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Theories of Bonding and Structure CHAPTER 10 Chemistry: The Molecular Nature of Matter, 6 th edition By Jesperson, Brady, & Hyslop

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Theories of Bonding and Structure CHAPTER 10 Chemistry: The Molecular Nature of Matter, 6 th edition By Jesperson , Brady, & Hyslop. CHAPTER 10: Bonding & Structure. Learning Objectives VESPR theory: Determine molecular geometry based on molecular formula and/or lewis dot structures. - PowerPoint PPT Presentation

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Page 1: Theories of Bonding and Structure CHAPTER 10

Theories of Bonding and Structure

CHAPTER 10

Chemistry: The Molecular Nature of Matter, 6th editionBy Jesperson, Brady, & Hyslop

Page 2: Theories of Bonding and Structure CHAPTER 10

2

CHAPTER 10: Bonding & Structure

Learning Objectives VESPR theory:

Determine molecular geometry based on molecular formula and/or lewis dot structures.

Effect of bonded atoms & non-bonded electrons on geometry Molecular polarity & overall dipole moment

Assess overall dipole moment of a molecule Identify polar and non-polar molecules

Valence Bond Theory Hybridized orbitals Multiple bonds Sigma vs pi orbitals

Molecular Orbital Theory Draw & label molecular orbital energy diagrams Bonding & antibonding orbitals Predict relative stability of molecules based on MO diagrams

Page 3: Theories of Bonding and Structure CHAPTER 10

3

Molecular Geometry Basic Molecular Geometries

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Linear3 atoms

Trigonal Planaror

Planar Triangular

4 atoms

Tetrahedral:5 atoms

Trigonal Bipyramidal6 atoms

Octahedral:7 atoms

Page 4: Theories of Bonding and Structure CHAPTER 10

4

VESPR Definition

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E http://chemistry-desk.blogspot.com/2011/05/prediction-of-shape-of-molecules-by.html

Valence Shell Electron Pair Repulsion ModelElectron pairs (or groups of electron pairs) in the valence shell of an atom repel each other and will position themselves so that they are far apart as

possible, thereby minimizing the repulsions.

Electron pairs can either be lone pairs or bonding pairs.

Tetrahedral arrangement of electron pairsBent geometry

Page 5: Theories of Bonding and Structure CHAPTER 10

5

VESPR Definition

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Valence Shell Electron Pair Repulsion ModelElectron pairs (or groups of electron pairs) in the valence shell of an atom repel each other and will position themselves so that they are far apart as

possible, thereby minimizing the repulsions.

Text uses “electron domain” to describe electron pairs:

Bonding domain: contains electrons that are shared between two atoms. So electrons involved in single, double, or triple are

part of the same bonding domain.

Nonbonding Domain: Valence electrons associated with one atom, such as a lone pair, or a unpaired electron.

Page 6: Theories of Bonding and Structure CHAPTER 10

6

VESPR Basic Examples

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

2 bonding domains

3 bonding domains

4 bonding domains

5 bonding domains

6 bonding bonding domains

Page 7: Theories of Bonding and Structure CHAPTER 10

7

VESPR When Lone Pairs or Multiple Bonds Present

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Including lone pairs: • Take up more space around central atom • Effect overall geometry • Counted as nonbonded electron domains

Including multiple bonds (double and triple) • For purposes of determining geometry focus on the number

of atoms bonded together rather then the number of bonds in between them: ie, treat like a single bond.

• Treat as single electron bonding domain

Page 8: Theories of Bonding and Structure CHAPTER 10

8

VESPR Electrons that are Bonding & Not Bonding

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Bonding Electrons – More oval in shape – Electron density focused

between two positive nuclei.

