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Molecular Orbital Theory

  • In MO theory, valence electrons are delocalized over the entire molecule, not confined to individual atoms or bonds

  • Molecular orbitals arise from adding together (superimposing) atomic orbitals

  • A linear combination of atomic orbitals (LCAO) creates molecular orbitals (bonding and antibonding orbitals)

    • An electron in a bonding MO will be attracted to both nuclei, and will be lower in energy (more stable) compared to an atomic orbital for a single nuclei

    • An electron in an antibonding MO will be excluded from the internuclear region, and thus have a higher energy than if in an atomic orbital

  • N molecular orbitals can be created from N atomic orbitals

    • 2 atomic orbitals generate 2 MOs (one is bonding (lower in energy) and one is antibonding (higher in energy))

  • Bond order = ½ (# of bonding electrons - # of antibonding electrons)

Homonuclear Diatomic Molecules with MOs Originating From s Orbitals

  • 1s + 1s = σ₁ₛ (bonding MO)

    • σ orbital: cylindrically symmetric about the bond axis; no nodal plane along the bond axis

    • 1s - 1s = σ₁ₛ* (antibonding MO)

Homonuclear Diatomic Molecules with MOs Originating From s and p Orbitals

  • Bonding orbitals formed by LCAO of 2pₓ and 2pᵧ

    • 2pₓ + 2pₓ = 𝜋₂ₚₓ

    • 2pᵧ + 2pᵧ = 𝜋₂ₚᵧ

    • 𝜋 orbital (bonding orbital): molecular orbital with a nodal plane along the bond axis

  • Antibonding orbitals formed by LCAO of 2pₓ and 2pᵧ

    • 2pₓ - 2pₓ = 𝜋₂ₚₓ*

    • 2pᵧ - 2pᵧ = 𝜋₂ₚᵧ*

    • 𝜋 orbital (antibonding orbital): MO with 2 nodal planes along the bond axis

  • The stability of the resulting molecule depends on the number of electrons that occupy lower energy orbitals compared to the number that occupy higher energy orbitals

    • If the net molecule formation is that more electrons have a lower energy, then the molecule is stable

    • If the energy differential is small, then the molecule is not as stable

  • Bonding orbitals formed by LCAO of 2pz

    • 2pz +  2pz = σ2pz

    • Nodes pass through the nuclei but no nodes along the bond axis

  • Antibonding orbitals formed by LCAO of 2pz

    • 2pz   -  2pz = σ2pz *

    • Nodes pass through and between the nuclei, but not along the bond axis

  • The relative energies of the σ2pz compared to the  𝜋₂ₚₓ or y orbitals depend on the z value of the atoms

    • The relative energy ordering is 𝜋₂ₚₓ and 𝜋₂ₚy < σ2pz if Z < 8

    • The relative energy ordering is σ2pz < 𝜋₂ₚₓ and 𝜋₂ₚ if Z = or > 8

    • This only applies to the bonding orbitals because the relative energy ordering of the antibonding orbitals is the same regardless of Z (𝜋₂ₚₓ* and 𝜋₂ₚy*< σ2pz*)

TR

Molecular Orbital Theory

  • In MO theory, valence electrons are delocalized over the entire molecule, not confined to individual atoms or bonds

  • Molecular orbitals arise from adding together (superimposing) atomic orbitals

  • A linear combination of atomic orbitals (LCAO) creates molecular orbitals (bonding and antibonding orbitals)

    • An electron in a bonding MO will be attracted to both nuclei, and will be lower in energy (more stable) compared to an atomic orbital for a single nuclei

    • An electron in an antibonding MO will be excluded from the internuclear region, and thus have a higher energy than if in an atomic orbital

  • N molecular orbitals can be created from N atomic orbitals

    • 2 atomic orbitals generate 2 MOs (one is bonding (lower in energy) and one is antibonding (higher in energy))

  • Bond order = ½ (# of bonding electrons - # of antibonding electrons)

Homonuclear Diatomic Molecules with MOs Originating From s Orbitals

  • 1s + 1s = σ₁ₛ (bonding MO)

    • σ orbital: cylindrically symmetric about the bond axis; no nodal plane along the bond axis

    • 1s - 1s = σ₁ₛ* (antibonding MO)

Homonuclear Diatomic Molecules with MOs Originating From s and p Orbitals

  • Bonding orbitals formed by LCAO of 2pₓ and 2pᵧ

    • 2pₓ + 2pₓ = 𝜋₂ₚₓ

    • 2pᵧ + 2pᵧ = 𝜋₂ₚᵧ

    • 𝜋 orbital (bonding orbital): molecular orbital with a nodal plane along the bond axis

  • Antibonding orbitals formed by LCAO of 2pₓ and 2pᵧ

    • 2pₓ - 2pₓ = 𝜋₂ₚₓ*

    • 2pᵧ - 2pᵧ = 𝜋₂ₚᵧ*

    • 𝜋 orbital (antibonding orbital): MO with 2 nodal planes along the bond axis

  • The stability of the resulting molecule depends on the number of electrons that occupy lower energy orbitals compared to the number that occupy higher energy orbitals

    • If the net molecule formation is that more electrons have a lower energy, then the molecule is stable

    • If the energy differential is small, then the molecule is not as stable

  • Bonding orbitals formed by LCAO of 2pz

    • 2pz +  2pz = σ2pz

    • Nodes pass through the nuclei but no nodes along the bond axis

  • Antibonding orbitals formed by LCAO of 2pz

    • 2pz   -  2pz = σ2pz *

    • Nodes pass through and between the nuclei, but not along the bond axis

  • The relative energies of the σ2pz compared to the  𝜋₂ₚₓ or y orbitals depend on the z value of the atoms

    • The relative energy ordering is 𝜋₂ₚₓ and 𝜋₂ₚy < σ2pz if Z < 8

    • The relative energy ordering is σ2pz < 𝜋₂ₚₓ and 𝜋₂ₚ if Z = or > 8

    • This only applies to the bonding orbitals because the relative energy ordering of the antibonding orbitals is the same regardless of Z (𝜋₂ₚₓ* and 𝜋₂ₚy*< σ2pz*)