Chapter 10

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Chapter 10

 Molecular Geometries and Bonding

Theories

– Lewis structures do not indicate the molecular architecture – the shape of the molecule.

– The shape and structure of a molecule determines much of its physical and chemical characteristics.

VSEPR Theory

 Valence-shell

Electron Pair

Repulsion

– Electron pairs

(domains or regions) repel each other completely.

– Balloon model.

Electron Regions

1.

2.

3.

The number of electron regions around the central atom are counted as:

Each single bond counts as a region.

Each lone pair counts as a region.

A multiple bond counts as a single region.

Electron Regions

 How many?

Electron Pair Geometry (EPG)

Can be from two to six regions.

Thus, only five EPG’s are possible.

 Two regions produces a linear EPG.

Electron Pair Geometry

 Three regions produces a trigonal planar geometry.

 Planar = 2D.

 Ex) BF

3

Electron Pair Geometry

Four regions becomes a three dimensional structure based on the tetrahedron.

Formally called tetrahedral with bond angles of 109.5

o

Electron Pair Geometry

 Tetrahedral is very common and symmetrical.

 An example is CF

4

Electron Pair Geometry

 Five regions produces a trigonal bipyramidal geometry with two sets of bond angles.

Electron Pair Geometry

 An example is PCl

5

Electron Pair Geometry

 Six regions produces an octahedral geometry.

Electron Pair Geometry

 An example is SF

6

Molecular Geometry (MG)

 This is based on the shape of the electron pairs.

 When a molecule has no lone pairs, the

EPG = MG.

 If the molecules DOES have one or more lone pairs, then the shape of the atoms is determined based off of the

EPG.

Molecular Geometry

Molecular Geometry

Molecular Geometry

Examples

Bent (120), SO

2

Trigonal pyramidal, NH

3

Bent (109.5), H

2

O

Seesaw, SF

4

T-shaped, ClF

3

Linear, I

3

-

Square pyramidal, BrF

5

Square planar, XeF

4

Sketching the Molecules

 Simple = Ball and Stick figures

 Representing the 3D shapes:

– Put as many of the molecules in the same plane as possible including the central atom. Use straight lines for bonds connected to atoms in plane.

– For atoms in front of the plane, use a solid wedge.

– For atoms behind the plane, use a hashed wedge.

3D Representations

Lone Pairs

 A non-bonding pair will always take up more space.

 This compresses the normal bond angles.

Lone Pairs

Lone Pairs

 This also explains the MG’s for the trigonal bipyramidal family.

Shapes of Larger Molecules

 A molecule like acetic acid has three central atoms.

Shapes of Larger Molecules

Polarity

 A molecule can contain very polar bonds, but can be non-polar.

 An example is

CO

2

.

Polarity

 On the other hand, sometimes polar bonds DO make a molecule polar.

 An example of a polar molecule is

H

2

O.

Polarity

Polarity

 A molecule with a symmetrical distribution of polar bonds will be nonpolar.

 A molecule with an un-symmetrical distribution of polar bonds will be polar.

– presence of lone pairs

– different external atoms

Polarity

Polarity

 Polar molecules are attracted to other polar molecules

 Because water is a polar molecule, other polar molecules dissolve well in water

– and ionic compounds as well

 Non-polar molecules do

NOT dissolve in water.

Valence Bond Theory

 How can we explain the formation of the bonds in a molecular compound?

 A bond occurs when a valence orbital on one atom overlaps with a valence orbital of another atom.

Valence Bond Theory

 The H

2 molecule – a closer look.

nuclear repulsion no interaction minimum energy

Valence Bond Theory

 Three (or more) atom molecules cannot be explained by simple overlap of orbitals.

 Fact: a bond generally forms between two half-filled orbitals.

 Fact: an s-type orbital is spherical, so it could form a bond in any direction.

 Fact: the three p-type orbitals are at 90 degree angles to each other.

Valence Bond Theory

 CH

4

– has an EPG and

MG of tetrahedral with bond angles of 109.5

o .

 Valence diagram for C and H before any bonding is:

Valence Bond Theory

 Solution: promote the paired electron from the s orbital to the empty p orbital.

 Solution: mix the one s and three p orbitals together to get a new set of four orbitals all equal in energy. This is called _____________________.

Valence Bond Theory

 Each hybrid orbital has some s and some p characteristics.

 Thus, they look different!

Types of Hybrids

 Determined from the EPG.

EPG

Linear

Atomic orbitals s+p = sp

Hybrid diagram

Trigonal planar s+p+p = sp 2

Tetrahedral s+p+p+p = sp 3

Examples

BeF

2

BF

3

CH

4

Types of Hybrids

 Atoms in the third period and beyond have empty d orbitals that can potentially be used for hybridization.

 PCl

5

– requires five bonds, so need a set of five orbitals.

 Once again, must first promote the s electron to an empty d orbital.

