Molecular Orbital (MO) theory provides a more in-depth analysis of how electrons operate in molecules by considering the wave nature of electrons. Instead of localized electron pairs, as seen in Lewis theory, MO theory describes electrons in terms of molecular orbitals that span the entire molecule. When applying MO theory to \(\mathrm{C}_2\), its 8 valence electrons fill available molecular orbitals according to their energy levels. These include bonding and antibonding orbitals such as \(\sigma_{1s}, \sigma_{1s}^*, \sigma_{2s}, \sigma_{2s}^*, \pi_{2p}\), among others. In \(\mathrm{C}_2\), after populating these molecular orbitals, the remaining electrons in the \(\pi_{2p}\) bonding orbitals account for a bond order of 2 because:
- The bond order equation is given by \[\frac{1}{2} (N_b - N_a)\], where \(N_b\) is the number of bonding electrons and \(N_a\) is the number of antibonding electrons.
- For \(\mathrm{C}_2\), \(N_b = 4\) and \(N_a = 0\), resulting in a bond order of 2 \[\frac{1}{2} (4-0) = 2\].
This indicates a double bond, which reflects the delocalization of electrons not accounted for in simple Lewis structures.