Dual Nature of Matter: NEET MCQs with Answers
15 free questions on Dual Nature of Matter for NEET (UG), starting with previous-year NEET and AIPMT questions. Try each one, then tap Show answer for the answer and a short explanation.
Syllabus covered: Dual nature of matter, de Broglie's relationship. Heisenberg uncertainty principle.
Question 1
Previous-year questionThe uncertainty in the position of an electron (mass of an electron = 9.1 × 10⁻²⁸ g) moving with a velocity of 3 × 10⁴ cm/s, accurate up to 0.001%, will be (use h/4π in the uncertainty expression, where h = 6.626 × 10⁻²⁷ erg s) [AIPMT 1995]
- 1.93 cm
- 3.84 cm
- 5.76 cm
- 7.68 cm
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Answer: (A) 1.93 cm
Explanation: First find the uncertainty in velocity from the stated accuracy: Δv = 0.001% of (3 × 10⁴) = (0.001/100) × 3 × 10⁴ = 0.3 cm s⁻¹. Then apply Δx = h/(4πmΔv). All quantities are in CGS units, so the answer emerges in cm. Denominator = 4 × 3.14 × (9.1 × 10⁻²⁸) × 0.3 = 3.429 × 10⁻²⁷. Δx = (6.626 × 10⁻²⁷)/(3.429 × 10⁻²⁷) = 1.93 cm. Striking result: knowing the electron’s speed to within 0.001% leaves its position uncertain by almost 2 cm — enormously larger than an atom.
Question 2
Previous-year questionThe momentum of a particle having a de-Broglie wavelength of 10⁻¹⁷ m is (Given h = 6.625 × 10⁻³⁴ Js) [AIPMT 1996]
- 3.3125 × 10⁻⁷ kg m s⁻¹
- 26.5 × 10⁻⁷ kg m s⁻¹
- 6.625 × 10⁻¹⁷ kg m s⁻¹
- 13.25 × 10⁻¹⁷ kg m s⁻¹
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Answer: (C) 6.625 × 10⁻¹⁷ kg m s⁻¹
Explanation: The de-Broglie relation can be written directly in terms of momentum: λ = h/p, so p = h/λ. p = (6.625 × 10⁻³⁴)/(10⁻¹⁷) = 6.625 × 10⁻³⁴ × 10¹⁷ = 6.625 × 10⁻¹⁷ kg m s⁻¹. Neither the mass nor the velocity is needed — momentum follows from the wavelength alone.
Question 3
Previous-year questionThe position of both an electron and a helium atom is known within 1.0 mm. Further, the momentum of the electron is known within 5.0 × 10⁻²⁶ kg ms⁻¹. The minimum uncertainty in the measurement of the momentum of the helium atom is [AIPMT 1998]
- 50 kg ms⁻¹
- 80 kg ms⁻¹
- 80 × 10⁻²⁶ kg ms⁻¹
- 5.0 × 10⁻²⁶ kg ms⁻¹
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Answer: (D) 5.0 × 10⁻²⁶ kg ms⁻¹
Explanation: Heisenberg’s uncertainty principle, Δx · Δp ≥ h/4π, contains NO reference to the mass or identity of the particle. Since the position of the helium atom is known to the same precision (1.0 mm) as that of the electron, the right-hand side h/4π is unchanged. Therefore the minimum uncertainty in momentum must also be the same: Δp = 5.0 × 10⁻²⁶ kg ms⁻¹. Trap: the heavier mass of helium tempts students to scale the answer, but momentum uncertainty depends only on the positional uncertainty.
Question 4
Previous-year questionThe uncertainty in the momentum of an electron is 1 × 10⁻⁵ kg m/s. The uncertainty in its position will be (Given h = 6.62 × 10⁻³⁴ kg m²/s) [AIPMT 1999]
- 1.05 × 10⁻²⁸ m
- 1.05 × 10⁻²⁶ m
- 5.27 × 10⁻³⁰ m
- 5.25 × 10⁻²⁸ m
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Answer: (C) 5.27 × 10⁻³⁰ m
Explanation: From Δx · Δp ≥ h/4π, the minimum uncertainty in position is Δx = h/(4πΔp). Taking π = 22/7: Δx = (6.62 × 10⁻³⁴ × 7)/(4 × 22 × 1 × 10⁻⁵) = (46.34 × 10⁻³⁴)/(88 × 10⁻⁵) = 5.265 × 10⁻³⁰ ≈ 5.27 × 10⁻³⁰ m.
