A bond that belongs to the whole molecule
The core claim is a shift in what a chemical bond is taken to be. Rather than assigning a shared pair of electrons to a specific bond between two named atoms, as the older valence bond picture does, molecular orbital theory treats a molecule’s electrons as moving under the combined influence of every atomic nucleus present, distributed across orbitals that can span the entire structure rather than sitting between just one pair of atoms. Molecular orbitals are typically built from the Linear Combination of Atomic Orbitals method, which combines existing atomic orbitals into new ones, provided those atomic orbitals share compatible symmetry, meaningful spatial overlap, and reasonably similar energy levels.
Built on a decade of new physics
This picture only became possible once quantum mechanics itself had been worked out. Quantum theory developed through the mid-1920s, building on Max Planck’s 1900 treatment of black-body radiation and Einstein’s 1905 explanation of the photoelectric effect, into the fuller framework established by Niels Bohr, Erwin Schrödinger, Werner Heisenberg, Max Born and Paul Dirac. Central to this framework is the Schrödinger equation, whose solutions are wave functions, and the Born rule, which interprets the square of a wave function as a probability density rather than a certainty about where a particle actually is — a foundation molecular orbital theory applies directly to electrons distributed across a molecule.
The test valence bond theory failed
The theory’s clearest advantage over valence bond theory is a specific, checkable prediction rather than a general claim of superiority. Molecular orbital theory correctly explains why ordinary molecular oxygen is paramagnetic, meaning it is weakly attracted into a magnetic field, a property that follows naturally from how electrons fill oxygen’s molecular orbitals but that the valence bond picture, built around paired electrons in fixed bonds, cannot account for. Friedrich Hund, Robert Mulliken and John Lennard-Jones developed the framework mainly through the late 1920s and 1930s, with Lennard-Jones’s 1929 work providing the first quantitative application, and Mulliken introducing the term orbital itself in 1932.
Arithmetic that predicts whether a molecule exists
The theory also comes with working arithmetic that predicts molecular stability directly. Bond order is calculated as half the difference between the number of electrons in bonding orbitals and the number in antibonding orbitals, and this simple figure tracks real chemical behaviour: hydrogen, with a bond order of one, has a bond energy of 436 kilojoules per mole, while the more weakly bound hydrogen cation, with a bond order of one half, holds together with roughly 171 kilojoules per mole. A hypothetical two-atom helium molecule comes out with a bond order of zero, correctly predicting that no such stable molecule exists under ordinary conditions, since its bonding and antibonding electrons cancel out entirely.
From benzene’s equal bonds to graphite’s conductivity
The same delocalised picture extends naturally to more complex molecules. In benzene, six electrons spread evenly around the ring explain why all six carbon-carbon bonds are chemically identical rather than alternating between two different bond types, and in graphite, electrons delocalised across entire sheets of carbon atoms account for the material’s unusually high electrical conductivity. Extended systems of this kind, found in molecules such as beta-carotene and chlorophyll, are also what allow those molecules to absorb specific wavelengths of visible light, connecting the same underlying orbital picture to something as directly observable as a pigment’s colour.
A framework worth the effort it asks for
This is worth the effort selectively rather than universally: the payoff is real, but it asks a reader to give up the intuitive picture of a bond as a simple line between two atoms in exchange for a more accurate, more abstract one. That trade is worth making for anyone who wants an explanation that actually predicts oxygen’s magnetism, distinguishes real molecules from impossible ones through a short calculation, and extends cleanly from simple diatomic gases to the electronic structure of pigments and conductive materials. Readers content with the simpler valence bond picture for everyday purposes will find rather less urgency here, since molecular orbital theory earns its keep specifically in the cases where the simpler picture breaks down.