Physics › Heat and Thermodynamics › Thermodynamics · Part 4/10
1. Zeroth Law 2. First Law 3. P–V Diagrams & Cycles 4. Cv, Cp and γ 5. Iso-processes 6. Adiabatic 7. Free Expansion 8. Polytropic 9. Engines & Fridges 10. Second Law & Carnot
Thermodynamics · Part 4 of 10
Molar Specific Heats: Cv, Cp and γ
A gas's specific heat depends on how it is heated. This part derives the two standard ones from the first law, C v = 2 f R at constant volume and C p = C v + R at constant pressure (Mayer's relation), then their ratio γ for one gas and for a mixture.
Builds on: Part 2 · First Law of Thermodynamics .
Video coming soon
Constant volume
C v = 2 f R With the volume fixed, d W = 0 , so d Q = d U : n C v d T = 2 f n R d T , giving C v = 2 f R (2 3 R monatomic, 2 5 R diatomic).
Locked lid: all the heat raises U.
Free piston: some heat goes into work.
Constant pressure
Mayer: C p = C v + R At constant pressure the gas also does work P d V = n R d T . So n C p d T = n C v d T + n R d T and C p = C v + R = 2 f + 2 R : always bigger than C v .
Ratio of heat capacities
γ = C v C p = f f + 2 Monatomic 5/3 ≈ 1.67, diatomic 7/5 = 1.4, non-linear polyatomic (f = 6) 4/3. More degrees of freedom, smaller γ; always γ > 1.
Cv, Cp and γ for common gases.
Average Cv, not γ.
Mixtures
∑ γ i − 1 n i = γ mi x − 1 ∑ n i Internal energies add at the common temperature, so C v values average by moles. With C v = R / ( γ − 1 ) this gives the rule above. Never average γ directly.
Summary
Key formulas
C v = 2 f R Molar Heat Capacity at Constant Volume (Cv )
C p = C v + R = 2 f + 2 R Molar Heat Capacity at Constant Pressure (Cp )
γ = C v C p = f f + 2 Ratio of Heat Capacities of a Gas
γ 1 − 1 n 1 + γ 2 − 1 n 2 = γ e q − 1 n 1 + n 2 Ratio of Specific Heats for a Mixture of Gases
Worked examples
One for every idea
Molar Heat Capacity at Constant Volume (Cv )
1. Find the heat required to raise the temperature of 1 mol of a diatomic gas by 10 K at constant volume (C v = 2 5 R ).
Diatomic: f = 5 , C v = 2 5 R = 20.785 J/mol·K. Q = n C v Δ T = 1 × 20.785 × 10 .Q ≈ 207.9 J.
Molar Heat Capacity at Constant Pressure (Cp )
2. A monatomic gas has C v = 2 3 R . Using Mayer's relation, find C p .
C p = C v + R = 2 3 R + R .C p = 2 5 R ≈ 20.79 J/mol·K.
Ratio of Heat Capacities of a Gas
3. Find γ for a diatomic gas at ordinary temperature.
Vibration is frozen: 3 translational + 2 rotational, f = 5 . γ = f f + 2 = 5 7 .γ = 1.4 .
Ratio of Specific Heats for a Mixture of Gases
4. A mixture contains 2 mol of a monatomic gas (γ 1 = 3 5 ) and 3 mol of a diatomic gas (γ 2 = 5 7 ). Find the equivalent γ of the mixture.
2/3 2 + 2/5 3 = 3 + 7.5 = 10.5 .γ mi x − 1 5 = 10.5 ⇒ γ mi x − 1 = 0.476 .A plain mole-weighted average of γ (1.51) is wrong. γ mi x ≈ 1.48 .
JEE-style question
Your turn
For an ideal gas, Cp /Cv = 1.4. Its molar heat capacity at constant volume Cv is:
(a) 1.5R
(b) 2.5R
(c) 3.5R
(d) 1.4R
Show the answer and the traps
Cv = R/(γ − 1) = R/0.4 = 2.5R: option b.
1.5R is the monatomic value. 3.5R is Cp, not Cv .
And 1.4R confuses γ, a ratio, with Cv /R.
Watch out
Common mistakes
Using Cv in a constant-pressure problem (or the reverse) Constant volume: C v . Constant pressure: C p = C v + R .
Averaging γ by moles for a mixture Average C v (equivalently add n / ( γ − 1 ) ), then find γ.
Using f = 7 for a diatomic gas at room temperature Vibration is frozen at ordinary temperatures: f = 5, γ = 1.4.
Practice
Try these
1. Find C p and γ for a gas with C v = 3 R . C p = 4 R , γ = 4/3 .
2. For a gas, C p = 29.1 J/mol·K. Find C v . C v = C p − R ≈ 20.8 J/mol·K (a diatomic gas).
3. A gas has γ = 1.4. Find its degrees of freedom. f f + 2 = 1.4 ⇒ f = 5 .
4. 1 mol of He (γ = 5/3) is mixed with 1 mol of O₂ (γ = 7/5). Find γ of the mixture. 2/3 1 + 2/5 1 = 4 = γ − 1 2 ⇒ γ = 1.5 .