Question 5
Previous-year questionThe de-Broglie wavelength of a particle with mass 1 g and velocity 100 m/s is [AIPMT 1999]
- 6.63 × 10⁻³³ m
- 6.63 × 10⁻³⁴ m
- 6.63 × 10⁻³⁵ m
- 6.65 × 10⁻³⁶ m
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Answer: (A) 6.63 × 10⁻³³ m
Explanation: λ = h/mv, where all quantities must be in SI units. Convert the mass: m = 1 g = 1 × 10⁻³ kg. λ = (6.63 × 10⁻³⁴)/(10⁻³ × 100) = (6.63 × 10⁻³⁴)/(10⁻¹) = 6.63 × 10⁻³³ m. Common error: forgetting to convert grams to kilograms, which shifts the answer by three powers of ten.
Question 6
Previous-year questionGiven that the mass of an electron is 9.11 × 10⁻³¹ kg and Planck’s constant is 6.626 × 10⁻³⁴ Js, the uncertainty involved in the measurement of velocity within a distance of 0.1 Å is [AIPMT 2006]
- 5.79 × 10⁶ ms⁻¹
- 5.79 × 10⁷ ms⁻¹
- 5.79 × 10⁸ ms⁻¹
- 5.79 × 10⁵ ms⁻¹
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Answer: (A) 5.79 × 10⁶ ms⁻¹
Explanation: From Δx · mΔv = h/4π, we get Δv = h/(4πmΔx). Convert the distance: Δx = 0.1 Å = 0.1 × 10⁻¹⁰ m = 1 × 10⁻¹¹ m. Denominator = 4 × 3.14 × (9.11 × 10⁻³¹) × (1 × 10⁻¹¹) = 1.144 × 10⁻⁴⁰. Δv = (6.626 × 10⁻³⁴)/(1.144 × 10⁻⁴⁰) = 5.79 × 10⁶ ms⁻¹. Note how large this is — confining an electron to atomic dimensions makes its velocity almost completely indeterminate, which is the essence of the uncertainty principle.
Question 7
Previous-year questionIf the uncertainty in position and the uncertainty in momentum are equal, then the uncertainty in velocity is [AIPMT 2008]
- (1/2m)√(h/π)
- √(h/2π)
- (1/m)√(h/π)
- √(h/π)
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Answer: (A) (1/2m)√(h/π)
Explanation: Heisenberg’s uncertainty principle: Δx · Δp = h/4π. Given the condition Δx = Δp, substituting gives (Δp)² = h/4π. Since Δp = mΔv, we get m²(Δv)² = h/4π ⇒ (Δv)² = h/(4πm²) ⇒ Δv = (1/2m)√(h/π). The factor of ½ emerges from taking the square root of the 4 in the denominator.
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Question 8
Previous-year questionThe measurement of the electron position is associated with an uncertainty in momentum which is equal to 1 × 10⁻¹⁸ g cm s⁻¹. The uncertainty in electron velocity is (mass of an electron = 9 × 10⁻²⁸ g) [AIPMT 2008]
- 1 × 10⁹ cm s⁻¹
- 1 × 10⁶ cm s⁻¹
- 1 × 10⁵ cm s⁻¹
- 1 × 10¹¹ cm s⁻¹
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Answer: (A) 1 × 10⁹ cm s⁻¹
Explanation: Momentum and velocity are related by Δp = m × Δv, so Δv = Δp/m. Both quantities are already in the same (CGS) system of units, so no conversion is needed. Δv = (1 × 10⁻¹⁸ g cm s⁻¹)/(9 × 10⁻²⁸ g) = 0.111 × 10¹⁰ ≈ 1 × 10⁹ cm s⁻¹. The uncertainty principle itself is not needed here — only the definition of momentum.
Question 9
Previous-year questionA 0.66 kg ball is moving with a speed of 100 m/s. The associated wavelength will be (h = 6.6 × 10⁻³⁴ Js) [AIPMT 2010]
- 6.6 × 10⁻³² m
- 6.6 × 10⁻³⁴ m
- 1.0 × 10⁻³⁵ m
- 1.0 × 10⁻³² m
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Answer: (C) 1.0 × 10⁻³⁵ m
Explanation: The de-Broglie relation is λ = h/mv. λ = (6.6 × 10⁻³⁴)/(0.66 × 100) = (6.6 × 10⁻³⁴)/66 = 1.0 × 10⁻³⁵ m. This vanishingly small wavelength is precisely why wave behaviour is never observed for macroscopic objects — it is far too small to be detected by any experiment.
