Reaction Energetics — Internal Energy and Enthalpy

Theoretical Background

  • First Law of Thermodynamics:
    \(\Delta U = q + w\)

  • Enthalpy definition:
    \(H = U + pV \;\Rightarrow\; \Delta H = \Delta U + \Delta(pV)\)

  • At constant pressure, when the only mechanical work is pressure–volume work: $ \Delta H=q_p. $

  • For an ideal-gas reaction at a fixed temperature: $ \Delta_r H^\circ =\Delta_r U^\circ+\Delta\nu_{\text{gas}}RT, \qquad \Delta_r U^\circ =\Delta_r H^\circ-\Delta\nu_{\text{gas}}RT, $ where $\Delta\nu_{\text{gas}}$ is the sum of the gaseous stoichiometric coefficients of the products minus that of the reactants.

Validity note.
The relation containing $\Delta\nu_{\text{gas}}RT$ follows from the ideal-gas equation for the gaseous species. It is exact for the all-gas ideal reaction considered below. Real gases require an appropriate equation of state.

Sign convention used here.
$w>0$ denotes work done on the system, while $w<0$ denotes work done by the system. With this convention, the First Law is $\Delta U=q+w$.

Exercise

Consider the combustion of carbon monoxide:

\[2\,\mathrm{CO}(g) + \mathrm{O}_2(g) \;\longrightarrow\; 2\,\mathrm{CO}_2(g)\]

At $T = 298\,\text{K}$ and $p = 1\,\text{bar}$, the standard enthalpy of reaction is:

\[\Delta_r H^{\circ} = -566.0\,\text{kJ mol}^{-1}\]

Tasks:

  1. Calculate the standard molar internal-energy change $\Delta_r U^{\circ}$.
  2. Explain the relation between $\Delta U$ and $\Delta H$ for reactions involving gases.

Step-by-Step Solution

Step 1. Count moles of gas

  • Reactants: $n_{\text{gas}} = 2 + 1 = 3$
  • Products: $n_{\text{gas}} = 2$

So: \(\Delta\nu_{\text{gas}} = \sum\nu_{\text{products}}-\sum\nu_{\text{reactants}} =2-(2+1)=-1\)


Step 2. Relation between $\Delta H$ and $\Delta U$
For ideal gases: \(\Delta_r U^\circ =\Delta_r H^\circ-\Delta\nu_{\text{gas}}RT\)


Step 3. Insert data
With $T = 298\,\text{K}$ and $R = 8.314\,\text{J mol}^{-1}\text{K}^{-1}$: \(\Delta\nu_{\text{gas}}RT =(-1)(8.314)(298) =-2.48 \times 10^{3}\,\text{J mol}^{-1} =-2.48\,\text{kJ mol}^{-1}\)


Step 4. Final value
\(\Delta_r U^{\circ} =(-566.0)\,\text{kJ mol}^{-1} -(-2.48)\,\text{kJ mol}^{-1} =-563.5\,\text{kJ mol}^{-1}.\)


Answer:
\(\Delta_r U^{\circ} = -563.5\,\text{kJ mol}^{-1}\)

Notes

  • The difference between $\Delta_r U^\circ$ and $\Delta_r H^\circ$ is small here because $\Delta\nu_{\text{gas}}=-1$.
  • If $\Delta\nu_{\text{gas}}=0$ for an ideal-gas reaction, then $\Delta_r H^\circ=\Delta_r U^\circ$.
  • The magnitude of the correction $\Delta\nu_{\text{gas}}RT$ grows with temperature and with the change in gaseous stoichiometric coefficients.
  • Standard reaction enthalpies are commonly tabulated, while the First Law is written directly in terms of internal energy.
  • For non-ideal gases, the simple $RT\Delta\nu_{\text{gas}}$ correction is only approximate.