Principles of Linear Combination of Atomic Orbitals (LCAO)
The wave functions for molecular orbitals can be obtained by solving the Schrödinger wave equation for the molecule. However, solving the Schrödinger wave equation directly for complex molecules is mathematically difficult. Therefore, the Linear Combination of Atomic Orbitals (LCAO) approximation method is used to obtain the wave functions for molecular orbitals.
Atomic orbitals are represented by wave functions ψ. Let us consider two atomic orbitals represented by the wave functions ψA and ψB of atoms A and B respectively, possessing comparable energy. When they combine, they form two molecular orbitals: a bonding molecular orbital (ψbonding) and an anti-bonding molecular orbital (ψanti-bonding).
The formation of a bonding molecular orbital is the result of addition (i.e., constructive interference) of the two atomic orbitals. Conversely, the formation of an anti-bonding molecular orbital is the result of subtraction (i.e., destructive interference) of the two atomic orbitals.
ψBMO = ψA + ψB
ψABMO = ψA − ψB
Explanation: In a homonuclear or heteronuclear bimolecular system, an electron near one nucleus belongs predominantly to the wave function of that specific nucleus at any particular moment. But when the electron is distributed between two nuclei, it is governed by their combined wave function. This configuration is the core basis of the LCAO principle.
If ψA and ψB represent the baseline atomic wave functions of the interacting atoms, the structural outcome behaves as follows:
Hence, according to the LCAO principle, we mathematically define the state transformations as:
ψBMO = ψ(1)A + ψ(1)B
ψABMO = ψ(1)A − ψ(1)B