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Dr. S. M. Condren Chapter 4 Molecular Symmetry

Dr. S. M. Condren Chapter 4 Molecular Symmetry. Dr. S. M. Condren

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Dr. S. M. Condren

Chapter 4

Molecular Symmetry

Dr. S. M. Condren

Dr. S. M. Condren

Symmetry Elements and Symmetry Operations

• Identity

• Proper axis of rotation

• Mirror planes

• Center of symmetry

• Improper axis of rotation

Dr. S. M. Condren

Symmetry Elements and Symmetry Operations

• Identity => E

Dr. S. M. Condren

Symmetry Elements and Symmetry Operations

• Proper axis of rotation => Cn

– where n = 2, 180o rotation– n = 3, 120o rotation– n = 4, 90o rotation– n = 6, 60o rotation– n = , (1/)o rotation

• principal axis of rotation, Cn

Dr. S. M. Condren

2-Fold Axis of Rotation

Dr. S. M. Condren

3-Fold Axis of Rotation

Dr. S. M. Condren

Rotations for a Trigonal Planar Molecule

Dr. S. M. Condren

Symmetry Elements and Symmetry Operations

Mirror planes =>h => mirror plane perpendicular to a

principal axis of rotationv => mirror plane containing principal

axis of rotationd => mirror plane bisects dihedral angle made

by the principal axis of rotation and two adjacent C2 axes perpendicular to principal rotation axis

Dr. S. M. Condren

Mirrors

v v

Cl Cl

h

I d

d

Cl Cl

Dr. S. M. Condren

Rotations and Mirrors in a Bent Molecule

Dr. S. M. Condren

Benzene Ring

Dr. S. M. Condren

Symmetry Elements and Symmetry Operations

• Center of symmetry => i

Dr. S. M. Condren

Center of Inversion

Dr. S. M. Condren

Inversion vs. C2

Dr. S. M. Condren

Symmetry Elements and Symmetry Operations

• Improper axis of rotation => Sn

– rotation about n axis followed by inversion through center of symmetry

Dr. S. M. Condren

Improper Rotation in a Tetrahedral Molecule

Dr. S. M. Condren

S1 and S2 Improper Rotations

Dr. S. M. Condren

Successive C3 Rotations onTrigonal Pyramidal Molecule

Dr. S. M. Condren

Linear Molecules

Dr. S. M. Condren

Selection ofPoint Group from Shape

• first determine shape using Lewis Structure and VSEPR Theory

• next use models to determine which symmetry operations are present

• then use the flow chart Figure 3.9, Pg. 81 text to determine the point group

Dr. S. M. Condren

Dr. S. M. Condren

Decision Tree

Dr. S. M. Condren

Selection ofPoint Group from Shape

1.determine the highest axis of rotation

2.check for other non-coincident axis of rotation

3.check for mirror planes

Dr. S. M. Condren

H2O and NH3

Dr. S. M. Condren

Dr. S. M. Condren

Dr. S. M. Condren

Geometric Shapes

Dr. S. M. Condren

Orbital Symmetry, pz C2v

z E + X(E) = +1

- +

+ C2(z)

x

- + - X(C2(z)) = +1

y v(xz)

- X(v(xz)) = +1

v(yz) +

- X(v(xz)) = +1

Dr. S. M. Condren

Orbital Symmetry, py C2v

+

-

+-

-+

-

+

+-

zE

x

y

X(E) = +1

C2(z)X(C2(z)) = -1

v(xz)

X(v(xz)) = -1

X(v(xz)) = +1

v(yz)

Dr. S. M. Condren

Orbital Symmetry, px C2v

- +

- +

+ -

- +

+ -

z

x

y

EX(E) = +1

C2(z)

X(C2(z)) = -1v(xz)

v(yz)X((xz)) = +1

X(v(xz)) = -1

Dr. S. M. Condren

Water, C2v Point GroupTranslational motion in y

z

y o o

H H H H

x v(xz)

“asymmetric” => -1

Dr. S. M. Condren

Water, C2v Point GroupTranslational motion in y

z

o

y H H

x o

H H v(yz)

“symmetric” => +1

Dr. S. M. Condren

Water, C2v Point GroupTranslational motion in y

z

y C2(z)

x

O

H H

“asymmetric” = - 1

Dr. S. M. Condren

Water, C2v Point GroupTranslational motion in y

Representation:

E C2(z) v(xz) v(yz)

3 +1 -1 -1 +1

Dr. S. M. Condren

Water, C2v Point GroupRotation about z axis

z

O

Ha Hb

- movement out of plane towards observer

- movement out of plane away from observer

a,b - labeling to distinguish hydrogens before and after symmetry operations

Dr. S. M. Condren

Water, C2v Point GroupRotation about z axis

z

O E O

Ha HbHa Hb

+1

Dr. S. M. Condren

Water, C2v Point GroupRotation about z axis

z

O C2z O

Ha HbHb Ha

+1

Dr. S. M. Condren

Water, C2v Point GroupRotation about z axis

z

O v(xz) O

Ha HbHb Ha

x -1

Dr. S. M. Condren

Water, C2v Point GroupRotation about z axis

z

O v(yz) O

Ha HbHa Hb

-1

Dr. S. M. Condren

Water, C2v Point GroupRotation about z axis

Representation

E C2(z) v(xz) v(yz)

4 +1 +1 -1 -1

Dr. S. M. Condren

Water, C2v Point Group

Representations:

Rotation

E C2(z) v(xz) v(yz)

4 +1 +1 -1 -1

Dr. S. M. Condren

Water, C2v Point Group

Representation:

Translation

E C2(z) v(xz) v(yz)

1 +1 +1 +1 +1 Tz

2 +1 -1 +1 -1 Tx

3 +1 -1 -1 +1 Ty

Dr. S. M. Condren

Water, C2v Point Group

Representation:

Rotation

E C2(z) v(xz) v(yz)

4 +1 +1 -1 -1 Rz

5 +1 -1 +1 -1 Ry

6 +1 -1 -1 +1 Rx

Dr. S. M. Condren

Water, C2v Point Group

Character Table

E C2(z) v(xz) v(yz)

A1 +1 +1 +1 +1 Tz 1

A2 +1 +1 -1 -1 Rz 4

B1 +1 -1 +1 -1 Ry, Tx 2 , 5

B2 +1 -1 -1 +1 Rx,Ty 3, 6

Dr. S. M. Condren

Dr. S. M. Condren

Vibrational Modes in CO2

For linear molecules: 3N - 5 IR fundamentals

Dr. S. M. Condren

Vibrational Modes in SO2

For non-linear molecules: 3N - 6 IR fundamentals

Dr. S. M. Condren

Vibration Modes for SO3

For non-linear molecules: 3N - 6 IR fundamentals

Dr. S. M. Condren

Vibrational Modes for CH4

For non-linear molecules: 3N - 6 IR fundamentals

Dr. S. M. Condren

Vibrational Modes for [PtCl4]-2

For non-linear molecules: 3N - 6 IR fundamentals

Dr. S. M. Condren

Enantiomer Pairs

Dr. S. M. Condren

Enantiomer Pairs

Dr. S. M. Condren

Polarimeter