Title: Covalent Bonding
1Chapter 3
2History of Bonding Theories
- Gilbert N. Lewis (1875-1946)
3Lewis Shortcoming
- O2 has been experimentally determined to possess
a double bond plus two unpaired electrons
(paramagnetic) - Electron dot diagrams cannnot be drawn to satisfy
BOTH of these criteria
4Molecular Orbital (MO) Theory
- the study of the resulting molecular orbitals
from the overlap of atomic orbitals - In covalent molecules, it is called the linear
combination of atomic orbitals (LCAO theory)
5MO Theory
- Electrons placed in bonding orbitals create a
more stable energy
6MO Theory
- For orbitals to overlap, the signs on the
overlapping lobes must be the same
7MO Theory
- Whenever two atomic orbitals mix, two molecular
orbitals are formed. The bonding orbital is
always lower in energy
8MO Theory
- For significant mixing to occur, the atomic
orbitals must be of similar energy
9MO Theory
- Each molecular orbital can hold a maximum of two
electrons, one with spin ½ , the other ½
10MO Theory
- The electron configuration of a molecule can be
constructed by using the Aufbau principle by
filling the lowest energy molecular orbitals in
sequence. - Li2 ?1s2 ?1s2 ?2s2
11MO Theory
- When electrons are placed in different molecular
orbitals of equal energy, the parallel
arrangement (Hunds Rule) will have the lowest
energy
12MO Theory
- The bond order in a diatomic molecule is defined
as the number of bonding electrons minus the
number of antibonding electrons divided by two.
13First Row Diatomic MOs
14First Row Diatomic MOs
15First Row Diatomic MOs
16First Row Diatomic MOs
17Second Row Diatomic MOs
- Due to increased Zeff, the 1s orbitals are pulled
closer to the nucleus and are not involved in
bonding. - The 2s and 2p are involved in bonding and are
called frontier orbitals.
18Second Row Diatomic MOs
Li2 (?1s)2(?1s)2(?2s)2 Be2
(?1s)2(?1s)2(?2s)2 (?2s)2
19Mixing of p Orbitals
- End on end and side to side mixing
20MO Configurations of Mixing of p Orbitals
21Second Row Diatomics
22Heteronuclear Diatomics
- Different atomic orbitals will have different
energies - the higher the Zeff, the lower the atomic orbital
energy
23Heteronuclear Diatomics
- CO
- The s orbital on the oxygen atom is too low in
energy to interact with the s orbital on the
carbon atom, so a non-bonding orbital is formed
24Heteronuclear Diatomics
- CO
- Due to the rotation axis, only the pz orbital on
the oxygen atom has the appropriate symmetry to
interact with the s orbital on carbon
25Heteronuclear Diatomics
- CO
- The px and py orbitals on both carbon and oxygen
are of the correct orientation to interact
26Heteronuclear Diatomics
- CO
- The pz orbital is left unused on the carbon atom
which remains as a nonbonding orbital
27Heteronuclear Diatomics
- CO
- Bond order is correctly predicted as 3 (6
bonding electrons 0 antibonding electrons)/2
28Heteronuclear Diatomics
29Lewis Theory
- Most simplistic view of bonding
- Useful for deducing molecular shape
- Octet rule
30Lewis Theory
- 4 rules to constructing electron-dot diagrams
- identify the central atom (lower
electronegativity), place the symbols of the
other atoms around the central atom - NF3
31Lewis Theory
- 4 rules to constructing electron-dot diagrams
- count the total number of valence electrons
- NF3
- N He2s22p3 5 valence electrons
- F He2s22p5 7 valence electrons each
- 5 (3x7) 26 total valence electrons
32Lewis Theory
- 4 rules to constructing electron-dot diagrams
- place an electron pair between the central atom
and each of the surrounding atoms, add lone pairs
to the surrounding atoms - 26 total valence electrons
33Lewis Theory
- 4 rules to constructing electron-dot diagrams
- If the number of electrons on the central atom is
less than 8, and there are left-over electrons,
add lone pairs to the central atom. If there are
no more electrons, use lone pairs from
surrounding atoms - 26 total valence electrons
34Exceptions to the Octet Rule
- Rule is only generally applicable to Period 2
elements - boron only has six, hydrogen only two
- many elements have more than eight
35Partial Bond Order
36Partial Bond Order
37Formal Charge
1.
2.
3.
