82
SYMMETRY AND GROUP THEORY

Symmetry and Point Group Theory

Embed Size (px)

Citation preview

Page 1: Symmetry and Point Group Theory

SYMMETRY AND GROUP THEORY

Page 2: Symmetry and Point Group Theory
Page 3: Symmetry and Point Group Theory
Page 4: Symmetry and Point Group Theory
Page 5: Symmetry and Point Group Theory
Page 6: Symmetry and Point Group Theory
Page 7: Symmetry and Point Group Theory
Page 8: Symmetry and Point Group Theory
Page 9: Symmetry and Point Group Theory

Rotation Angle Symmetry Operation

600 C6

1200 C3 (= C62)

1800 C2(= C63)

2400 C32 (= C6

4)

3000 C65

3600 E (C66)

Page 10: Symmetry and Point Group Theory
Page 11: Symmetry and Point Group Theory
Page 12: Symmetry and Point Group Theory
Page 13: Symmetry and Point Group Theory
Page 14: Symmetry and Point Group Theory
Page 15: Symmetry and Point Group Theory
Page 16: Symmetry and Point Group Theory
Page 17: Symmetry and Point Group Theory
Page 18: Symmetry and Point Group Theory
Page 19: Symmetry and Point Group Theory
Page 20: Symmetry and Point Group Theory
Page 21: Symmetry and Point Group Theory
Page 22: Symmetry and Point Group Theory
Page 23: Symmetry and Point Group Theory
Page 24: Symmetry and Point Group Theory
Page 25: Symmetry and Point Group Theory
Page 26: Symmetry and Point Group Theory
Page 27: Symmetry and Point Group Theory
Page 28: Symmetry and Point Group Theory
Page 29: Symmetry and Point Group Theory
Page 30: Symmetry and Point Group Theory
Page 31: Symmetry and Point Group Theory
Page 32: Symmetry and Point Group Theory
Page 33: Symmetry and Point Group Theory
Page 34: Symmetry and Point Group Theory
Page 35: Symmetry and Point Group Theory
Page 36: Symmetry and Point Group Theory
Page 37: Symmetry and Point Group Theory
Page 38: Symmetry and Point Group Theory
Page 39: Symmetry and Point Group Theory
Page 40: Symmetry and Point Group Theory
Page 41: Symmetry and Point Group Theory
Page 42: Symmetry and Point Group Theory
Page 43: Symmetry and Point Group Theory
Page 44: Symmetry and Point Group Theory
Page 45: Symmetry and Point Group Theory
Page 46: Symmetry and Point Group Theory
Page 47: Symmetry and Point Group Theory
Page 48: Symmetry and Point Group Theory
Page 49: Symmetry and Point Group Theory
Page 50: Symmetry and Point Group Theory
Page 51: Symmetry and Point Group Theory
Page 52: Symmetry and Point Group Theory
Page 53: Symmetry and Point Group Theory
Page 54: Symmetry and Point Group Theory
Page 55: Symmetry and Point Group Theory
Page 56: Symmetry and Point Group Theory
Page 57: Symmetry and Point Group Theory

Examples

Determine the point group where the following molecules belong:

1. Water

2. Staggered ethane

3. Eclipsed ethane

4. Trans-1,2-Dichloroethane

Page 58: Symmetry and Point Group Theory

Notes:

Page 59: Symmetry and Point Group Theory
Page 60: Symmetry and Point Group Theory
Page 61: Symmetry and Point Group Theory
Page 62: Symmetry and Point Group Theory
Page 63: Symmetry and Point Group Theory
Page 64: Symmetry and Point Group Theory
Page 65: Symmetry and Point Group Theory
Page 66: Symmetry and Point Group Theory
Page 67: Symmetry and Point Group Theory

Properties of Characters of IrreducibleRepresentations in Point Group

1. The total number of symmetry operations in the group is known as the order (h) which is the same as the total number of symmetry operations in a given point group.

Example: C2V pt group: h = 4

2. Symmetry operations are arranged in classes which is represented by the column in the character table

Example: C2V pt group: no. columns = classes=4

Page 68: Symmetry and Point Group Theory

3. The number of irreducible representations equals the number of classes (they are square)

4. The sums of the squares of the dimensions (characters under E) of each of the irreducible representations equals the order of the group.

h = [ i (E) ]2

5. For any irreducible representation, the sum ofthe squares of the characters multiplied by thenumber of operations in the class, equals theorder of the group

h = [ i (R) ]2

Page 69: Symmetry and Point Group Theory

6. Irreducible representations are orthogonalto each other. The sum of the products ofthe characters (multiplied together for eachclass) for any pair of irreduciblerepresentation is 0.

i (R) j (R) = 0, when i not equal to j

7. A totally symmetry representation isincluded in all groups, with characters of 1for all operations

Example: C2V has A1 which has allcharacters = 1

Page 70: Symmetry and Point Group Theory
Page 71: Symmetry and Point Group Theory
Page 72: Symmetry and Point Group Theory
Page 73: Symmetry and Point Group Theory
Page 74: Symmetry and Point Group Theory
Page 75: Symmetry and Point Group Theory
Page 76: Symmetry and Point Group Theory
Page 77: Symmetry and Point Group Theory
Page 78: Symmetry and Point Group Theory
Page 79: Symmetry and Point Group Theory

Examples:

Determine the Irreducible representation of the following:

1. Water molecule: = 9 -1 3 1

2. NH3 molecule: = 12 0 2

Page 80: Symmetry and Point Group Theory

Degrees of Freedom (3N)

• Translational modes

• Rotational modes

• Vibrational modes

– For linear molecule: 3N – 5

– For non-linear molecule: 3N – 6

where: N = no. of atoms

Page 81: Symmetry and Point Group Theory

Example

• Consider the irreducible representation of thewater molecule determined in the previousexample,

(a) how many vibrational mode(s) do thiscompound contain?

(b) what irreducible representation(s)represent(s) the vibrational modes of water?

Page 82: Symmetry and Point Group Theory

E N D