By convention, place the nuclei along the z axis.
So we can define the relative positions of the two sets of p orbitals from each atom and identify which give σ bonding and which give π bonding.
The 2s and 2pz atomic orbitals on O are used to construct σ-bonding MOs.
pz.
px and py.
They combine to form a 2pz σ-bonding MO and a 2pz* σ-antibonding MO.
By end-on overlap along the internuclear axis.
By sideways overlap of p orbitals perpendicular to the internuclear axis.
Same-phase lobes pointing toward each other combine to make the σ-bonding MO.
Opposite-phase lobes face each other and give a σ-antibonding MO.
The opposite-phase lobes pointing toward each other are smaller.
The opposite-phase lobes pointing away from the nucleus–nucleus bond are larger.
One nodal plane.
A planar node containing the internuclear axis.
They form π-bonding and π* antibonding molecular orbitals by sideways overlap in the x-z plane.
They form π-bonding and π* antibonding molecular orbitals in the analogous way, perpendicular to the px set.
Electron density is above and below, or on either side of, the internuclear axis, with bonding overlap between the nuclei.
Electron density is mainly outside the nucleus–nucleus bonding region.
Another planar node between the nuclei, in addition to the nodal plane containing the internuclear axis.
The 2s bonding and antibonding MOs are both full, so there is no net 2s σ bonding, and the 2p-derived MOs determine the bonding.
O=O.
One σ bond and one net π bond, so overall bond order 2.
Because the π bonding set is filled, but the π* antibonding set contains two electrons, reducing the net π bond order to 1.
Because it has 2 unpaired electrons in the π* orbitals.
In the degenerate π*(2px) and π*(2py) orbitals.
Triplet O2.
Because it has two unpaired electrons with parallel spins, giving S = 1 and multiplicity 2S + 1 = 3.
2S + 1.
The total spin quantum number, obtained from the sum of the electron spins.
S = 1.
2(1) + 1 = 3.
An excited form of O2 in which the electron spins are paired overall to give S = 0.
2(0) + 1 = 1.
Because of spin exchange stabilization energy.
Triplet O2 is lower in energy and spin-restricted, so it is not as reactive as singlet O2.
Using light and a photocatalyst.
Photodynamic cancer therapy.
A photocatalyst is added near a tumour, light is applied, and triplet O2 in blood is converted locally into singlet O2 in the tumour region.
Because it is more reactive and forms locally in the tumour.
Because traces of singlet O2 react with molecules in the body and give off faint amounts of light.
Rotation of the orbital about the internuclear axis generates no phase change.
If you rotate it around the internuclear axis, the phase does not change.
There is a nodal plane between the nuclei, and the plane is orthogonal to the internuclear axis.
A nodal plane between the nuclei perpendicular to the atom–atom axis.
Rotation around the internuclear axis gives phase change.
If you rotate it 180° around the internuclear axis, the phase changes.
Rotation around the internuclear axis gives phase change and there is a nodal plane between the nuclei.
It has phase change on rotation around the internuclear axis and a nodal plane between the nuclei.
The relative energy levels of the 2pz σ MO and the 2px, 2py π MOs change and depend on the s-p gap.
The relative ordering of σ(2p) and π(2p) changes as Zeff increases.
The σ 2p MO drops below the energy of the π 2p bonding MOs as Zeff increases.
B2, C2, and N2.
O2 and F2.
Bond order 3.
:N≡N:
Because MO theory indicates a bond order of 3, consistent with a very strong triple bond.
Much of nature is N-starved because N2 is so stable and hard to react.
Lightning and a few nitrogenase enzymes.
Early life on the planet was based on enzymes and systems that reacted with N2 when very little O2 was present.
Cyanobacteria produced O2 from water and sunlight.
H2O + sunlight → O2 + “H2”
O2 is more reactive than N2, and increasing O2 in the early atmosphere destroyed many N2-consuming life forms and converted much Fe(s) into Fe2O3.
Through σ donation from a lone pair on N to an empty σ orbital on Fe and π-back donation from filled Fe dπ orbitals into empty 2p π* orbitals on N2.
An empty σ orbital on Fe, described as some lowest-energy combination such as s, pz, or dz2.
From a lone pair on N.
Into the empty 2p π* orbital on N2.
Filled dxy on Fe.
Synergistic bonding.
Because both σ donation and π-back donation occur simultaneously and reinforce the interaction.
They are constructed in the same manner as homonuclear diatomics.
HF.
It is used to clean or etch Si wafers in making logic chips.
Because the Si–F bond is very strong.
P–F.
HF can go through skin and etch bone underneath.
Because the electronegativity, or Zeff, for F is higher than for H.
The H 1s valence AO is too high in energy relative to F 2s to interact significantly.
F 2pz, when the z axis is taken along the H–F bond.
Because the z axis is along the bond between the atoms, so pz points directly along the H–F bond.
Because px is oriented incorrectly for strong overlap along the bond axis.
Because both orbitals point along the bond axis and can overlap end-on.
H 1s and F 2pz.
H 1s and F 2pz in the out-of-phase combination.
A planar node inherited from the p orbital character.
Planar nodes, including the antibonding node between the atoms.
Because detailed MO construction requires computational methods such as density functional theory.
Because it is simpler for routine bonding descriptions, while MO theory is more detailed.
Largely covalent.
It is a weak source of H+(aq), so Ka is small.
HF(aq) ⇌ H+(aq) + F−(aq)
H3O+(aq).
pz gives σ bonding; px and py give π bonding.
Two unpaired electrons remain in the π* orbitals.
Triplet O2 has two parallel unpaired electrons and is ordinary O2; singlet O2 is a higher-energy reactive form with paired spin overall.
As Zeff increases across the row, σ(2p) drops below π(2p).
N2 donates a lone pair to Fe by σ donation, and Fe back-donates from filled d orbitals into N2 π*; together this is synergistic bonding.
σ = no phase change on rotation, σ* = σ with a node between nuclei, π = phase change on rotation, π* = π plus a node between nuclei.