Nonbonding Electrons– More bell or balloon shaped– Take up more space – Electron density only has positive

nuclei at one end

Page 9: Theories of Bonding and Structure CHAPTER 10

9

VESPR 3 atoms or lone pairs

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Number of Bonding Domains

3

2

Number of Nonbonding Domains

0

1

Molecular Shape

Planar Triangular(e.g. BCl3)All bond angles 120

NonlinearBent or V-shaped(e.g. SnCl2)

Bond <120

Structure

Page 10: Theories of Bonding and Structure CHAPTER 10

10

VESPR 4 atoms or lone pairs

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Number of Bonding Domains

4

3

2

Number of Nonbonding Domains

0

1

2

Molecular Shape

Tetrahedron(e.g. CH4)All bond angles 109.5

Trigonal pyramidal(e.g. NH3)Bond angle less than 109.5

Nonlinear, bent(e.g. H2O)Bond angle less than109.5

Structure

Page 11: Theories of Bonding and Structure CHAPTER 10

11

VESPR 5 atoms or lone pairs

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

90

120

Trigonal Bipyramidal• Two atoms in axial position

– 90 to atoms in equatorial plane

• Three atoms in equatorial position– 120 bond angle to atoms

in axial position– More room here– Substitute here first

Page 12: Theories of Bonding and Structure CHAPTER 10

12

VESPR 5 atoms or lone pairs

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Number of Bonding Domains

5

4

Number of Nonbonding Domains

0

1

Molecular Shape

Trigonal bipyramid(e.g. PF5)Ax-eq bond angles 90Eq-eq 120

Distorted Tetrahedron, or Seesaw(e.g. SF4)Ax-eq bond angles < 90

Structure

Page 13: Theories of Bonding and Structure CHAPTER 10

13

5 atoms or lone pairs

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Lone pair takes up more space• Goes in equatorial plane• Pushes bonding pairs out of way• Result: distorted tetrahedron

VESPR

Page 14: Theories of Bonding and Structure CHAPTER 10

14

VESPR 5 atoms or lone pairs

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Number of Bonding Domains

3

2

Number of Nonbonding Domains

2

3

Molecular Shape

T-shape(e.g. ClF3)Bond angles 90

Linear(e.g. I3

–)Bond angles 180

Structure

Page 15: Theories of Bonding and Structure CHAPTER 10

15

VESPR 6 atoms or lone pairs

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Number of Bonding Domains

6

5

Molecular Shape

Octahedron(e.g. SF6)

Square Pyramid(e.g. BrF5)

StructureNumber of Nonbonding Domains

0

1

Page 16: Theories of Bonding and Structure CHAPTER 10

16

VESPR 6 atoms or lone pairs

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Number of Bonding Domains

4

Number of Nonbonding Domains

2

Molecular Shape

Square planar(e.g. XeF4)

Structure

Page 17: Theories of Bonding and Structure CHAPTER 10

17

VESPR Determining 3-D Structures

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

1. Draw Lewis Structure of Molecule– Don't need to compute formal charge– If several resonance structures exist, pick only one

2. Count electron pair domains– Lone pairs and bond pairs around central atom– Multiple bonds count as one set (or one effective pair)

3. Arrange electron pair domains to minimize repulsions• Lone pairs

– Require more space than bonding pairs– May slightly distort bond angles from those predicted.– In trigonal bipyramid lone pairs are equatorial – In octahedron lone pairs are axial

4. Name molecular structure by position of atoms—only bonding electrons

Page 18: Theories of Bonding and Structure CHAPTER 10

Molecular Polarity Polar Molecules

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

18

• Have net dipole moment– Negative end– Positive end

• Polar molecules attract each other.– Positive end of polar molecule attracted to

negative end of next molecule.– Strength of this attraction depends on

molecule's dipole moment– Dipole moment can be determined

experimentally• Polarity of molecule can be predicted by taking

vector sum of bond dipoles• Bond dipoles are usually shown as crossed

arrows, where arrowhead indicates negative end

Page 19: Theories of Bonding and Structure CHAPTER 10

19

Molecular Polarity Molecular Shape & Polarity

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6Ehttp://wps.prenhall.com/wps/media/objects/3081/3155729/blb0903.html

• Many physical properties (melting and boiling points) affected by molecular polarity

• For molecule to be polar:– Must have polar bonds

• Many molecules with polar bonds are nonpolar - Possible because certain

arrangements of bond dipoles cancel

- For molecules with more than two atoms, must consider the combined effects of all polar bonds

Page 20: Theories of Bonding and Structure CHAPTER 10

20

Molecular Polarity Symmetrical Nonpolar Molecules

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Symmetrical molecules – Nonpolar because bond dipoles cancel

• All five shapes are symmetrical when all domains attached to them are composed of identical atoms

