<<

Chem 104A, UC, Berkeley

Molecular Orbital

Reading: DeKock and Gray, Chap 4 (but not 4-8) Chap 5 (through 5-8)

Miessler and Tarr, Chap 5

Chem 104A, UC, Berkeley

1 Chem 104A, UC, Berkeley Linear Combination of Atomic Orbitals (LCAO)

 k  c11  c22 .... cnn

1. n atomic orbitals  n molecular orbitals.

2. Like atomic orbitals, MOs are ortho-normal   dv 1...(i  j)  i j   dv  0...(i  j)  i j

Chem 104A, UC, Berkeley

2 Chem 104A, UC, Berkeley

* *  ( u )  N (1sA 1sB ) b b  ( g )  N (1sA 1sB )

[ ( b )]2dv  [N b (1s 1s )]2 dv 1  g  A B (N b )2[ (1s )2 dv  2 (1s )(1s )dv  (1s )2 dv] 1  A  A B  B

1 SAB 1 1 N b   2  2S AB Overlap integral

* 1 Degree of spatial overlap between any two AOs N   From different in a molecule. 2  2S AB

Chem 104A, UC, Berkeley

Gerade and Ungerade MO symmetry

1s 1s 1s 1s    a b  b a   2(1 Sab ) 2(1 Sab ) a, b, exchange position, MO does not change, inversion Even parity, Gerade: German word for “even”.

1s 1s 1s 1s    a b  b a    2(1 Sab ) 2(1 Sab )

a, b, exchange position, MO does change, no inversion odd parity, ungerade: German word for “odd”.

3 Chem 104A, UC, Berkeley

The energy of these two orbitals are obtained by applying Schrodinger Equation

Orbital Interaction Diagram 1. Always draw axis

2. Fill in using Aufbau principle

Chem 104A, UC, Berkeley

* N*=1.4 *   u

-13.6 eV b Nb=0.53 * b >   b  g

4 Chem 104A, UC, Berkeley

= ½ (#bonding e-s - #antibonding e-s) •Bond order = 0 indicates the species will not exist.

Chem 104A, UC, Berkeley Photoelectron Spectroscopy M  h  M   e

hv electron

Photoelectric effect (Einstein) 1 h  IE  mv2 M 2 e

5 Chem 104A, UC, Berkeley

PES instruments consist of an X-ray or UV source, an energy analyzer for the photoelectrons, and an electron detector.

Chem 104A, UC, Berkeley Computer System Hemispherical Energy Analyzer

Outer Sphere Magnetic Shield

Analyzer Control Inner Sphere

Multi-Channel Plate Electron Lenses for Energy Multiplier Adjustment Optics (Retardation) Resistive Anode X-ray Encoder Source

Lenses for Analysis Position Address Area Definition Converter Position Sensitive Detector (PSD)

Sample 54.7

6 Chem 104A, UC, Berkeley

13.6 eV H

Electron emitted 1 2200cm H2 15.45 eV

24.59 eV He

12 16 20 IE(eV) 24

Chem 104A, UC, Berkeley

Koopman’s Theorem

IE (n) = - En

The of electron n is equal to the negative of its Orbital energy.

We can obtain orbital energies via PES!

7 Chem 104A, UC, Berkeley

N*=1.4 * *   u

-13.6 eV b Nb=0.53

b  g

Chem 104A, UC, Berkeley

1 k   2 

Quantum Harmonic Oscillator

8 Chem 104A, UC, Berkeley

Energy  H 2 1 Ev  (n  )hv Probability distribution 2 Of the vibrational   H 2  hv  H 2  e b 2 b 1  ( g )  hv  ( g )  e

H2

Internuclear Distance

Ground state molecule is typically in its lowest vibrational state. + Upon ionization, H2 could be in a vibrational excited state.

 Chem 104A, UC, Berkeley H 2 Energy Vibrational Probability Distribution:

For n=0: largest at equil. Distance

For higher levels: 2 H Largest at the extreme of compression & expansion (KE=0)

Internuclear Distance

9 Chem 104A, UC, Berkeley

Wave functions, allowed energies, and corresponding probability densities for the harmonic oscillator

Chem 104A, UC, Berkeley Energy  H 2 n  0  n,  0

, n  0 Adiabatic ionization

H2 n  0

Internuclear Distance

10 Chem 104A, UC,Vertical Berkeley Energy  ionization H 2

Adiabatic ionization

H2 Relative Intensity

overlap of vibrational Wave function Internuclear Distance

Chem 104A, UC, Berkeley Vertical Energy  ionization H 2

2200cm1 Adiabatic ionization

H2 1 k   2 

Internuclear Distance Removing electron from bonding MO

11 Chem 104A, UC, Berkeley

13.6 eV H

Electron emitted 1 2200cm H2 15.45 eV

24.59 eV He

12 16 20 IE(eV) 24

Chem 104A, UC, Berkeley Vertical Energy ionization

Adiabatic ionization

Internuclear Distance Removing electron from antibonding MO

12 Chem 104A, UC, Berkeley

Energy

Adiabatic ionization

Internuclear Distance Removing electron from nonbonding MO

Chem 104A, UC, Berkeley

* *  ( u )  N (1sA 1sB ) b b  ( g )  N (1sA 1sB ) 1 N b   2  2S AB 1 N *   2  2S AB Overlap integral Degree of spatial overlap between any two AOs From different atoms in a molecule.

Degree of AO interaction is closely related to their overlap

Functions of distance, symmetry.

13 Chem 104A, UC, Berkeley

SAB >0, bonding interaction, E stabilized

  

Chem 104A, UC, Berkeley

SAB <0, antibonding interaction, E destabilized

 *  *  *

SAB =0, nonbonding, no orbital interaction.

14 Chem 104A, UC, Berkeley

Chem 104A, UC, Berkeley

15