Unit 1.1(Molecular Orbital Theory)

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ENGINEERING CHEMISTRY DR FARHAT A ANSARI ASSISTANT PROFESSOR (AS) JETGI

Transcript of Unit 1.1(Molecular Orbital Theory)

Page 1: Unit 1.1(Molecular Orbital Theory)

ENGINEERING CHEMISTRY

DR FARHAT A ANSARIASSISTANT PROFESSOR (AS)

JETGI

Page 2: Unit 1.1(Molecular Orbital Theory)

Molecular Orbital TheoryBand Theory of SolidsLiquid Crystal & Its ApplicationPoint Defects in SolidsStructure of Graphite & Fullerene

UNIT-I

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Molecular Orbital Theory

1. MO theory suggests that atomic orbitals of different atoms combine to create MOLECULAR ORBITALS

2. Electrons in these MOLECULAR ORBITALS belong to the molecule as whole

3. This contrasts to VB theory which suggests that electrons

are shared by simple overlap atomic orbital's or hybridized atomic orbital's .

4. Molecular orbital can be constructed from linear combination of atomic orbital's

MO = LCAO

INTRODUCTION

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Rules for linear combination

1. Atomic orbital's must be roughly of the same energy.

2. The orbital must overlap one another as much as possible- atoms must be close enough for effective overlap.

3. In order to produce bonding and antibonding MOs, either the symmetry of two atomic orbital must remain unchanged when rotated about the internuclear line or both atomic orbital's must change symmetry in identical manner.

Linear combination of atomic orbitals

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Rules for the use of MOs * When two AOs mix, two MOs will be produced * Each orbital can have a total of two electrons (Pauli principle) * Lowest energy orbitals are filled first (Aufbau principle) * Unpaired electrons have parallel spin (Hund’s rule)

Bond order = ½ (bonding electrons – antibonding electrons)

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A B

A B

AB = N(cA A + cBB)

Linear Combination of Atomic Orbitals (LCAO)

2AB = (cA2 A2 + 2cAcB A B + cB2 B 2)

Overlap integral

The wave function for the molecular orbitals can be approximated by taking linear combinations of atomic orbitals.

Probability density

c – extent to which each AOcontributes to the MO

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When 2 atomic orbitals combine there are 2 resultant orbitals.

low energy bonding orbital

high energy antibonding orbital1sb 1sa

s1s

s*

E 1s

Molecularorbitals

Eg. s orbitals

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First period diatomic molecules

s1s2H

Energy

HH2

1s 1s

sg

su*

Bond order = ½ (bonding electrons – antibonding electrons)

Bond order: 1

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s1s2, s*1s2 HeEnergy

HeHe2

1s 1s

sg

su*

Molecular Orbital theory is powerful because it allows us to predict whether molecules should exist or not and it gives us a clear picture of the of the electronic structure of any hypothetical molecule that we can imagine.

Diatomic molecules: The bonding in He2

Bond order: 0

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Second period diatomic molecules

s1s2, s*1s2, s2s2

Bond order: 1

Li

Energy

LiLi2

1s 1s

1sg

1su*

2s 2s

2sg

2su*

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s1s2, s*1s2, s2s2, s*2s2

Bond order: 0

BeEnergy

BeBe2

1s 1s

1sg

1su*

2s 2s

2sg

2su*

Diatomic molecules: Homonuclear Molecules of the Second Period

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Diamagnetic

2sg

2su*

3sg

1u

1g*

3su*

MO diagram for B2

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Simplified

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Simplified

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