Molecular shapes_MO(download)
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Molecular orbital theory
Overcoming the shortcomings of
the valence bond
Learning objectives
Describe basic principles of MO theory
Write MO diagrams for some simple
diatomic molecules
Explain optical and magnetic properties of
O2 using MO theory
Shortcomings of valence bond
The orbitals still maintain atomic identity
Bonds are limited to two atoms
Cannot accommodate the concept of
delocalized electrons – bonds covering
more than two atoms
Problems with magnetic and spectroscopic
properties
Molecular orbital theory:
wavefunctions revisited
The wave function
describes the path of the
electron – ΨA (has no real
physical meaning)
Wave functions have
phase – indicated by “+”
and “-”
Approach of atoms causes
overlap of orbitals
+ adds to + (constructive
interference); + subtracts
from – (destructive
interference)
Wavefunctions and electron density
Ψ describes the electron path
Ψ2 describes the electron density
Molecular wavefunction ΨA + ΨB
Joint density is (ΨA + ΨB)2 = ΨA2 + ΨB2 +
2ΨAΨB
In molecular orbital the density is greater
between the nuclei by an amount 2ΨAΨB
Molecular orbital theory: bonding
and antibonding
Bonding orbital: additive
combination of atomic
orbitals
Antibonding orbital:
subtractive combination of
atomic orbitals
In antibonding orbital there
is no density between the
atoms
The antibonding orbitals
are at higher energy
MO energy level diagrams:
H2 exists but He2 does not
In H2 two electrons are
paired in the bonding σ
MO, and the antibonding
σ* MO is vacant.
Total number of bonds = 1
Configuration (σ1s)2
In He2 four electrons are
paired, two in the bonding
and two in the antibonding
σ*
Total number of bonds = 0
Configuration (σ1s)2(σ*1s)2
Bond order
Bond order = ½(no. bonding electrons – no.
antibonding electrons)
Bond order 1 = single bond
Bond order 2 = double bond
Bond order 3 = triple bond
Second row elements
Li2 contains 6
electrons
Bonding σ orbitals
between 1s and 2s
Antibonding σ* orbitals
between 1s and 2s
Occupied: σ1s,σ2s, and
σ*1s
Bond order = 2 – 1 = 1
Does Be2 exist?
Formation of π orbitals in MO
Defining the
internuclear axis as z
Overlap of the pz
orbitals produces σ
bond
Overlap of px and py
orbitals produces π
bonds
General energy level diagram for
second-row homonuclear diatomics
Assumes no interaction
between the 2s and 2p orbitals
2s orbitals are lower in energy
than the 2p orbitals. The σ2s
and σ*2s orbitals are lower than
the σ2p orbital
Overlap of the 2pz is greater
than that of the 2px or 2py so σ2p
is lower than the π2p orbital
The π2p and π*2p are
degenerate (2 orbitals with the
same energy)
2s - 2p interactions affect energy
levels
The 2s and 2p orbitals
do interact
σ2s and σ2p orbitals
move further apart in
energy
Strength of interaction
changes with atomic
number
Case A: σ2p < π2p
Case B: σ2p > π2p
Filling the orbitals: the second row
diatomics
B2, C2, and N2 are case B
O2, F2 and Ne2 are case A
Note bond order from MO theory matches what we
obtain from Lewis dot diagrams
MO theory and magnetism
Paramagnetism: substance is attracted by a magnetic field
Diamagnetism: substance is repelled by a magnetic field
Paramagnetic effect is much greater than diamagnetic effect
Diamagnetic substances have no unpaired electrons
Paramagnetic substances have unpaired electrons
Magnetic properties of O2 expose
limitations of Lewis
MO theory gives two degenerate π and π* orbitals
In O2, Hund’s rule states that these are singly
occupied
O2 is paramagnetic
O
O
Correlate magnetic properties with
MO diagram
Heteronuclear molecules and NO
NO contains 11 electrons implies high reactivity
Two possible Lewis structures
0
N
0
O
-1
N
+
1
O
Lewis structure favours unpaired electron on N
Experimental bond order appears greater than 2
MO description of NO
AOs of more electronegative
atom are lower in energy
The bonding orbitals have more
of the more electronegative
atom character
The antibonding orbitals have
more of the less electronegative
atom character
MO diagram shows bond order
2.5 consistent with experiment
Unpaired electron is in π* orbital
which is more N-like (consistent
with Lewis dot structure