Thermodynamics
Exercise L.V.3 — Thermodynamics & Heat
Clear, step-by-step solutions in HTML format
Q1 — Linear expansion
Formula: ΔL = L · α · ΔT
Given: L = 100 mm, α = 4.5 × 10-6/°C, ΔT = 200 °C
Calculation:
ΔL = 100 × (4.5 × 10-6) × 200 = 0.09 mm
Increase in length = 0.09 mm
Q2 — Energy removed cooling steam to liquid
Given: m = 10 g = 0.01 kg
Lv = 2.26 × 106 J/kg, Cwater = 4.26 × 103 J/(kg·°C), Csteam = 2.0 × 103 J/(kg·°C)
- Cool steam from 113 °C to 100 °C:
Q1 = m·Csteam·(113−100) = 0.01·2000·13 = 260 J - Condense steam at 100 °C to liquid at 100 °C:
Q2 = m·Lv = 0.01·2.26×106 = 22,600 J - Cool liquid water from 100 °C to 53 °C:
Q3 = m·Cwater·(100−53) = 0.01·4260·47 = 2,009 J
Total: Q = Q1 + Q2 + Q3 = 260 + 22600 + 2009 = 24,869 J ≈ 24.9 kJ
Q3 — Mass of steam condensed
Given: mw = 200 g = 0.2 kg, Cw = 4200 J/(kg·°C), Lv = 2.26×106 J/kg
Heat gained by water: Qw = mw·Cw·(100−5) = 0.2·4200·95 = 79,800 J
Heat released by condensed steam: Qs = ms·Lv
Equate: ms·2.26×106 = 79,800 → ms = 79,800 / 2.26×106 = 0.0353 kg = 35.3 g
Q4 — Ideal gas law (final temperature)
Use P1V1/T1 = P2V2/T2
T2 = (P2 V2 T1)/(P1 V1) = (3.5·10·310)/(2·15) = 361.7 K
Final temperature ≈ 362 K
Q5 — First law of thermodynamics (two parts)
a)
Given: Work done on gas W = 135 J (on the gas → +135 J), internal energy increase ΔU = +445 J.
First law (sign convention used here): ΔU = Q + W. So Q = ΔU − W = 445 − 135 = 310 J.
b)
Given: Initial internal energy Ui = 27 J, heat added Q = 383 J, system does work W = 67 J.
ΔU = Q − W = 383 − 67 = 316 J → Uf = Ui + ΔU = 27 + 316 = 343 J.
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