◈ Thermodynamics
Ideal gases, thermodynamic transformations, 1st and 2nd law, heat engines, Carnot and Otto cycles, entropy. Every topic with step-by-step theory, interactive diagrams and solved exercises.
Complete Theory
Worked Examples
Example 1Free adiabatic expansion — Entropy increases even without heat
Example 2Spontaneous heat flow — Why heat goes from hot to cold
Exercises with Solutions
Exercise 1Irreversible heating — A copper block in contact with a hot sourceHard
📋 Problem to solve
A copper block of mass kg at is placed in contact with a source at . Compute of the block, the source, and the universe. ( J/(kg·K))
📌 Given data
m=2 kgT_1=293 KT_H=473 Kc_Cu=385 J/(kg·K)
Exercise 2Irreversible cycle — Entropy production in a real engineVery Hard
📋 Problem to solve
A heat engine operates between K and K. It absorbs J and rejects J to the cold reservoir. Compute , and . Why is even though the engine is cyclic?
📌 Given data
T_H=500 KT_C=200 KQ_H=3000 JQ_C=1800 J
Recommended Books
As an Amazon Associate I earn from qualifying purchases.
🔥
Integrative Problems
Problems combining all chapters — exam levelProblem 1The Thermoelectric Power Plant: from Gas to Molecules to EntropyEXTREME
A thermoelectric power plant uses of a diatomic gas (, ) running through the following cycle on a PV diagram:
State A: , . A→B: adiabatic compression to (compression ratio ). B→C: isochoric, heating to (combustion). C→D: adiabatic expansion to (return to original volume). D→A: isochoric, cooling (Otto cycle).
State A: , . A→B: adiabatic compression to (compression ratio ). B→C: isochoric, heating to (combustion). C→D: adiabatic expansion to (return to original volume). D→A: isochoric, cooling (Otto cycle).
📌 Problem data
(a)Ideal Gas — Thermodynamic States(b)First Law — Work and Heat for Each Process(c)Cycles — Otto vs Carnot Efficiency(d)Kinetic Theory — Molecules in Motion(e)Entropy — Second Law and Global Balance