Page 21: Theories of Bonding and Structure CHAPTER 10

21

Molecular Polarity Symmetrical Nonpolar Molecules

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Cancellation of Bond Dipoles In Symmetrical Trigonal Bipyramidal and Octahedral Molecules

• All electron pairs around central atom are bonding pairs and • All terminal groups (atoms) are same• The individual bond dipoles cancel

Page 22: Theories of Bonding and Structure CHAPTER 10

22

Molecular Polarity Polar Molecules

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Molecule is usually polar if – All atoms attached to central atom are NOT same Or, – There are one or more lone pairs on central atom

Page 23: Theories of Bonding and Structure CHAPTER 10

23

Molecular Polarity Polar Molecules

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Water and ammonia both have non-bonding domains Bond dipoles do not cancel Molecules are polar

Page 24: Theories of Bonding and Structure CHAPTER 10

24

Molecular Polarity Polar Molecules: Exception

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Exception to these general rules for identifying polar molecules:

Nonbonding domains (lone pairs) are symmetrically placed around central atom

Page 25: Theories of Bonding and Structure CHAPTER 10

25

ProblemSet A

1. For the following molecules: a. Draw a lewis dot structure.b. Determine the molecular geometry at each central atom.c. Identify the bond angles.d. Identify all polar bonds: δ+ / δ-e. Assess the polarity of the molecule & indicate the overall

dipole moment if one exists

AsF5 AsF3 SeO2

GaH3

ICl2- SiO4-4

TeF6

Page 26: Theories of Bonding and Structure CHAPTER 10

26

VB Theory Review: Modern Atomic Theory of Bonding

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Modern Atomic Theory of Bonding is based on wave mechanics and gave us:

– Electrons and shapes of orbitals– Four quantum numbers– Heisenberg uncertainty principle

• Electron probabilities– Pauli Exclusion Principle

Page 27: Theories of Bonding and Structure CHAPTER 10

27

VB Theory Valence Bond Theory & Molecular Orbital Theory

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Valence Bond Theory• Individual atoms, each have their own orbitals and orbitals

overlap to form bonds• Extent of overlap of atomic orbitals is related to bond strength

Molecular Orbital Theory • Views molecule as collection of positively charged nuclei

having a set of molecular orbitals that are filled with electrons (similar to filling atomic orbitals with electrons)

• Doesn't worry about how atoms come together to form molecule

Page 28: Theories of Bonding and Structure CHAPTER 10

28

VB Theory Valence Bond Theory & Molecular Orbital Theory

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Both Theories:• Try to explain structure of molecules, strengths of

chemical bonds, bond orders, etc.• Can be extended and refined and often give same

results

Valence Bond Theory Bond between two atoms formed when pair of electrons with paired (opposite) spins is shared by two overlapping atomic orbitals

Page 29: Theories of Bonding and Structure CHAPTER 10

29

VB Theory H2

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

H2 bonds form because 1s atomic valence orbital from each H atom overlaps

Page 30: Theories of Bonding and Structure CHAPTER 10

30

VB Theory F2

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• F2 bonds form because atomic valence orbitals overlap• Here 2p overlaps with 2p• Same for all halogens, but different np orbitals

Page 31: Theories of Bonding and Structure CHAPTER 10

31

VB Theory HF

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

HF involves overlaps between 1s orbital on H and 2p orbital of F

1s 2p

Page 32: Theories of Bonding and Structure CHAPTER 10

32

VB Theory H2S

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Predicted 90˚ bond angle is very close to experimental value of 92˚.

• Assume that unpaired electrons in S and H are free to form paired bond

• We may assume that H—S bond forms between s and p orbital

Page 33: Theories of Bonding and Structure CHAPTER 10

33

VB Theory Need to Change Approach to Explain Bonding in CH4

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Example: CH4 C 1s 22s 22p 2 and H 1s 1

• In methane, CH4 – All four bonds are the same– Bond angles are all 109.5°

• Carbon atoms have– All paired electrons except two unpaired 2p– p orbitals are 90° apart– Atomic orbitals predict CH2 with 90° angles

