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First & Second Laws of Thermodynamics and Their Applications

Systems and properties, state and path functions, the zeroth and first laws, internal energy and enthalpy, specific heats, ideal-gas processes (isothermal, adiabatic, isobaric, isochoric), the second law (Kelvin–Planck and Clausius statements), heat engines, refrigerators and heat pumps, the Carnot cycle, entropy and the third law — with worked examples.

📑 Contents (5 sections)

Last reviewed 4 Nov 2026 · 4 min read

1. Basic terms

Term Meaning
System types Open (mass and energy cross), closed (only energy crosses), isolated (neither)
Intensive / extensive properties Independent of size (T, P, density) / depend on size (V, U, H, mass)
State function Depends only on the state — U, H, S, G, T, P
Path function Depends on the path — heat Q and work W
Zeroth law If A and B are each in thermal equilibrium with C, they are in equilibrium with each other — basis of temperature measurement

2. First law — conservation of energy

FormulaFirst law (closed system)

Q = heat added to the system; W = work done by the system (sign convention used in engineering). For a cycle, .

  • Enthalpy ; at constant pressure, ; at constant volume, .
  • For an ideal gas: ; (≈ 1.4 for air, 1.67 for monatomic gases).
  • A perpetual motion machine of the first kind (work without energy input) is impossible.

Ideal-gas processes

Process Condition Work done by gas Heat
Isochoric V constant 0
Isobaric P constant
Isothermal T constant ( = const) (ΔU = 0)
Adiabatic (reversible) , = const 0
Polytropic = const —
Worked Example1 — Adiabatic compression of air

Air (γ = 1.4) at 300 K and 1 bar is compressed reversibly and adiabatically to 8 bar. 543 K.

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