Solution: The finely spaced tracks on a CD act like a diffraction grating, splitting white light into colours by diffraction.
Q28 — Diffraction · medium · theory
As a single slit is made narrower and narrower (approaching the wavelength of light), the diffraction pattern:
A. Is unaffected
B. Disappears
C. Spreads out more widely ✓ Correct
D. Becomes sharper and narrower
Solution: A narrower slit gives a wider central maximum (width ∝ 1/a), so the light spreads out more.
Q29 — Diffraction · easy · theory
In a single-slit diffraction pattern, the point directly opposite the centre of the slit is:
A. A dark fringe
B. The second minimum
C. The first secondary maximum
D. The centre of the bright central maximum ✓ Correct
Solution: At θ = 0 all secondary wavelets arrive in phase, giving the central bright maximum.
Q30 — Diffraction · medium · theory
Which of the following is TRUE about a single-slit diffraction pattern using monochromatic light?
A. There is only one bright fringe and no others
B. The fringes are equally spaced and equally bright
C. The bright fringes are of steadily decreasing intensity on either side of the centre ✓ Correct
D. All bright fringes have equal intensity
Solution: The central maximum is brightest, and the secondary maxima decrease rapidly in intensity as one moves away from the centre.