1 + s 12 1 e 1 = 1 = c 1 1 + c 1 2 1 - s 12 1 e 2 = - 2 = c 1 1 - c 1 2 bonding antibonding

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1 + S 12 1 E 1 = 1 = c 1 1 + c 1 2 1 - S 12 1 E 2 = - 2 = c 1 1 - c 1 2 bonding antibonding

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DESCRIPTION

Ethylene  system of ethylene

TRANSCRIPT

Page 1: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

1 + S12

1E1 =

1 = c11 + c12

1 - S12

1E2 = -

2 = c11 - c12

bonding

antibonding

Page 2: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

Let overlap term go to zeroOverlap term is non zero

Page 3: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

C CH

H H

HEthylene

system of ethylene

Page 4: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

H2 C2H4

Page 5: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

antibondingempty orbital

bondingfille with 2 e-

Page 6: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

Now let us look at a more complicated system.

Three Orbitals!

H

H

H H

H

H

H

HH

H

Allyl anion

Page 7: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

1 23 How do we calculate

the energies and coefficientsof the MO’s?

We are going to use the LCAOapproximation to make threeMO’s.

Use Symmetry!

The ends are the same so they must contibuteequally to any MO. So we can make linear combinationswhere atoms one and three contribute equally.1 = pz1 + pz3 2 = pz1 - pz3

3 = pz2 The second carbon is unique.

Page 8: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

pza Ĥ pza = E = = 0Coulomb integral

pza Ĥ pzb = Eint = Interaction integral

Only if the two p orbitals are adjacentotherwise Interaction is 0.

pza pza = 1normalized

pza pzb = 0assume overlap = 0

Huckel Approximation

Page 9: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

1 23 How do we calculate

the energies and coefficientsof the MO’s?

We are going to use the LCAOapproximation to make threeMO’s.

Use Symmetry!

The ends are the same so they must contibuteequally to any MO. So we can make linear combinationswhere atoms one and three contribute equally.1 = pz1 + pz3 2 = pz1 - pz3

3 = pz2 The second carbon is unique.

Page 10: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

1 23

1 = pz1 + pz3

We need to normalizeour LCAOs 1

2 = 1

N2(pz1 + pz3 ) (pz1 + pz3 ) = 1

N2 (pz12

+ 2pz3 pz1 + pz32

) = 1 1 + 2 x 0 + 1

N2 x 2 = 1 So N = 12

Page 11: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

1 23 How do we calculate

the energies and coefficientsof the MO’s?

We are going to use the LCAOapproximation to make threeMO’s.

Use Symmetry!

The ends are the same so they must contibuteequally to any MO. So we can make linear combinationswhere atoms one and three contribute equally.

1 = (pz1 + pz3 ) 2 = ( pz1 - pz3 )

3 = pz2 The second carbon is unique.

12

12

Page 12: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

1 = (pz1 + pz3 )

2 = ( pz1 - pz3 )

3 = pz2

12

12

1 23

Same Symmetry

1 23

1 23

1 32

1 2 3

Page 13: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

1 = (pz1 + pz3 ) 3 = pz2

12

1 3

1 23

1 23-

1 3

1 23

1 23+ Bonding MO

Antibonding MO

Page 14: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

1 = (pz1 + pz3 )

3 = pz2

12

(pz1 + pz3 ) Ĥ pz2 = 12 21

2 = 2

1 23

3

+

Energy =

2

1 23

1

12

Page 15: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

1 = (pz1 + pz3 )

-3 = -pz2

12

(pz1 + pz3 ) Ĥ (- pz2) = 12 - 21

2 = - 2

Energy =

2 -

1 23

3

-1 2

3

1

12

Page 16: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

1 23

3

+

Energy =

1 23

1

12

1 23

2

Bonding

Page 17: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

1 23

3

-

Energy =

1 23

1

12

2

2 -1 3

Antibonding

Page 18: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

1 23

What about 2 ?

Thereis no overlapbetween ends so

E = 0

Page 19: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

1 3

1 23

1 23

2 -

2

0

H

H

HH

H

H

H

H H

H

Page 20: 1 + S 12 1 E 1 =   1 = c 1  1 + c 1  2 1 - S 12 1 E 2 = -   2 = c 1  1 - c 1  2 bonding antibonding

This is painful!

It makes the brain hurt.

So use a computer instead.

Simple Huckel MolecularOrbital Theory Calculator