Types of Hybrids

EPG Atomic orbitals

Trigonal bipyramidal s+p+p+p+d

= sp 3 d

Hybrid diagram

Examples

PCl

5

Octahedral s+p+p+p+d+d = sp 3 d 2

SF

6

Molecules with Lone Pairs

 Ex) NH

3

 Ex) H

2

O

 Ex) BrF

3

Multiple Bonds

Two types of bonds are possible.

1. Sigma ( s

) bonds have a cylindrical shape of electron density along the central axis between the two nuclei.

s bond

Multiple Bonds

 2. Pi ( p

) bonds have an electron density above and below the central axis.

– Are formed by the overlap of two parallel half-filled p-type orbitals.

Multiple Bonds

 The majority of bonds are sigma bonds.

 When a double bond is present, the first bond is a sigma and the second is a pi.

Pi bonds

Multiple Bonds

 For any pi bonds, you MUST use an unhybridized half-full p-type orbital.

 Ex) C

2

H

4

 Ex) CO

2

Multiple Bonds

Pi Bond Significance

 Sigma bonds have free-rotation about the central axis.

 Ex) C

2

H

4

Cl

2

 Pi bonds have NO free-rotation due to the fact that they must overlap above and below the central axis.

 Ex) C

2

H

2

Cl

2

Pi Bond Significance

Isomers

 When two compounds share the exact same formula but are different either structurally or spatially, then they are said to be isomers.

 Structural isomers

– C

5

H

12

– C

2

H

6

O

Isomers

 Geometric isomers are different spatially.

 This can occur for our carbon-carbon double bond.

X Y

C=C

Y

C=C

Y

Y X X X

Trans Cis

Isomers

 The last molecule in your packet has three possible structures. One is structural and two are geometric isomers.

 One other geometry can have cis/trans isomerism – is it tetrahedral or square planar?

 Ex) CH

2

Cl

2 or Pt(NH

3

)

2

Cl

2

?

Limitations of V.B. Theory

 Valence Bond Theory does not adequately explain molecules with resonance structures nor some other observed properties.

 Ex) O

2 or molecular oxygen is paramagnetic (unpaired electrons).

Lewis structure for O

2

Molecular Orbital Theory

 A more sophisticated and complex model of bonding.

 Atomic orbitals from each atom contribute to new MO’s.

 Like atomic orbitals, each MO can hold up to two electrons.

 A MO, though, is spread out over the entire molecule.

MO Theory

 For each atomic orbital contributed we get one MO.

 Half of the MO’s become bonding and the other half become anti-bonding.

– Waveforms add either constructively or destructively like light!

 For the n=1 period, each atom contributes a 1s atomic orbital.

MO Theory

MO Theory

MO Theory

 The Bond Order in MO theory is found by: BO = ½ (Bonding e - Anti-bonding e ).

 Any bond order = 0 implies that the molecule is not possible.

 Odd number of electrons will produce halfinteger BO’s.

MO Theory

 Period 2 elements have both the 2s and

2p atomic orbitals to contribute towards

MO’s.

 Thus, two atoms from period 2 will have how many atomic orbitals total?

 How many MO bonding orbitals will be produced? Anti-bonding?

MO Theory

 The two 2s orbitals overlap just like the

 two 1s orbitals did in period 1.

This produces the s

2s and s

2s

* MO’s.

 The six 2p orbitals overlap differently.

– Two will overlap end-on-end and produce a s

2p type MO.

– Four will overlap sideways and produce two p MO’s that are equal in energy.

MO Theory

 The energy level diagram produced for all of these new

MO’s is:

MO Theory

 Diagram assumes that no 2s-2p orbitals interactions occur.

 For B s

2p

2

, C

2 and p

2p

, and N

2 the interactions cause the order to trade places on the diagram.

 Since these are filled for O

2

, F

2

, and Ne

2 the diagram can be written with those two always reversed to simplify.

MO Theory

MO Theory

It is possible for some molecules and ions to be paramagnetic – one or more unpaired electrons.

Most will be diamagnetic – all paired electrons.

n=2 Diatomic Molecules

n=2 Diatomic Molecules

Molecular Oxygen

 According to MO theory, it has a BO = 2 and it is paramagnetic!

 As liquid O

2 is poured between the poles of a magnetic, it will have a strong attraction.

 Clip.

Heteronuclear Diatomics

 For period 2, we can mix and match other elements and apply the same MO diagram.

 Simply add up the total valence electrons that each contribute and place in the diagram.

 For ions, a positive charge means we would decrease by one electron and a negative charge means we would increase by one electron.

Heteronuclear Diatomics

 More electronegative element has lower energy orbitals.

 Can produce bond orders with ½ values.

 B.O. = ___________

Polyatomic Molecules

 When many atoms are combined together, the atomic orbitals of all the atoms are combined to make a set of molecular orbitals, which are delocalized over the entire molecule

 Gives results that better match real molecule properties than either Lewis or valence bond theories

 This is why resonance structures cannot be explained by valence bond theory.

Ozone, O

3

 The structure of O

3 includes two resonances.

M.O. showing delocalized pi bonds

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