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Molecular orbital theory and its application to form homo
(H2 N2 &O2) and hetero (HF,NO) diatomic molecules.
Molecular Orbital (MO) Theory
 Developed by F. Hund and R.S. Mulliken in 1932
 Diagram of molecular energy levels
 Magnetic and spectral properties
 Paramagnetic vs. Diamagnetic
 Electronic transitions
 Solid State - Conductance
 Predicts existence of molecules
 Bond Order
Molecular Orbital (MO) Theory
 Two atomic orbitals combine to form
 a bonding molecular orbital
 an anti-bonding molecular orbital
 e- in bonding MO’s = stability
 e- in anti-bonding MO’s = instability
 # atomic orbitals combined equals # of molecular
orbitals formed
 The molecular orbitals like atomic orbitals are filled
in accordance with the aufbau principle obeying the
Pauli’s exclusion principle and the Hund’s rule.
Central Themes
 Quantum mechanical level
 Molecule viewed as a collection of nuclei surrounded by
delocalized molecular orbitals
 Atomic wave functions are summed to obtain
molecular wave functions.
 If wave functions reinforce each other, a bonding MO is
formed (region of high electron density exists between
the nuclei).
 If wave functions cancel each other, an antibonding MO
is formed (a node of zero electron density occurs
between the nuclei).
 Formation of Molecular Orbitals Linear
combination of Atomic Orbitals (LCAO)
The atomic orbitals of these atoms may be
represented by the wave functions ψA and ψB.
Therefore, the two molecular orbitals σ and σ*
are formed as :
BA CC  21 
BA CC  21* 
Where the coefficients C, indicate the contribution of the AO to the MO
An Analogy
Amplitudes of wave
functions added
Amplitudes of wave
functions subtracted.
MO: Molecular Hydrogen
The bonding MO is lower in energy than an AO
The anti- bonding MO is higher in energy than an AO
Considerations…
 Bond Order =1/2( # bonding e- – # antibonding e- )
 Higher bond order = stronger bond
 Molecular electron configurations
 Highest Occupied Molecular Orbital = HOMO
 Lowest Unoccupied Molecular Orbital = LUMO
 An Example: H2 (1s)2
MO: Molecular Hydrogen
Predicting Stability: H2
+ & H2
-


1s
AO of H
1s
AO of H
MO of H2
+
bond order
= 1/2(1-0)
= 1/2
H2
+ does exist
bond order
= 1/2(2-1)
= 1/2
H2
- does exist
1s


MO of H2
-
1s
AO of H AO of H-
configuration is (1s)1
configuration is
(1s)2(1s)1
Helium: He2
+ vs He2
Energy
MO of
He+
*1s
1s
AO of
He+
1s
MO of
He2
AO of
He
1s
AO of
He
1s
*1s
1s
Energy
He2
+ bond order = 1/2 He2 bond order = 0
AO of
He
1s
Next Row: 2s & 2p orbitals
*2
s
2s
2s
1s
*1
s
1s
*1
s
1s
1s
2s
*2
s
2s
Li2 B.O. = 1 Be2 B.O. = 0
Bonding in s-block
homonuclear
diatomic molecules.
Energy
Li2
Be2
Combinations for p-orbitals
Axial symmetry
means  bond
Non-axial
symmetry
means  bond
MO – Now with S & P
X 2
X 2
S - P orbital mixing
Relative Energy Levels for 2s & 2p
MO energy levels
for O2, F2, and Ne2
MO energy levels
for B2, C2, and N2
WITHOUT big
2s-2p repulsion
WITH big 2s-2p
repulsion
Triumph for MO Theory?
Can MO Theory Explain Bonding?
SOLUTION:
PROBLEM: As the following data show, removing an electron from N2 forms
an ion with a weaker, longer bond than in the parent molecules,
whereas the ion formed from O2 has a stronger, shorter bond:
PLAN: Find the number of valence electrons for each species, draw the MO
diagrams, calculate bond orders, and then compare the results.
Explain these facts with diagrams that show the sequence and occupancy of MOs.
Bond energy (kJ/mol)
Bond length (pm)
N2 N2
+ O2 O2
+
945
110
498841 623
112121112
N2 has 10 valence electrons, so N2
+ has 9.
O2 has 12 valence electrons, so O2
+ has 11.
Real World Applications
 Most molecules are heteroatomic
 What needs to be considered?
 Orbitals involved
 Electronegativity (Orbital energies)
 Hybridization (Group Theory)
 Mixing
BA CC  21 
BA CC  21* 
Where the coefficients C, indicate the contribution of the AO to the MO
Energy
The MO diagram for NO
MO of NO
2s
AO of N
2p
*2s
2s
2s
AO of O
2p
2p
2p
*2p
*2s
N O
0 0
N O
-1 +1
possible Lewis
structures
Let’s Start Slowly: HF
 Valence electrons
 H – 1s1
 F – 1s2 2s2 2p5
 Focus on the valence interactions
 Accommodate for differences in electronegativity
 Allow mixing between symmetry-allowed states
HFEnergy
MO
of HF
AO
of H
1
s

