Isothermal and Adiabatic changes
S.No Isothermal Change Adiabatic Change
1. Temperature remains constant, i.e Δ = 0 No exchange of heat ΔQ = 0
2. System is thermally conducting to the surroundings System is thermally insulated from the surroundings
3. The process takes place slowly The process takes place quickly
4. Internal energy remains constant ΔU = 0 Internal energy changes ΔU ≠ 0
5. Specific heat capacity is infinite Specific heat capacity is zero
6. Equation of state is PV = constant Equation of state is PVγ = constant
7.
8. Isothermal elasticity Eθ = P Adiabatic elasticity Eϖ = γP
9.

Comparison between isothermal and adiabatic curves:

When expanded to the same volume from the same initial state.

Work done: W1 > W2

Final pressure: P1 > P2

Final temperature: T1 > T2

When compressed to the same volume from the same initial state

Work done: W1 < W2

Final pressure: P1 > P2

Final temperature: T1 > T2

When expanded to the same pressure from the same initial state.

Work done: W1 > W2

Final volume: V1 > V2

Final temperature: T1 > T2

When compressed to the same pressure from the same initial state.

Work done: W1 < W2

Final volume: V1 < V2

Final temperature: T1 < T2