Q3
(a) Calculate the number of collisions that oxygen makes per second on 1·00 cm² of the surface of the vessel containing them if the pressure is 1·00 × 10⁻⁶ atm and the temperature is 25°C. 10 (b) Suppose that 10·0 J of work is required to create droplets of uniform size from a mole of water in bulk at 25°C and 1 atm pressure. (i) Assuming that surface tension is independent of area, calculate the radius of the droplets. (ii) Calculate the number of water molecules in a droplet. Given : Surface tension of water = 0·072 J/m² 15 (c) You are given the following data for butane : Normal melting point = – 138°C Normal boiling point = 0°C Critical temperature = 152°C Critical pressure = 38 atm Assume that the triple point is slightly lower in temperature than the melting point and that the vapour pressure at the triple point is 3 × 10⁻⁵ torr. (i) Sketch a phase diagram for butane. (ii) Butane at 1 atm and 140°C is compressed to 40 atm. Are two phases present at any time during this process ? (iii) Butane at 1 atm and 200°C is compressed to 40 atm. Are two phases present at any time during this process ? 10 (d) A container with 100 g of ice at 0°C is placed in a humid room whose temperature is 40°C. The ice melts as water vapour condenses into the container. Assuming that all the heat transferred to the container comes from the condensation, how much water will have condensed in the container once all the ice is melted and has reached 40°C ? Given : Heat of fusion of ice = 334 Jg⁻¹ Heat of vaporization of water = 2260 Jg⁻¹ Heat capacity of water = 4184 J kg⁻¹ K⁻¹ 10 (e) Explain why crystalline solids are generally more defective as a result of increasing temperature. 5
हिंदी में प्रश्न पढ़ें
(a) यदि ताप 25°C और दाब 1·00 × 10⁻⁶ atm है, तो 1·00 cm² की सतह वाले बर्तन पर ऑक्सीजन के प्रति सेकंड संघट्टन की संख्या का परिकलन कीजिए। 10 (b) मान लीजिए कि 25°C और 1 atm दाब पर पानी के आयतन (bulk) में से एक मोल पानी से एकसमान आकार के बिंदुक उत्पन्न करने के लिए 10·0 J कार्य अपेक्षित है। (i) यह मानते हुए कि पृष्ठीय तनाव क्षेत्रफल से स्वतंत्र है, बिंदुओं की त्रिज्या का परिकलन कीजिए। (ii) एक बिंदुक में पानी के अणुओं की संख्या का परिकलन कीजिए। दिया गया है : पानी का पृष्ठीय तनाव = 0·072 J/m² 15 (c) आपको ब्यूटेन के लिए निम्नलिखित आँकड़े दिए गए हैं : सामान्य गलनांक = – 138°C सामान्य क्वथनांक = 0°C क्रांतिक ताप = 152°C क्रांतिक दाब = 38 atm मान लीजिए कि त्रिक बिंदु तापमान में सामान्य गलनांक से थोड़ा नीचे है और त्रिक बिंदु पर वाष्प दाब 3 × 10⁻⁵ torr है। (i) ब्यूटेन का प्रावस्था आरेख बनाइए। (ii) 1 atm और 140°C पर ब्यूटेन को 40 atm तक संपीड़ित किया जाता है। क्या इस क्रिया के दौरान किसी भी समय दो अवस्थाएँ उपस्थित होती हैं ? (iii) 1 atm और 200°C पर ब्यूटेन को 40 atm तक संपीड़ित किया जाता है। क्या इस क्रिया के दौरान किसी भी समय दो अवस्थाएँ उपस्थित होती हैं ? 10 (d) एक आर्द्र कमरा जिसका तापमान 40°C है, उसमें एक डिब्बे में 0°C पर 100 g बर्फ रखी गई है। जल वाष्प डिब्बे के अंदर संघनित होने से बर्फ पिघलती है। यह मानते हुए कि डिब्बे के अंदर सारी ऊष्मा का स्थानांतरण संघनन से होता है, डिब्बे में कितना जल संघनित होगा जब सारी बर्फ पिघल जाए और उसका तापमान 40°C तक पहुँच जाए ? दिया गया है : बर्फ की संगलन ऊष्मा = 334 Jg⁻¹ जल की वाष्पन ऊष्मा = 2260 Jg⁻¹ जल की ऊष्मा धारिता = 4184 J kg⁻¹ K⁻¹ 10 (e) व्याख्या कीजिए कि बढ़ते तापमान के परिणामस्वरूप क्रिस्टलीय ठोस सामान्यतः अधिक दोषपूर्ण क्यों होते हैं। 5
Directive word: Calculate
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How this answer will be evaluated
Approach
Begin with the directive to calculate across all sub-parts, showing systematic problem-solving. Allocate approximately 20% time to part (a) on collision theory, 30% to part (b) on surface tension and droplet formation, 20% to part (c) on phase diagrams with careful sketching, 20% to part (d) on thermal equilibrium calculations, and 10% to part (e) on crystal defects. Structure as: brief statement of principles → step-by-step calculations with units → labeled diagram for (c) → concluding physical interpretation of results.
