Q3
(a) Find out the difference in frequencies of Lyman-alpha line in hydrogen and deuterium atoms. 15 marks (b) The Stern-Gerlach experiment is a landmark experiment in quantum mechanics. Discuss about the most important findings of this experiment. 15 marks (c) (i) From the pure rotational absorption spectra of a diatomic molecule (HF), the wave number difference between the consecutive rotational lines is found to be Δν̄ = 4050 m⁻¹. Calculate the following: (1) Rotational constant (2) Moment of inertia (3) Distance between two atoms (bond length) [Given, M_H = 1 u, M_F = 19 u] 10 marks (ii) The force constant of HCl molecule is 4.8×10⁵ dyne/cm. Calculate the wave numbers of Stokes and anti-Stokes lines, when excited with a radiation of wavelength 4358 Å. [Given, μ_HCl = 1.61×10⁻²⁴ g] 10 marks
हिंदी में प्रश्न पढ़ें
(a) हाइड्रोजन व ड्यूटीरियम परमाणुओं के लिए लाइमेन-अल्फा लाइन की आवृत्तियों में अंतर ज्ञात कीजिए। 15 अंक (b) स्टर्न-गार्लेक प्रयोग, क्वांटम यांत्रिकी का एक अति विशिष्ट प्रयोग है। इस प्रयोग के अति महत्वपूर्ण निष्कर्षों पर चर्चा कीजिए। 15 अंक (c) (i) एक डाइपरमाणुक अणु (HF) के विद्युद् घुर्णी अवशोषण स्पेक्ट्रम से दो क्रमागत घुर्णी लाइनों की तरंग संख्याओं का अंतर Δν̄ = 4050 m⁻¹ पाया जाता है। निम्नलिखित की गणना कीजिए: (1) घुर्णी स्थिरांक (2) जड़त्व आघूर्ण (3) दो परमाणुओं के बीच की दूरी (आबंध लंबाई) [दिया गया है, M_H = 1 u, M_F = 19 u] 10 अंक (ii) HCl अणु का बल स्थिरांक 4.8×10⁵ dyne/cm है। स्टोक्स और प्रति-स्टोक्स रेखाओं की तरंग संख्याओं की गणना कीजिए, जब 4358 Å तरंगदैर्घ्य के विकिरण द्वारा उत्तेजित की जाएं। [दिया गया है, μ_HCl = 1.61×10⁻²⁴ g] 10 अंक
Directive word: Calculate
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How this answer will be evaluated
Approach
Begin with the directive to calculate and discuss across four sub-parts: spend ~30% time on (a) isotope shift calculation using reduced mass correction; ~25% on (b) discussing Stern-Gerlach findings with experimental schematic; ~25% on (c)(i) rotational spectroscopy of HF; and ~20% on (c)(ii) Raman spectroscopy of HCl. Structure as: brief theory → step-by-step derivation → numerical substitution → final result with units → physical significance.
Key points expected
- (a) Reduced mass calculation for H (μ_H) and D (μ_D), Rydberg formula with reduced mass correction, frequency difference Δν = ν_H − ν_D ≈ 4.53×10¹¹ Hz or equivalent
- (b) Experimental setup with inhomogeneous magnetic field, silver atom beam splitting into two discrete components, direct evidence of space quantization and electron spin (intrinsic angular momentum ℏ/2)
- (c)(i) Rotational constant B = Δν̄/2 = 2025 m⁻¹, moment of inertia I = h/(8π²cB), bond length r₀ = √(I/μ) ≈ 0.92 Å for HF
- (c)(ii) Vibrational frequency ω = (1/2π)√(k/μ), Raman shift Δν̄ = ±(ν₀ ∓ ν_vib), Stokes and anti-Stokes lines at ν̄₀ − ν̄_vib and ν̄₀ + ν̄_vib respectively
- Proper unit conversions throughout: CGS to SI for (c)(ii), unified atomic mass to kg, wavenumber to frequency where needed
- Physical significance: isotope shift tests QED predictions, Stern-Gerlach validates quantum mechanics vs classical expectations, spectroscopic constants determine molecular structure
Evaluation rubric
| Dimension | Weight | Max marks | Excellent | Average | Poor |
|---|---|---|---|---|---|
| Concept correctness | 20% | 10 | Correctly identifies reduced mass dependence in (a), space quantization and spin-½ in (b), rigid rotor model in (c)(i), and Raman scattering mechanism with selection rules in (c)(ii); no conceptual errors in any sub-part | Minor errors like using atomic mass instead of reduced mass in (a), confusing orbital and spin angular momentum in (b), or misapplying vibrational frequency formula in (c)(ii) | Fundamental misconceptions such as ignoring reduced mass entirely, attributing Stern-Gerlach splitting to orbital angular momentum only, or treating Raman as fluorescence process |
| Derivation rigour | 20% | 10 | Complete step-by-step derivations: reduced mass substitution in Rydberg formula, force equation for beam deflection, rotational energy levels J(J+1)ħ²/2I, and vibrational frequency from classical harmonic oscillator; all steps logically connected | Correct final formulas but skips key steps like showing how Δν̄ = 2B arises from selection rule ΔJ = ±1, or assumes Raman shift without deriving from polarizability | Plugs numbers without showing any derivation, or presents garbled derivations with dimensional inconsistencies and missing physical justification |
| Diagram / FBD | 15% | 7.5 | Clear labeled diagram for Stern-Gerlach apparatus in (b) showing magnet geometry, beam source, screen with doublet splitting; energy level diagrams for rotational transitions in (c)(i) and Raman process in (c)(ii) | Basic Stern-Gerlach sketch without labels or missing beam path; no energy level diagrams for spectroscopic parts | No diagrams despite (b) requiring experimental visualization, or completely incorrect schematic showing continuous beam spreading |
| Numerical accuracy | 25% | 12.5 | Precise calculations: Δν ≈ 4.5×10¹¹ Hz for (a), B = 2025 m⁻¹, I ≈ 1.37×10⁻⁴⁷ kg·m², r₀ ≈ 0.917 Å for HF; ν̄_vib ≈ 2885 cm⁻¹, Stokes at ~4167 cm⁻¹ and anti-Stokes at ~4550 cm⁻¹ for HCl; proper significant figures and unit handling | Correct method but arithmetic errors like wrong powers of 10, mixing CGS-SI units without conversion, or bond length off by factor of √2 due to reduced mass error | Order-of-magnitude errors, missing unit conversions (especially dyne/cm to N/m), or nonsensical results like bond length in meters without Å conversion |
| Physical interpretation | 20% | 10 | Interprets (a) as test of nuclear motion effects and QED; (b) as definitive proof of quantization and electron spin; (c)(i)-(ii) as structural determination tools; connects to Indian research context (e.g., Raman effect discovery by C.V. Raman at IISc, 1930 Nobel) | States results without explaining why they matter; mentions Raman effect without acknowledging Indian scientific heritage | Purely mathematical treatment with no physical insight; fails to distinguish spectroscopic techniques or their applications |
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