Page 34: Theories of Bonding and Structure CHAPTER 10

34

VB Theory Hybridization

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Mixing of atomic orbitals to allow formation of bonds that have realistic bond angles.– Realistic description of bonds often requires combining

or blending two or more atomic orbitals• Hybridization just rearranging of electron probabilities

Why do it? • To get maximum possible overlap• Best (strongest) bond formed

Page 35: Theories of Bonding and Structure CHAPTER 10

35

VB Theory Hybrid Orbitals

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Blended orbitals result from hybridization process• Hybrid orbitals have

– New shapes– New directional properties– Each hybrid orbital combines properties of parent atomic

orbitals

Page 36: Theories of Bonding and Structure CHAPTER 10

36

VB Theory Hybrid Orbitals

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Symbols for hybrid orbitals combine the symbols of the orbitals used to form them– Use s + p form two sp hybrid orbitals– Use s + p + p form three sp 2 hybrid orbitals

• One atomic orbital is used for each hybrid orbital formed

• Sum of exponents in hybrid orbital notation must add up to number of atomic orbitals used

Page 37: Theories of Bonding and Structure CHAPTER 10

37

VB Theory Hybrid Orbitals

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Mixing or hybridizing s and p orbital of same atom results in two sp hybrid orbitals

Two sp hybrid orbitals point in opposite directions

Page 38: Theories of Bonding and Structure CHAPTER 10

38

VB Theory Ex: sp Hybridized Orbitals: BeH2

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Now have two sp hybrid orbitals • Oriented in correct direction for

bonding• 180 bond angles

– As VSEPR predicts and– Experiment verifies

• Bonding = – Overlap of H 1s atomic

orbitals with sp hybrid orbitals on Be

Page 39: Theories of Bonding and Structure CHAPTER 10

39

VB Theory Hybrid Orbitals

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Hybrid Atomic Orbitals Used Electron Geometry

sp s + p LinearBond angles 180°

sp2 s + p + p Trigonal planarBond angles 120°

sp3 s + p + p + p TetrahedralBond angles 109.5°

sp3d s + p + p + p + d Trigonal BipyramidalBond angles 90° and 120°

sp3d2 s + p + p + p + d + d OctahedralBond angles 90°

Page 40: Theories of Bonding and Structure CHAPTER 10

40

VB Theory Bonding in BCl3

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Overlap of each half- filled 3p orbital on Cl with each half-filled sp2 hybrid on B

Forms three equivalent bonds

Trigonal planar shape 120 bond angle

Page 41: Theories of Bonding and Structure CHAPTER 10

41

VB Theory

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Overlap of each half- filled 1s orbital on H with each half-filled sp3 hybrid on carbon

Forms four equivalent bonds Tetrahedral geometry 109.5 bond angle

Bonding in CH4

Page 42: Theories of Bonding and Structure CHAPTER 10

42

VB Theory Hybrid sp Orbitals

Two sp hybrids

Three sp2 hybrids

Four sp3 hybrids

Linear

Planar Triangular

Tetrahedral

All angles 120

All angles 109.5

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Page 43: Theories of Bonding and Structure CHAPTER 10

43

VB Theory Expanded Octet Hybridization

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Hybridization When Central Atom has More Than Octet• If there are more than four equivalent bonds on central atom, then must add

d orbitals to make hybrid orbitalsWhy? • One s and three p orbitals means that four equivalent orbitals is the most you

can get using s and p orbitals alone

So, only atoms in third row of the periodic table and below can exceed their octet• These are the only atoms that have empty d orbitals of same n level as

s and p that can be used to form hybrid orbitals• One d orbital is added for each pair of electrons in excess of standard

octet

Page 44: Theories of Bonding and Structure CHAPTER 10

44

VB Theory Expanded Octet Hybridization

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Page 45: Theories of Bonding and Structure CHAPTER 10

45

VB Theory Hybridization in Molecules with Lone Pairs

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

CH4 sp3 tetrahedral geometry 109.5° bond angleNH3

107° bond angleH2O

104.5° bond angle• Angles suggest that NH3 and H2O both use sp3 hybrid orbitals in

bonding• Not all hybrid orbitals used for bonding e–

– Lone pairs can occupy hybrid orbitals• Lone pairs must always be counted to determine geometry

Page 46: Theories of Bonding and Structure CHAPTER 10

46

VB Theory Ex: H2O Hybridization

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Page 47: Theories of Bonding and Structure CHAPTER 10

47

VB Theory Multiple Bonds

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• So where do extra electron pairs in multiple bonds go?– Not in hybrid orbitals– Remember VSEPR, multiple bonds have no

effect on geometry• Why don’t they effect geometry?