- To find formal charge, divide the bonding
electrons equally among the atoms, subtract the
resulting electrons from the original number of
valence electrons - For 1, N (5-6) -1, N (5-4) 1, O (6-6) 0
- For 2, N (5-5) 0, N (5-4) 1, O (6-7) -1
- For 3, N (5-7) -2, N (5-4) 1. O (6-5) 1
38Formal Charge
-1 1 0
0 1 -1
-2 1 1
- The lowest energy structure will have the
smallest formal charges on the atoms - Resulting bond order of NN of 2 ½ and NO of 1
½
39VSEPR Theory
- Valence shell electrons will be located as far
from each other as possible - good for deducing molecular shape but not much
else - concerned with electron groupings around the
central atom - single, double, and triple bonds are all
considered one grouping
40VSEPR Theory
- Linear geometry
- two electron groups, no lone pairs
- 180 bond angles
41VSEPR Theory
- Trigonal planar geometry
- three electron groups, no lone pairs
- 120 bond angles
42VSEPR Theory
- Bent (V-shaped or angular) geometry
- three electron groups, one lone pair
- 120 bond angles (many deviations)
43VSEPR Theory
- Tetrahedral geometry
- four electron groups, no lone pairs
- 109.5 bond angles
44VSEPR Theory
- Trigonal pyramidal geometry
- four electron groups, one lone pair
- 109.5 bond angles (many deviations)
45VSEPR Theory
- Bent (V-shaped or angular) geometry
- four electron groups, two lone pairs
- 109.5 bond angles (many deviations)
46VSEPR Theory
- Trigonal bipyramidal geometry
- five electron groups, no lone pairs
- 120 equatorial bond angles
- 90 axial bond angles
47VSEPR Theory
- Seesaw geometry
- five electron groups, one lone pair
- 120 equatorial bond angles (many deviations)
- 90 axial bond angles (many deviations)
48VSEPR Theory
- T-shaped geometry
- five electron groups, two lone pairs
- 120 equatorial bond angles (many deviations)
- 90 axial bond angles (many deviations)
49VSEPR Theory
- Linear geometry
- five electron groups, three lone pairs
- 180 bond angles
50VSEPR Theory
- Octahedral geometry
- six electron groups, no lone pairs
- 90 bond angles
51VSEPR Theory
- Square-based pyramidal geometry
- six electron groups, one lone pair
- 90 bond angles (many deviations)
52VSEPR Theory
- Square planar geometry
- six electron groups, two lone pairs
- 90 bond angles
53VSEPR Theory
- Structures with seven electron groups
- pentagonal bipyramidal
- capped trigonal prismatic
- capped octahedral
54Valence-Bond Theory
- Quantum mechanical adaptation of the Lewis theory
by Pauling - Summarized in four statements
- A covalent bond results from the pairing of
unpaired electrons in neighboring atoms - The spins of the paired electrons must be
antiparallel - To provide enough unpaired electrons in each atom
for the maximum bond formation, electrons can be
excited to fill empty orbitals - The shape of the molecule results from the
directions in which the orbitals of the central
atom point
55Valence-bond Theory
- Valence-bond theory originally did not account
for certain bond angles - NH3
- should point in the x, y, and z directions
according to bonding using nitrogens px, py, and
pz orbitals (90 angles) - observed angles are 107
56Orbital Hybridization
- Wavefunctions of electrons in atomic orbitals can
mix together to form hybrid orbitals - sp, sp2, sp3, sp3d, and sp3d2 are common
hybridizations - number formed is the sum of the atomic orbitals
57Orbital Hybridization
Orbitals Orbitals Orbitals Type of Hybridization Number of Hybrid Orbitals Resulting Molecular Geometry
s p d Type of Hybridization Number of Hybrid Orbitals Resulting Molecular Geometry
1 1 0 sp 2 Linear
1 2 0 sp2 3 Trigonal Planar
1 3 0 sp3 4 Tetrahedral
1 3 1 sp3d 5 Trigonal Bipyramidal
1 3 2 sp3d2 6 Octahedral
58Orbital Hybridization
- BF3
- boron has an electron configuration of
He2s22p1, gets excited to He2s12p2 - orbitals mix to provide three sp2 hybridized
orbitals at 120 angles
59Orbital Hybridization
- CO2
- carbon has an electron configuration of
He2s22p2, gets excited to He2s12p3 - the s and one p orbital mix to provide two sp
hybridized orbitals at 180 angles - single electrons in the two remaining p orbitals
interact with a p orbital on oxygen to give a ?
bond
60Network Covalent Substances
- A crystal lattice which consists solely of
covalently bound atoms - diamond and quartz
- high melting points, hard, and insoluble
61Intermolecular Forces
- If no intermolecular forces existed, all
substances would be gases - All molecules exhibit London Dispersion Forces
- induced dipole attractions
- Other forces are dipole-dipole, ion-dipole, and
hydrogen bonding
62London (Dispersion) Forces
- Separation of charges lead to a temporary dipole
- this leads to a partial positive and negative
charge which will attract themselves between
molecules
63London (Dispersion) Forces
- Strength of the dispersion forces is related to
the number of electrons and shape - The higher the force, the higher the melting and
boiling points
64Electronegativity
- Power of an atom to attract electrons
- greater for higher Zeff
- dipoles can cancel each other out as in CO2
65Dipole-Dipole Forces
- Attractions between permanent dipoles
- Induced dipole attractions are much higher than
dipole-dipole forces
66Hydrogen Bonding
- Exceptionally strong dipole-dipole forces
- strongest intermolecular force
- similar to a weak, covalent bond