Chapter 9 Molecular Geometries and Bonding Theories

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Chapter 9 Molecular Geometries and Bonding Theories

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Chapter 9 Molecular Geometries and Bonding Theories. Multiple Bonds. Formation of two π bonds in acetylene. Fig 9.26. Describing σ and π bonds in a molecule. σ. σ. formaldehyde. σ. π. Fig 9.27 Formation of σ and π bonds in formaldehyde, CH 2 O. - PowerPoint PPT Presentation

Transcript of Chapter 9 Molecular Geometries and Bonding Theories

Page 1: Chapter 9 Molecular Geometries and Bonding Theories

Chapter 9Molecular Geometriesand Bonding Theories

Page 2: Chapter 9 Molecular Geometries and Bonding Theories

Multiple Bonds

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Formation of two π bonds in acetylene

Fig 9.26

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Fig 9.27 Formation of σ and π bonds in formaldehyde, CH2O

Describing σ and π bonds in a molecule

formaldehyde σ

σ

σ

π

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Sigma () and Pi Bonds ()

Single bond 1 sigma bond

Double bond 1 sigma bond and 1 pi bond

Triple bond 1 sigma bond and 2 pi bonds

How many and bonds are in the acetic acid(vinegar) molecule CH3COOH?

C

H

H

CH

O

O H bonds = 6 + 1 = 7

bonds = 1

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Molecular Orbital (MO) Theory

• If waves interact constructively, the resulting orbital is lower in energy: a bonding molecular orbital.

• If waves interact destructively, the resulting orbital is higher in energy: an antibonding molecular orbital.

In MO theory, we invoke the wave nature of electrons

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MO Theory

In H2 the two electrons go into the bonding molecular orbital.

The bond order is one half the difference between the number of bonding and antibonding electrons:

Bond order = ½ (no. of bonding e− – no. of antibonding e−)

Here: ½ (2-0) = 1

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MO Theory

In the case of He2, the bond order would be:

• Therefore, MO theory predicts that He2 does not exist, which we know to be true.

Here: ½ (2-2) = 0

Fig 9.35

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• In the case of He2+, the

bond order would be:

MO TheoryHe2

+

½ (2-1) = 1/2

• Therefore, MO theory predicts that He2+ does exist and it will be

relatively stable

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MO Theory – Second-Row Diatomics

Consider only homonuclear diatomic molecules

• Number of MOs = number of AOs combined

• AOs combine most effectively with other AOs of similar energy

• The greater the overlap of AOs, the lower the energy of MO

• Each MO can hold max of 2 electrons (Pauli exclusion)

• Hund’s rule applies (same spin in degenerate orbitals)

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MOs for Li2 and Be2

Fig 9.37 Energy-level diagram for the Li2 molecule

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For atoms with both s and p orbitals, there are two types of interactions:

The p orbitals that are head to head overlap in fashion.

The other two sets of p orbitals overlap in fashion.

MOs from 2p Atomic OrbitalsFig 9.38

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• There are both and bonding molecular orbitals and * and * antibonding molecular orbitals

• Diagram fits only O2 and F2

MO Theory – Second-Row DiatomicsFig 9.43

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MO Theory• The smaller p-block elements in the

second period have a sizeable interaction between the s and p orbitals:

• This flips the order of the and molecular orbitals in O2 and F2

Fig 9.45

Fig 9.44

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Fig 9.48 Paramagentism of O2

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Figure 09.48

Fig 9.48 Paramagentism of O2