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Question 74 of 83

Q.For questions 13 to 16, two statements are given – one labelled Assertion (A) and the other labelled Reason (R). Select the correct answer from the codes (A), (B), (C) and (D) below: (A) Both Assertion (A) and Reason (R) are true and Reason (R) is the correct explanation of the Assertion (A). (B) Both Assertion (A) and Reason (R) are true, but Reason (R) is not the correct explanation of the Assertion (A). (C) Assertion (A) is true, but Reason (R) is false. (D) Both Assertion (A) and Reason (R) are false. Assertion (A) : If accelerated electrons are passed through a narrow slit, a diffraction pattern is observed. Reason (R) : Electrons behave as both particles and waves.

CBSECBSE Class XII Board 2026MCQ· 1mImportance★★★★★
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Electrons exhibit wave-particle duality; their wave nature (de Broglie wavelength) causes diffraction when passing through narrow slits, just like light waves. Both statements are true, and the Reason correctly explains the Assertion.

Understanding Wave-Particle Duality

The heart of this question lies in one of quantum mechanics' most profound insights: matter at the atomic scale doesn't fit neatly into our classical categories of "particle" or "wave." Louis de Broglie proposed in 1924 that every moving particle has an associated wavelength, given by

λ=hp=hmv\lambda = \frac{h}{p} = \frac{h}{mv}

where hh is Planck's constant, pp is momentum, mm is mass, and vv is velocity.

When we accelerate electrons, we increase their momentum. Yet even at high speeds, electrons retain a measurable de Broglie wavelength—typically on the order of angstroms for electrons accelerated through a few hundred volts. This wavelength is comparable to the spacing between atoms in crystals or the width of carefully engineered slits.

Examining the Assertion

Assertion (A): If accelerated electrons are passed through a narrow slit, a diffraction pattern is observed.

This is experimentally verified and true. The classic demonstration is the Davisson-Germer experiment (1927), which showed electron diffraction from crystal lattices. More dramatically, modern versions of the double-slit experiment with electrons—sending them one at a time—build up an interference pattern on a detector screen over time.

Diffraction occurs when waves encounter obstacles or apertures comparable to their wavelength. The electron beam, despite being composed of particles with mass and charge, produces the characteristic bright and dark fringes we associate with wave phenomena. The central maximum, secondary maxima, and minima all appear exactly as wave theory predicts.

For single-slit diffraction, minima occur at angles θ\theta satisfying:

asin⁡θ=nλa \sin\theta = n\lambda

where aa is the slit width, n=1,2,3,…n = 1, 2, 3, \ldots, and λ\lambda is the de Broglie wavelength.

Examining the Reason

Reason (R): Electrons behave as both particles and waves.

This is the principle of wave-particle duality, a cornerstone of quantum mechanics. It is unequivocally true.

Electrons exhibit particle properties: they have definite mass (9.11×10−319.11 \times 10^{-31} kg), charge (−1.6×10−19-1.6 \times 10^{-19} C), and produce localized impacts on detectors (you can count individual electron arrivals). Simultaneously, they exhibit wave properties: they diffract, interfere, and possess a wavelength and frequency.

Neither description alone is complete. The electron is a quantum object, and which aspect we observe depends on the experimental setup. When we look for particle behavior (measuring position or momentum), we find particles. When we create conditions for wave behavior (slits, crystals), we observe diffraction and interference. …

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