Two types of bond result from orbital overlap• Sigma () bond

– Accounts for first bond• Pi () bond

– Accounts for second and third bonds

Page 48: Theories of Bonding and Structure CHAPTER 10

48

VB Theory Sigma () Bonds

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Head on overlap of orbitals• Concentrate electron density concentrated most

heavily between nuclei of two atoms• Lie along imaginary line joining their nuclei

s + s

p + p

sp + sp

Page 49: Theories of Bonding and Structure CHAPTER 10

49

VB Theory Pi () Bonds

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Sideways overlap of unhybridized p orbitals • Electron density divided into two regions

– Lie on opposite sides of imaginary line connecting two atoms

• Electron density above and below bond.

No electron density along bond axis

bond consists of both regions

Both regions = one bond

Page 50: Theories of Bonding and Structure CHAPTER 10

50

VB Theory Pi () Bonds

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Can never occur alone– Must have bond

• Can form from unhybridized p orbitals on adjacent atoms after forming bonds

• bonds allow atoms to form double and triple bonds

Page 51: Theories of Bonding and Structure CHAPTER 10

51

VB Theory Multiple Bonds Ex: Ethene (C2H4)

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Each carbon is – sp

2 hybridized (violet)– has one unhybridized p

orbital (red)

• C=C double bond is– one bond (sp

2 – sp 2 )

– one bond (p – p)

p—p overlap forms a C—C bond

Page 52: Theories of Bonding and Structure CHAPTER 10

52

VB Theory Conformations

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• C—C single bond has free rotation around the C—C bond

• Conformations– Different relative

orientations on molecule upon rotation

Page 53: Theories of Bonding and Structure CHAPTER 10

53

VB Theory Conformations Ex: Pentane, C5H12

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Page 54: Theories of Bonding and Structure CHAPTER 10

54

VB Theory Properties of -Bonds

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Can’t rotate about double bond

• bond must first be broken before rotation can occur

Page 55: Theories of Bonding and Structure CHAPTER 10

55

Ex: Bonding in Formaldehyde

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• C and O each – sp 2 hybridized

(violet)– Has one

unhybridized p orbital (red)

C=O double bond is one bond (sp2 – sp2) one bond

(p – p)

Unshared pairs of electrons on oxygen in sp2 orbitals

sp2—sp2 overlap to form C—O bond

VB Theory

Page 56: Theories of Bonding and Structure CHAPTER 10

56

Bonding in Ethyne, C2H2

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Each carbon is sp hybridized (violet) Has two unhybridized p

orbitals, px and py (red)

CC triple bond one bond

sp – sp two bonds

px – px

py – py

VB Theory

Page 57: Theories of Bonding and Structure CHAPTER 10

57

VB Theory Ex: Bonding in N2

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Each nitrogen sp hybridized (violet) Has two unhybridized p orbitals,

px and py (red)NN triple bond one bond

sp – sp two bonds

px – px

py – py

Page 58: Theories of Bonding and Structure CHAPTER 10

58

ProblemSet B

2. What is the hybridization of oxygen in OCl2? 3. For the species and XeF4O, determine the following:

a. electron domain geometry (geometry including non-bonding pairs)

b. molecular geometryc. Hybridization around central atomd. Polarity

4. How many and bonds are there in CH2CHCHCH2, and what is the hybridization around the carbon atoms?

5. Draw & list the bonding orbitals for HCN.

Page 59: Theories of Bonding and Structure CHAPTER 10

59

ProblemSet B

2. sp3

3. XeF4O: octahedral, square pyramid, sp3d2, polar

4. 9, 2, sp2

5. HCN: C will be create a σ bond to H and N with sp2 hybridized orbitals and use 2 p orbitals to participate in 2 π bonds with N. N will participate in the σ bond with C with an sp2 hybridized orbital, the other will hold the N lone pair, and then N will use 2 p orbitals to π bond with C.

