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Published byCaroline Merilyn Arnold Modified over 9 years ago
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ψ 1 = c 1 φ 1 + c 2 φ 2 ψ 2 = c 1 φ 1 - c 2 φ 2 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)
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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
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Bonding and antibonding orbital energies in H 2 We typically draw MO energy level diagrams at the equilibrium bond distance
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MO energy level diagram for H 2 (H 2 +, HHe, He 2, …) 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, S 12 = ∫φ 1 *φ 2 dτ
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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”
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MO diagram for an ionic bond (e.g., in Na + F - ) Larger energy difference Bonding electron pair is localized on the F atom Excited state is Na 0 F 0
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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.
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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
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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)
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σ, π, and δ orbitals in inorganic compounds Face-to-face overlap of d-orbitals => δ bond e.g., in [Re 2 Cl 8 ] 2−
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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 metal Empty d-orbital Late transition metal Filled d-orbital
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MO diagram for 2 nd row diatomic molecules Li 2, Be 2, B 2, C 2, N 2 O 2, F 2 Fill up MOs in Aufbau order O 2 = 12 e = double bond, 2 unpaired electrons (paramagnetic) B 2, C 2 ?
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O 2 MO diagram & orbitals
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π-bonding: 2 nd row vs. 3 rd (4 th, 5 th, 6 th ) 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 N 2 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)
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