2px 2py


AO
of F
2p
HOMO is lone pair on C.
CO always binds to
metals via the C end

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introduction to MOT

  • 1. Molecular orbital theory and its application to form homo (H2 N2 &O2) and hetero (HF,NO) diatomic molecules.
  • 2. Molecular Orbital (MO) Theory  Developed by F. Hund and R.S. Mulliken in 1932  Diagram of molecular energy levels  Magnetic and spectral properties  Paramagnetic vs. Diamagnetic  Electronic transitions  Solid State - Conductance  Predicts existence of molecules  Bond Order
  • 3. Molecular Orbital (MO) Theory  Two atomic orbitals combine to form  a bonding molecular orbital  an anti-bonding molecular orbital  e- in bonding MO’s = stability  e- in anti-bonding MO’s = instability  # atomic orbitals combined equals # of molecular orbitals formed  The molecular orbitals like atomic orbitals are filled in accordance with the aufbau principle obeying the Pauli’s exclusion principle and the Hund’s rule.
  • 4. Central Themes  Quantum mechanical level  Molecule viewed as a collection of nuclei surrounded by delocalized molecular orbitals  Atomic wave functions are summed to obtain molecular wave functions.  If wave functions reinforce each other, a bonding MO is formed (region of high electron density exists between the nuclei).  If wave functions cancel each other, an antibonding MO is formed (a node of zero electron density occurs between the nuclei).
  • 5.  Formation of Molecular Orbitals Linear combination of Atomic Orbitals (LCAO) The atomic orbitals of these atoms may be represented by the wave functions ψA and ψB. Therefore, the two molecular orbitals σ and σ* are formed as : BA CC  21  BA CC  21*  Where the coefficients C, indicate the contribution of the AO to the MO
  • 6. An Analogy Amplitudes of wave functions added Amplitudes of wave functions subtracted.
  • 7. MO: Molecular Hydrogen The bonding MO is lower in energy than an AO The anti- bonding MO is higher in energy than an AO
  • 8. Considerations…  Bond Order =1/2( # bonding e- – # antibonding e- )  Higher bond order = stronger bond  Molecular electron configurations  Highest Occupied Molecular Orbital = HOMO  Lowest Unoccupied Molecular Orbital = LUMO  An Example: H2 (1s)2
  • 10. Predicting Stability: H2 + & H2 -   1s AO of H 1s AO of H MO of H2 + bond order = 1/2(1-0) = 1/2 H2 + does exist bond order = 1/2(2-1) = 1/2 H2 - does exist 1s   MO of H2 - 1s AO of H AO of H- configuration is (1s)1 configuration is (1s)2(1s)1
  • 11. Helium: He2 + vs He2 Energy MO of He+ *1s 1s AO of He+ 1s MO of He2 AO of He 1s AO of He 1s *1s 1s Energy He2 + bond order = 1/2 He2 bond order = 0 AO of He 1s
  • 12.
  • 13. Next Row: 2s & 2p orbitals *2 s 2s 2s 1s *1 s 1s *1 s 1s 1s 2s *2 s 2s Li2 B.O. = 1 Be2 B.O. = 0 Bonding in s-block homonuclear diatomic molecules. Energy Li2 Be2
  • 14. Combinations for p-orbitals Axial symmetry means  bond Non-axial symmetry means  bond
  • 15. MO – Now with S & P X 2 X 2
  • 16. S - P orbital mixing
  • 17. Relative Energy Levels for 2s & 2p MO energy levels for O2, F2, and Ne2 MO energy levels for B2, C2, and N2 WITHOUT big 2s-2p repulsion WITH big 2s-2p repulsion
  • 18.
  • 19. Triumph for MO Theory?
  • 20. Can MO Theory Explain Bonding? SOLUTION: PROBLEM: As the following data show, removing an electron from N2 forms an ion with a weaker, longer bond than in the parent molecules, whereas the ion formed from O2 has a stronger, shorter bond: PLAN: Find the number of valence electrons for each species, draw the MO diagrams, calculate bond orders, and then compare the results. Explain these facts with diagrams that show the sequence and occupancy of MOs. Bond energy (kJ/mol) Bond length (pm) N2 N2 + O2 O2 + 945 110 498841 623 112121112 N2 has 10 valence electrons, so N2 + has 9. O2 has 12 valence electrons, so O2 + has 11.
  • 21. Real World Applications  Most molecules are heteroatomic  What needs to be considered?  Orbitals involved  Electronegativity (Orbital energies)  Hybridization (Group Theory)  Mixing BA CC  21  BA CC  21*  Where the coefficients C, indicate the contribution of the AO to the MO
  • 22. Energy The MO diagram for NO MO of NO 2s AO of N 2p *2s 2s 2s AO of O 2p 2p 2p *2p *2s N O 0 0 N O -1 +1 possible Lewis structures
  • 23. Let’s Start Slowly: HF  Valence electrons  H – 1s1  F – 1s2 2s2 2p5  Focus on the valence interactions  Accommodate for differences in electronegativity  Allow mixing between symmetry-allowed states
  • 24. HFEnergy MO of HF AO of H 1 s  2px 2py   AO of F 2p
  • 25. HOMO is lone pair on C. CO always binds to metals via the C end