Page 60: Theories of Bonding and Structure CHAPTER 10

60

MO Theory Molecular Orbital Theory

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

1. Molecular orbitals are associated with entire molecule as opposed to one atom

2. Allows us to accurately predict magnetic properties of molecules

3. Energies of molecular orbitals determined by combining electron waves of atomic orbitals

Molecular Orbital Theory Views molecule as collection of positively charged nuclei having a set of molecular orbitals that are filled with electrons (similar

to filling atomic orbitals with electrons)Doesn't worry about how atoms come together to form

molecule

Page 61: Theories of Bonding and Structure CHAPTER 10

61

MO Theory Bonding Molecular Orbitals

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Come from various combinations of atomic orbital wave functions

• For H2, two 1s wave functions, one from each atom, combine to make two molecular orbital wave functions

1sA + 1sB Combined Bonding MO

Constructive interference of waves Energy of bonding MO lower than atomic orbitals

Page 62: Theories of Bonding and Structure CHAPTER 10

62

MO Theory * Antibonding Molecular Orbitals

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Destructive interference of the 1s waves• Energy of the bonding molecular orbital is higher

than energy of parent atomic orbitals

• Number of atomic orbitals used must equal number of molecular orbitals

• Other possible combination of two 1s orbitals: 1sA – 1sB

Page 63: Theories of Bonding and Structure CHAPTER 10

63

Summary of MO from 1s Atomic Orbital

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Bonding molecular orbital– Electron density builds up between nuclei– Electrons in bonding MOs tend to stabilize molecule

• Antibonding molecular orbital– Cancellation of electron waves reduces electron density

between nuclei– Electrons in antibonding MOs tend to destabilize molecule

MO Theory

Page 64: Theories of Bonding and Structure CHAPTER 10

64

MO Theory MO Diagram for H2

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Page 65: Theories of Bonding and Structure CHAPTER 10

65

MO Theory Rules for Filling in MO Energy Diagrams

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

1. Electrons fill lowest-energy orbitals that are available– Aufbau principle applies

2. No more than two electrons, with spin paired, can occupy any orbital

– Pauli exclusion principle applies3. Electrons spread out as much as possible, with spins unpaired,

over orbitals of same energy– Hund’s rules apply

Page 66: Theories of Bonding and Structure CHAPTER 10

66

MO Theory Bond Order

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Measure of number of electron pairs shared between two atoms

• H2 bond order = 1• A bond order of 1 corresponds to a single bond

Page 67: Theories of Bonding and Structure CHAPTER 10

67

MO Theory MO Diagram for He2

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Four electrons, so both and * molecular orbitals are filled

• Bond order

• There is no net bonding• He2 does not form

Page 68: Theories of Bonding and Structure CHAPTER 10

68

2p Molecular Orbitals

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

MO Theory

Page 69: Theories of Bonding and Structure CHAPTER 10

MO Theory 2nd Row Periodic Table MO Diagrams

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

69

Li2 N2 2p Lower in energy than 2p

O2, F2 and Higher 2p Lower in energy than 2p

Can ignore filled 1s bonding & antibonding and focus on valence electrons

Page 70: Theories of Bonding and Structure CHAPTER 10

70

MO Theory MO Diagram for Li2

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

2p Lower in Energy than 2p

LiLiLi2

Diamagnetic as no unpaired spinsBond order = (2 – 0)/2

= 1

Page 71: Theories of Bonding and Structure CHAPTER 10

71

MO Theory MO Energy Diagram for F2

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

F electron configuration = [He]2s22p5 Bond order = (8 – 6)/2

= 1

F – F single bond stable molecule

Diamagnetic as no unpaired spins

FFF2

2p Lower in Energy than 2p

Page 72: Theories of Bonding and Structure CHAPTER 10

72

MO Theory Heteronuclear Diatomic Molecules

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• If Li through N 2p below 2p • If O, F and higher atomic number, then 2p below 2p Example

– BC both are to left of N • so 2p below 2p

– OF both are to right of N • so 2p below 2p

– What about NF?• Each one away from O so average is O and 2p below 2p

Page 73: Theories of Bonding and Structure CHAPTER 10

73

MO Theory B-C and N-F

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

2p lower 2p lower

BC NFNumber of valence e = 3 + 4 = 7 Number of valence e = 5 + 7 = 12

Bond Order = (5 – 2)/2 = 1.5 Bond Order = (8 – 4)/2 = 2

Page 74: Theories of Bonding and Structure CHAPTER 10

74

MO Theory N-O

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Bond Order for NO tricky• N predicts 2p lower

