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MO Diagrams for Diatomic Molecules: Understanding Bonding and Orbital Interactions, Study notes of Chemistry

The use of MO (Molecular Orbital) diagrams to understand the electronic structures and bonding in diatomic molecules. Topics include homonuclear and heteronuclear diatomic molecules, orbital interactions, bond orders, and MO energies. The document also discusses the importance of symmetry in treating larger molecules within the LCAO-MO (Linear Combination of Atomic Orbitals - Molecular Orbitals) theory framework.

What you will learn

  • How do homonuclear and heteronuclear diatomic molecules differ in their MO diagrams?
  • What factors control the internuclear distance in diatomic molecules?
  • What role does symmetry play in treating larger molecules within the LCAO-MO theory framework?
  • How do orbital interactions and mixing affect the energies and bonding in diatomic molecules?
  • What is LCAO-MO theory and how is it used to predict the electronic structure of molecules?

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MO Diagrams for
Diatomic Molecules
Chapter 5
Friday, October 9, 2015
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MO Diagrams for

Diatomic Molecules

Chapter 5

Friday, October 9, 2015

Homonuclear Diatomic Molecules

What happens when we move to more complicated systems?Consider O

.

-^

The Lewis dot structure famously predicts the wrong electronicstructure for O

-^

We can use LCAO-MO theory to get a better picture:

s^ a

p

a

s^ b

p

b

Notice that

E

E

,

because theσ bonds havemore overlapthan π bonds

E

σ^

E

π

Orbital Mixing

Orbitals of similar but unequal energies can interact if they have thesame symmetryThe 2

s

and 2

p

z

orbitals form MOs with the same symmetry (

σ

g

and

σ

u

).

sp mixing

causes the

σ

g^

and

σ

u

MOs to be pushed apart in energy:

The σ andπ orbitals change order!

Orbital Mixing

The size ofthe effectdepends onthe 2s-2penergydifference.

small

Z

eff

=

small energydifference = large

sp

mixing

large

Z

eff

=

large energydifference = small

sp

mixing

order changes

Bond Order and Bond Distance

The MO bond order is the main factor controlling the internucelardistance.

B

2

σ

2 σ*

2 π

2

BO = 1
C

2

σ

2 σ*

2 π

4

BO = 2
N

2

σ

2 σ*

2 π

4 σ

2

BO = 3
O

2

σ

2 σ*

2 σ

2 π

4 π*

2

BO = 2
F

2

σ

2 σ*

2 σ

2 π

4 π*

4

BO = 1
O

- 2

σ

2 σ*

2 σ

2 π

4 π*

3

BO = 1.
O

+ 2

σ

2 σ*

2 σ

2 π

4 π*

1

BO = 2.
N

+ 2

σ

2 σ*

2 π

4 σ

1

BO = 2.
C

2– 2

σ

2 σ*

2 π

4 σ

2

BO = 3

Relative AO Energies for MO Diagrams

Photoelectron spectroscopy

gives us a pretty good idea of the relative

energies for AOs.

H

He

Li

Be

B

C

N

O

F

Ne

B

C

N

O

F

Na Ne

Mg

Al

Si

P

S

Cl

Ar

Al

Si

P

S

Cl

Ar

s

2 s

p

s

p

–13.6 eV

–18.6 eV –40.2 eV

Relative AO Energies for MO Diagrams^ H

He

Li

Be

B

C

N

O

F

Ne

B

C

N

O

F

Na Ne

Mg

Al

Si

P

S

Cl

Ar

Al

Si

P

S

Cl

Ar

s

2 s

p

s

p

–19.4 eV

–15.8 eV

–32.4 eV

–10.7 eV

Photoelectron spectroscopy

gives us a pretty good idea of the relative

energies for AOs.

Energy

Heteronuclear Diatomic Molecules: CO

In molecules with more than one type of atom, MOs are formed fromAOs that have different energies. Consider CO:

2 s

a

p

a

C

s b

2 p

b

O

C≡O

σ

σ*

π

π* σ

σ*

Bonding orbitals

get polarized

towards oxygen

Anti-bonding orbitalsget polarized towards

carbon

HOMO is on carbon

LUMO is on carbon too!