Download - ψ 1 = c 1 φ 1 + c 2 φ 2 ψ 2 = c 1 φ 1 - c 2 φ 2

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Page 1: ψ 1  = c 1 φ 1  + c 2 φ 2 ψ 2  = c 1 φ 1  - c 2 φ 2

ψ1 = c1φ1 + c2φ2

ψ2 = c1φ1 - c2φ2

Molecular Orbital Theory

LCAO-MO = linear combination of atomic orbitals

Add and subtract amplitudes of atomic orbitals to make molecular orbitals

Just like making hybrid orbitals, but AO’s come from different atoms

Bonding orbitals: Electrons have high probability of being between nuclei (lower energy)

Page 2: ψ 1  = c 1 φ 1  + c 2 φ 2 ψ 2  = c 1 φ 1  - c 2 φ 2

Orbital overlap determines bonding energy

Weak overlap => weak interaction (bonding & antibonding MO energy same as AO’s

Strong overlap => lowers energy of bonding MO, raises energy of antibonding MO

Page 3: ψ 1  = c 1 φ 1  + c 2 φ 2 ψ 2  = c 1 φ 1  - c 2 φ 2

Bonding and antibonding orbital energies in H2

We typically draw MO energy level diagrams at the equilibrium bond distance

Page 4: ψ 1  = c 1 φ 1  + c 2 φ 2 ψ 2  = c 1 φ 1  - c 2 φ 2

MO energy level diagram for H2 (H2+, HHe, He2, …)

α = Coulomb integral => ionization energy of electron in atomic orbital, e.g., H1s

β = Exchange integral => energy difference between AO and bonding orbital

S = Overlap integral, S12 = ∫φ1*φ2dτ

Page 5: ψ 1  = c 1 φ 1  + c 2 φ 2 ψ 2  = c 1 φ 1  - c 2 φ 2

MO diagram for a polar bond (e.g., in HCl)

α values are different because of electronegativity difference between H and Cl

Larger difference between bonding and antibonding orbital energies

Bonding orbital closer in energy to Cl 3pz AO = > bond has more “Cl character”

Page 6: ψ 1  = c 1 φ 1  + c 2 φ 2 ψ 2  = c 1 φ 1  - c 2 φ 2

MO diagram for an ionic bond (e.g., in Na+F-)

Larger energy differenceBonding electron pair is localized on the F atomExcited state is Na0F0

Page 7: ψ 1  = c 1 φ 1  + c 2 φ 2 ψ 2  = c 1 φ 1  - c 2 φ 2

Summary of MO theory so far:

• Add and subtract AO wavefunctions to make MOs. # of AOs = # of MOs.

• More nodes → higher energy MO

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

• Bond polarity emerges in the MO picture as orbital “character.”

• AOs that are far apart in energy do not interact much when they combine to make MOs.

Page 8: ψ 1  = c 1 φ 1  + c 2 φ 2 ψ 2  = c 1 φ 1  - c 2 φ 2

Orbital Symmetry

AO’s of different symmetries (in the point group of the molecule) do not interact

Greatly simplifies the problem of constructing MO’s for complex molecules

Page 9: ψ 1  = c 1 φ 1  + c 2 φ 2 ψ 2  = c 1 φ 1  - c 2 φ 2

MO diagram for HCl molecule

Cl 2px and 2py orbitals have π symmetry – no interaction with σ symmetry orbitals

Cl 3s is too low in energy to interact => nonbonding electron pair

8 electrons => 1 bond + 3 lone pairs (same result as valence bond picture)

Page 10: ψ 1  = c 1 φ 1  + c 2 φ 2 ψ 2  = c 1 φ 1  - c 2 φ 2

σ, π, and δ orbitals in inorganic compounds

Face-to-face overlap of d-orbitals => δ bond

e.g., in [Re2Cl8]2−

Page 11: ψ 1  = c 1 φ 1  + c 2 φ 2 ψ 2  = c 1 φ 1  - c 2 φ 2

σ and π bonding in metal d-orbital complexes

Ligand acts as a σ donor (= Lewis base), empty d-orbital is σ acceptor (Lewis acid)

Ligands can also act as π donors or π acceptors

Early transition metalEmpty d-orbital

Late transition metalFilled d-orbital

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MO diagram for 2nd row diatomic molecules

Li2, Be2, B2, C2, N2 O2, F2

Fill up MOs in Aufbau order

O2 = 12 e = double bond, 2 unpaired electrons (paramagnetic)

B2, C2?

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O2 MO diagram & orbitals

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π-bonding: 2nd row vs. 3rd (4th, 5th, 6th) rows

Ethylene: Stable molecule, doesn't polymerize without a catalyst.

Silylene: Never isolated, spontaneously polymerizes.

The large Ne core of Si atoms inhibits sideways overlap of 3p orbitals → weak π-bond

N can make π-bonds, so N2 has a very strong triple bond and is a relatively inert diatomic gas

“RTV” silicone polymer (4 single bonds to Si) vs. acetone (C=O double bond)