• O predicts 2p lower• Have to look at experiment • Shows that 2p is lower

2p lower

Number of valence e = 5 + 6 = 11

Bond Order = (8 – 3)/2 = 2.5

Page 75: Theories of Bonding and Structure CHAPTER 10

75

MO Theory N-O+ and N-O–

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

NO+ NO• Same diagram• Different number

of e–

• NO+ has 11 – 1 = 10 valence e

Bond order = (8 – 2)/2 = 3

• NO has11 + 1 = 12 valence e

Bond order = (8 – 4)/2 = 2

Page 76: Theories of Bonding and Structure CHAPTER 10

76

MO Theory Relative Stability of N-O, N-O+ and N-O–

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Recall that as bond order increases, bond length decreases, and bond energy increases

Molecule or ion

Bond Order

Bond Length (pm)

Bond Energy (kJ/mol)

NO+ 3 106 1025

NO 2.5 115 630

NO 2 130 400

So NO+ is most stable form Highest bond order, shortest and strongest bond

Page 77: Theories of Bonding and Structure CHAPTER 10

77

ProblemSet C

6. What is the MO Energy Diagram for B2? How many unpaired electrons does B2 have?

7. What is the bond order & number of unpaired electrons in

8. Draw the MO Energy Diagram for BN.

Page 78: Theories of Bonding and Structure CHAPTER 10

78

Bonding VB vs MO Theory

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Neither VB or MO theory is entirely correct– Neither explains all aspects of bonding– Each has its strengths and weaknesses

• MO theory correctly predicts unpaired electrons in O2 while Lewis structures do not

• MO theory is a difficult because even simple molecules have complex energy level diagrams

• MO theory is a difficult because molecules with three or more atoms require extensive calculations

Page 79: Theories of Bonding and Structure CHAPTER 10

79

Bonding VB vs MO Theory

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Successes of VB Theory• Based on simple Lewis structures and related geometric figures• Three dimensional structures based on electron domains without massive

calculations• Simple hybrid orbitals invoked where experimental evidence shows the need• Integer bond orders are often correct

Successes of MO Theory• MO theory is particularly successful in explaining paramagnetism of B2 and O2

– One electron each in 2px and 2py (for B2)

– One electron each in *2px and *2py (for O2)

Page 80: Theories of Bonding and Structure CHAPTER 10

80

Resonance VB Theory Treatment of Resonance

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Formate anion, HCOO–

• C has three electron domains (all bonding pairs) so – sp2 hybridized; trigonal planar

• Each O has three electron domains (one bonding pair and two lone pairs) – so sp2 hybridized; trigonal planar

Page 81: Theories of Bonding and Structure CHAPTER 10

81

Resonance VB Theory Treatment of Resonance

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Have two resonance structures• Have lone pair on each O atom in unhybridized p

orbitals as well as empty p orbital on C• Lewis theory says

– Lone pair on one O – Use lone pair of other O to form (pi) bond– Must have two Lewis structures

Page 82: Theories of Bonding and Structure CHAPTER 10

82

Resonance MO Theory Treatment of Resonance

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

Bonding MO delocalized over all three atoms

This is also our resonance hybrid picture This is the best view of what actually occurs and can be

obtained from both VB and MO theory

Page 83: Theories of Bonding and Structure CHAPTER 10

83

Resonance MO / VB Theory Treatment of Resonance:Benzene

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Six C atoms, each sp2 hybridized (3 bonds)• Each C also have one unhybridized p orbital (6 total)• So six MOs, 3 bonding and three antibonding• So three bonds

Page 84: Theories of Bonding and Structure CHAPTER 10

84

Resonance MO / VB Theory Treatment of Resonance: Benzene

Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E

• Can write benzene as two resonance structures• But actual structure is composite of these two• Electrons are delocalized • Have three pairs of electrons delocalized over six C atoms • Extra stability is resonance energy• Functionally, resonance and delocalization energy are the same

thing