Many chemical processes involve the transfer of electrons between atoms, ions, or molecules. The energy required to remove electrons and the energy released when electrons are added are therefore important thermodynamic quantities.
The ionization potential (or ionization energy) is defined as the enthalpy change for removing an electron from a gaseous species at \(0\ \mathrm{K}\):
\[ M(g) \rightarrow M^+(g) + e^- \]
\[ \Delta H \equiv IP_1 \]
Removing additional electrons gives the second, third, and higher ionization potentials:
\[ M^+(g) \rightarrow M^{2+}(g) + e^- \qquad IP_2 \]
Ionization potentials are always positive because energy must be supplied to remove an electron from a species.
The electron affinity is the enthalpy change associated with adding an electron to a gaseous species:
\[ X(g) + e^- \rightarrow X^-(g) \]
Electron affinities are commonly tabulated as positive quantities even though the process itself is often exothermic. Consequently,
\[ \Delta H = -EA \]
for the electron-capture process.
Ionization potentials and electron affinities allow thermodynamic cycles to be constructed for reactions involving ions. By combining these quantities with reaction enthalpies and Hess' Law, the energetics of electron-transfer processes can be determined even when the reaction itself is difficult to measure directly.
They are particularly important in Born-Haber cycles, electrochemistry, and the thermodynamics of ionic compounds.
Calculate the enthalpy change for the gas-phase electron-transfer reaction:
\[ Cu^{2+}(g) + 2K(g) \rightarrow Cu(g) + 2K^+(g) \]
Use the following ionization potentials:
| Process | Enthalpy |
|---|---|
| \(K(g) \rightarrow K^+(g)+e^-\) | \(IP_1(K)=418.8\ \mathrm{kJ\,mol^{-1}}\) |
| \(Cu(g) \rightarrow Cu^+(g)+e^-\) | \(IP_1(Cu)=745.5\ \mathrm{kJ\,mol^{-1}}\) |
| \(Cu^+(g) \rightarrow Cu^{2+}(g)+e^-\) | \(IP_2(Cu)=1957.9\ \mathrm{kJ\,mol^{-1}}\) |
Potassium is oxidized, so use the ionization process as written:
\[ 2K(g) \rightarrow 2K^+(g) + 2e^- \]
\[ \Delta H = 2 \left( 418.8\ \mathrm{kJ\,mol^{-1}} \right) \]
\[ \Delta H = 837.6\ \mathrm{kJ\,mol^{-1}} \]
Copper(II) is reduced to copper metal, so reverse the first and second ionization processes:
\[ Cu^{2+}(g) + 2e^- \rightarrow Cu(g) \]
\[ \Delta H = - \left( 745.5\ \mathrm{kJ\,mol^{-1}} + 1957.9\ \mathrm{kJ\,mol^{-1}} \right) \]
\[ \Delta H = -2703.4\ \mathrm{kJ\,mol^{-1}} \]
Adding the two processes gives the target reaction:
\[ Cu^{2+}(g) + 2K(g) \rightarrow Cu(g) + 2K^+(g) \]
\[ \Delta H_{\mathrm{rxn}} = 837.6\ \mathrm{kJ\,mol^{-1}} - 2703.4\ \mathrm{kJ\,mol^{-1}} \]
\[ \Delta H_{\mathrm{rxn}} = -1865.8\ \mathrm{kJ\,mol^{-1}} \]
Therefore,
\[ \boxed{ \Delta H_{\mathrm{rxn}} = -1.87\times10^3\ \mathrm{kJ\,mol^{-1}} } \]
Physical interpretation: Energy must be supplied to remove electrons from potassium atoms, but a much larger amount of energy is released when \(Cu^{2+}\) gains those electrons and becomes neutral copper. The energy released by reducing copper exceeds the energy required to ionize potassium, making the overall reaction strongly exothermic.
Big picture: Ionization potentials measure the energy required to remove electrons, while electron affinities describe the energetics of adding electrons. Together they allow electron-transfer reactions to be analyzed using Hess' Law and provide the foundation for understanding ionic bonding, lattice energies, and Born-Haber cycles.