19-9 The Adiabatic Expansion of an Ideal Gas

19-9 The Adiabatic Expansion of an Ideal Gas#

Prompts

  • In an adiabatic process, \(Q = 0\). What happens to the temperature when an ideal gas expands adiabatically? Why?

  • Write \(pV^\gamma = \text{constant}\) for an adiabatic process. What is \(\gamma\)? What is \(\gamma\) for a monatomic gas?

  • Derive or state the relation \(TV^{\gamma-1} = \text{constant}\). How does \(T\) change when \(V\) increases adiabatically?

  • Why does the relation \(pV^\gamma = \text{constant}\) NOT apply to a free expansion? What happens to \(T\) in a free expansion?

Lecture Notes#

Overview#

  • An adiabatic process has \(Q = 0\)—no heat exchange with the surroundings.

  • Achieved by rapid expansion/compression or a well-insulated container.

  • \(pV^\gamma = \text{constant}\) and \(TV^{\gamma-1} = \text{constant}\), where \(\gamma = C_P/C_V\).

  • Adiabatic expansion → gas does work → internal energy decreases → temperature drops.


Adiabatic relations#

Pressure–volume: $\( p_i V_i^\gamma = p_f V_f^\gamma \quad \text{(adiabatic)} \)$ (eq-adiabatic-pV)

Temperature–volume: $\( T_i V_i^{\gamma-1} = T_f V_f^{\gamma-1} \quad \text{(adiabatic)} \)$ (eq-adiabatic-TV)

\(\gamma = C_P/C_V\) (ratio of molar specific heats):

  • Monatomic: \(\gamma = 5/3 \approx 1.67\)

  • Diatomic: \(\gamma = 7/5 = 1.4\)


Physical picture#

  • Expansion (\(V_f > V_i\)): Gas does work on surroundings; \(W > 0\). With \(Q = 0\), first law gives \(\Delta E_{\text{int}} = -W < 0\) → internal energy decreases → temperature drops.

  • Compression (\(V_f < V_i\)): Work done on gas; \(W < 0\)\(\Delta E_{\text{int}} > 0\)temperature rises.

On a \(p\)\(V\) diagram, an adiabat is steeper than an isotherm: \(p \propto 1/V^\gamma\) vs \(p \propto 1/V\).


Free expansion (exception)#

In a free expansion (gas expands into a vacuum), \(Q = 0\) and \(W = 0\) (no external pressure to work against). So \(\Delta E_{\text{int}} = 0\)\(T\) stays constant.

  • \(p_i V_i = p_f V_f\) (ideal gas law; \(T\) and \(n\) unchanged).

  • \(pV^\gamma = \text{constant}\) does not apply—free expansion is not a quasi-static process.


Summary#

  • Adiabatic: \(Q = 0\); \(pV^\gamma = \text{constant}\); \(TV^{\gamma-1} = \text{constant}\).

  • \(\gamma = C_P/C_V\); monatomic \(\gamma = 5/3\), diatomic \(\gamma = 7/5\).

  • Expansion → cooling; compression → heating.

  • Free expansion: \(Q = W = 0\)\(T\) constant; \(pV^\gamma\) does not apply.