Key points expected
- Part (a): Apply kinetic theory of gases using Z = (P/√(2πmkT)) × N_A to find collision frequency per unit area, converting pressure to SI units and using O₂ molecular mass
- Part (b)(i): Use work of surface creation W = γ × ΔA = γ × n × 4πr² with n droplets from total surface area to solve for droplet radius
- Part (b)(ii): Calculate molecules per droplet using droplet volume, water density, and Avogadro's number
- Part (c)(i): Sketch phase diagram with correctly positioned triple point (-138°C, 3×10⁻⁵ torr), critical point (152°C, 38 atm), and phase boundaries showing solid-liquid line with negative slope
- Part (c)(ii)-(iii): Analyze compression paths relative to critical point to determine phase coexistence, noting 140°C < T_c and 200°C > T_c
- Part (d): Set up energy balance: heat from condensation = heat for fusion + heating water, solving for condensed mass using latent heats and specific heat
- Part (e): Explain Schottky and Frenkel defect formation with Arrhenius-type temperature dependence, citing Boltzmann factor for defect concentration
- Physical interpretation: Connect numerical results to real phenomena (e.g., droplet stability in clouds, LPG storage conditions, humidity effects)
Evaluation rubric
| Dimension | Weight | Max marks | Excellent | Average | Poor |
|---|---|---|---|---|---|
| Concept correctness | 20% | 10 | Demonstrates precise understanding of kinetic theory assumptions for (a), surface thermodynamics for (b), phase rule and critical phenomena for (c), calorimetry principles for (d), and defect thermodynamics for (e); correctly identifies when ideal gas approximations apply and when they fail | Shows basic familiarity with concepts but confuses collision frequency with collision rate per molecule, or misidentifies phase regions in (c); partial understanding of defect types | Fundamental misconceptions such as using rms speed instead of mean speed for flux, or treating supercritical fluid as two-phase in (c)(iii) |
| Mechanism / equation | 20% | 10 | States and correctly applies: kinetic theory flux equation for (a); surface work and area-volume relations for (b); Clausius-Clapeyron reasoning and lever rule for (c); first law energy balance for (d); Arrhenius defect formation for (e); all equations dimensionally consistent | Uses correct final equations but omits derivations or states them incompletely; minor errors in geometric relations for droplet surface area | Missing key equations, uses wrong formulas (e.g., ideal gas law for collision frequency), or applies thermodynamic relations to inappropriate conditions |
| Numerical accuracy | 25% | 12.5 | All calculations with correct unit conversions (atm→Pa, cm²→m², °C→K, torr→atm), proper significant figures, and physically reasonable magnitudes; final answers: (a) ~2.7×10²³ collisions/s, (b)(i) r~1.9 nm, (b)(ii) ~3×10⁴ molecules, (d) ~16.8 g condensed | Correct method but arithmetic errors or unit conversion mistakes (e.g., forgetting 10⁻⁶ in pressure, or cm³ vs m³ confusion); order of magnitude correct | Gross numerical errors, wrong powers of ten, or physically impossible results accepted without comment; missing essential data substitutions |
| Diagram / structure | 15% | 7.5 | Clear phase diagram for (c) with labeled axes (P vs T), correctly positioned critical point, triple point, three phase boundaries, and marked process paths for (ii) and (iii); compression paths clearly distinguished as crossing vs not crossing vapor-liquid coexistence curve | Rough sketch with correct general shape but misplaced critical point or incorrect slope of solid-liquid line; missing process path labels | No diagram, or diagram with serious errors (e.g., triple point above critical point, missing phase labels, or confused axes) |
| Application context | 20% | 10 | Interprets results physically: collision frequency relevance to vacuum technology and surface catalysis; droplet size significance for cloud seeding and nanotechnology; phase diagram application to LPG storage safety in Indian households; humidity calculation to condensation harvesting; defect concentration to semiconductor processing | Brief mention of applications without elaboration; generic statements about 'industrial importance' without specific examples | Purely mathematical treatment with no physical interpretation; or irrelevant applications that misrepresent the phenomena |
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