The Molecular Orbital (MO) Theory, proposed by Hund and Mullikan in 1932, describes chemical bonding through the combination of atomic orbitals to form molecular orbitals that are characteristic of the entire molecule. When atomic orbitals combine, they lose their individual identities. This process, known as the Linear Combination of Atomic Orbitals (LCAO), results in the formation of new molecular orbitals with different energy levels.
Bonding Molecular Orbital (BMO): A lower-energy, stable orbital formed from the constructive interference of atomic orbitals.
Antibonding Molecular Orbital (ABMO): A higher-energy, unstable orbital formed from the destructive interference of atomic orbitals.
Figure 3.27: Energy diagram of bonding and antibonding molecular orbitals
MO theory can effectively explain the magnetic properties of molecules:
Paramagnetic: Molecules with one or more unpaired electrons in their molecular orbitals. They are attracted by a magnetic field.
Diamagnetic: Molecules with no unpaired electrons. They are repelled by a magnetic field.
Occurs with the combination of s-s, s-p, and px−px orbitals.
Forms sigma (σ) molecular orbitals. For example, two s atomic orbitals combine to form one low-energy σs (BMO) and one high-energy σs∗ (ABMO).
Sideways Approach (Parallel Overlapping):
Occurs between py−py and pz−pz orbitals.
Forms pi (π) molecular orbitals. For example, two py atomic orbitals combine to form one low-energy πpy (BMO) and one high-energy πpy∗ (ABMO).
When the three 2p atomic orbitals (px,py,pz) of one atom overlap with those of another, six molecular orbitals are formed (three bonding and three anti-bonding).
Bond order is defined as half the difference between the number of electrons in bonding molecular orbitals and the number of electrons in antibonding molecular orbitals. It represents the number of chemical bonds between two atoms.
Bond order=2(No. of electrons in BMOs)−(No. of electrons in ABMOs)
If the bond order is zero, the molecule is unstable and does not exist.
A positive bond order indicates that the molecule is stable and can exist.
Example: Hydrogen Molecule (H2)
Number of electrons in Bonding MOs = 2
Number of electrons in Antibonding MOs = 0
Calculation:
Bond order=22−0=1
This indicates a single bond between the two hydrogen atoms.
The relative energies of molecular orbitals, determined by spectroscopy, differ for lighter and heavier diatomic molecules of the second period.
a) For Heavier Molecules (O2,F2, and their ions):
The increasing order of energy is:
σ1s<σ1s∗<σ2s<σ2s∗<σ2px<(π2py=π2pz)<(π2py∗=π2pz∗)<σ2px∗
b) For Lighter Molecules (B2,C2,N2):
These molecules show a slightly different order due to s-p mixing, where the energy difference between the 2s and 2p atomic orbitals is small. This mixing raises the energy of the σ2px orbital above the π2p orbitals.
σ1s<σ1s∗<σ2s<σ2s∗<(π2py=π2pz)<σ2px<(π2py∗=π2pz∗)<σ2px∗
A key success of MO theory is its ability to explain why oxygen is paramagnetic. The MO diagram for O2 shows two unpaired electrons, one in the π2py∗ orbital and another in the π2pz∗ orbital. These unpaired electrons give O2 its magnetic properties. This observation is not explained by the Valence Bond Theory.
Properties: The bond order of 2 indicates a stable double bond (O=O), with a high bond energy (498kJmol−1) and a bond length of 1.21A˚.
MO Configuration:(σ1s)2(σ1s∗)2(σ2s)2(σ2s∗)2(σ2px)2(π2py)2(π2pz)2(π2py∗)2(π2pz∗)2
Bond Order:210−8=1
Magnetic Character: Diamagnetic.
Properties: The bond order of 1 indicates a single bond (F−F). The bond energy is relatively low (159kJmol−1) and the bond distance is longer (1.43A˚) compared to N2 and O2.