Question 10
Previous-year questionWhich one is the wrong statement? [NEET 2017]
- de-Broglie’s wavelength is given by λ = h/mv, where m = mass of the particle and v = group velocity of the particle
- The uncertainty principle is ΔE × Δt ≥ h/4π
- Half-filled and fully filled orbitals have greater stability due to greater exchange energy, greater symmetry and a more balanced arrangement
- The energy of the 2s-orbital is less than the energy of the 2p-orbital in the case of hydrogen-like atoms
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Answer: (D) The energy of the 2s-orbital is less than the energy of the 2p-orbital in the case of hydrogen-like atoms
Explanation: A hydrogen-like (one-electron) species has no shielding, so orbital energy depends only on n and the 2s and 2p orbitals are degenerate; this statement is therefore wrong (it is true only for multi-electron atoms). The de Broglie relation, ΔE·Δt ≥ h/4π, and the extra stability of half-filled and fully filled orbitals are correct.
Question 11
Previous-year questionIn a hydrogen atom, the de-Broglie wavelength of an electron in the second Bohr orbit is [Given that Bohr radius, a₀ = 52.9 pm] [NEET (Odisha) 2019]
- 211.6 pm
- 211.6π pm
- 52.9π pm
- 105.8 pm
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Answer: (B) 211.6π pm
Explanation: From mvr = nh/2π and λ = h/mv, 2πr = nλ. For n = 2, r = 52.9 × 2² = 211.6 pm, so λ = 2π(211.6)/2 = 211.6π pm.
Question 12
Previous-year questionA particular station of All India Radio, New Delhi, broadcasts on a frequency of 1368 kHz (kilohertz). The wavelength of the electromagnetic radiation emitted by the transmitter is [Speed of light, c = 3.0 × 10⁸ ms⁻¹] [NEET 2021]
- 219.3 m
- 219.2 m
- 2192 m
- 21.92 cm
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Answer: (A) 219.3 m
Explanation: Convert the frequency to SI: ν = 1368 kHz = 1368 × 10³ s⁻¹ = 1.368 × 10⁶ s⁻¹. Using c = νλ, λ = c/ν: λ = (3.0 × 10⁸ m s⁻¹)/(1.368 × 10⁶ s⁻¹) = 219.3 m. A wavelength of a few hundred metres is exactly what is expected for the medium-wave radio band.
Question 13
In a hydrogen-like atom, an electron occupies the lowest shell that contains an orbital with magnetic quantum number m = −3. Treating that shell as a Bohr orbit, how many de Broglie wavelengths fit in its circumference?
- 4
- 3
- 1
- 7
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Answer: (A) 4
Explanation: An m value of −3 needs l ≥ 3, and since l ≤ n − 1, the lowest such shell has n = 4. In the nth Bohr orbit the circumference equals nλ, so 4 de Broglie wavelengths fit.
Question 14
The de Broglie wavelength of a moving particle A is 3.0 × 10⁻¹⁰ m. What is the de Broglie wavelength of particle B, whose momentum is one-third that of A?
- 3.0 × 10⁻¹⁰ m
- 1.0 × 10⁻¹⁰ m
- 2.7 × 10⁻⁹ m
- 9.0 × 10⁻¹⁰ m
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Answer: (D) 9.0 × 10⁻¹⁰ m
Explanation: The de Broglie wavelength is λ = h/p, so it is inversely proportional to momentum. Reducing the momentum to one-third makes the wavelength three times larger: 3 × 3.0 × 10⁻¹⁰ = 9.0 × 10⁻¹⁰ m.
Question 15
Assertion: A broadcast can report both the position and the speed of a racing motorbike at one instant to high precision, without conflict with the Heisenberg uncertainty principle. Reason: Since Δx · Δv ≥ h/(4πm), the limit set by the principle becomes negligibly small for a body of large mass.
- Both Assertion and Reason are false
- Both Assertion and Reason are true, and Reason is the correct explanation of Assertion
- Both Assertion and Reason are true, but Reason is not the correct explanation of Assertion
- Assertion is true, but Reason is false
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Answer: (B) Both Assertion and Reason are true, and Reason is the correct explanation of Assertion
Explanation: The principle applies to all moving bodies, but the product of the uncertainties varies inversely with mass. For a body of several hundred kilograms h/(4πm) is so tiny that it lies far below anything measurable. The practical limit on a motorbike's data is the measuring equipment, not the principle, so the principle matters only for microscopic particles such as electrons.
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