chemistry 125: lecture 13 overlap and energy-match covalent bonding depends primarily on two...
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Chemistry 125: Lecture 13
Overlap and Energy-Match Covalent bonding depends primarily on two factors: orbital overlap and energy-match.
Overlap depends on hybridization. Bond strength depends on the number of shared
electrons. In these terms quantum mechanics shows that Coulomb’s law answers Newton’s
query about what “makes the Particles of Bodies stick together by very strong Attractions.”
Energy mismatch between the constituent orbitals weakens the influence of their overlap.
The predictions of this theory are confirmed experimentally by measuring the bond strengths
of H-H and H-F during heterolysis and homolysis.
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Overlap&
Energy-Match
Consider how theOverlap Integral
(the “sum” of A x B over all space)
depends on the Distancebetween two Carbon Atoms
and on Hybridizationof their Atomic Orbitals
2s 2s
C Overlap Scale
Diameter of node for 2sC is 0.7 Å
Sliding together to1.4Å
(~CC bond distance)
superimposesthe two 'X's
xx
2s
x
C Overlap Scale
2s
x
2s
x
2s
x
2s
x
2s
x
2s
x
2s
x
Sliding together to1.4Å
superimposesthe two 'X's
Overlap Integral = 0.41!
Guess the overlap integral, A B
(remember that A A = 1)
C Overlap
C-C Orbital Overlap (Clementi)
0.00
0.10
0.20
0.30
0.40
0.50
0.60
0.70
0.80
0.90
1.00
1.15 1.25 1.35 1.45 1.55Angstroms
Orbital Overlap Integral
1.0
0.8
0.6
0.4
0.2
0.0
Ove
rlap
Inte
gra
l
1.2 1.3 1.4 1.5 Å
s-p
2s2p
2s2p
2p
2p
+ x -
+ x +
2p
xx
s-sp-p
C C C C C C
and are“orthogonal”(net overlap = 0)
to -1 at
D = 0
to 0 at
D = 0
to 1 at
D = 0
p-p
(sigma) is Greek “s” MO analogue of s AO.
(no node through nuclei)
(pi) is Greek “p” MO analogue of p AO.
(nodal planethrough nuclei)
C-C Orbital Overlap (Clementi)
0.00
0.10
0.20
0.30
0.40
0.50
0.60
0.70
0.80
0.90
1.00
1.15 1.25 1.35 1.45 1.55Angstroms
Orbital Overlap Integral
Curiosity:Over most of this range 2s overlaps with 2p
better than either 2s with 2s or 2p with 2p
1.0
0.8
0.6
0.4
0.2
0.0
Ove
rlap
Inte
gra
l
1.2 1.3 1.4 1.5 Å
s-p
p-p
s-sp-p
sp3-sp3
s2p-s2p
C C C C C C
sp3-sp3sp2-sp2sp-sp
xx
sp2-sp2
sp-sp
C-C Orbital Overlap (Clementi)
0.00
0.10
0.20
0.30
0.40
0.50
0.60
0.70
0.80
0.90
1.00
1.15 1.25 1.35 1.45 1.55Angstroms
Orbital Overlap Integral
1.0
0.8
0.6
0.4
0.2
0.0
Ove
rlap
Inte
gra
l
1.2 1.3 1.4 1.5 Å
s-p
p-p
s-sp-p
sp3-sp3
s2p-s2p
C C C C C C
sp2-sp2
sp-sp
Hybrids overlap about twice as much as pure atomic orbitals.
sp gives best overlap, but only allows two orbitals (50% s in each)
sp3 gives four orbitals with nearly as much overlap (25% s in each)
(because they allow nearly full measure of s with p overlap plus s with s, and p with p.)
Influence of Overlapon “MO” Energy ofa One-DimensionalDouble Minimum
Case I:
Perfect Energy Match
Degenerate
EnergyRising
EnergyFallingIncreasing Overlap
No SignificantEnergy Difference
Creates Splitting
Overlap Holds Atoms Together
A B
Ele
ctro
n E
nerg
y
separate separate
1/√2 (A+B)
1/√2 (A-B)
together
<
>
with greateroverlap
Electron Count and Bond Strength
•
•
•
•
A B
Ele
ctro
n E
nerg
y
separate separatetogether
•
•
•
•# Effect1 Bonding2 Strongly Bonding3 Weakly Bonding4 Antibonding
Why Doesn’t Increasing Overlap Make MolecularPlum Puddings Collapse?
H2 He?
Electrons do become 55% more stable (~650 kcal/mole)
But proton-proton repulsion increases much more dramatically (1/r)
(already increases by 650 kcal/mole from H-H to 0.3 Å)
Unless one uses neutron “glue” D2 He fusion fuels the Sun (200 million kcal/mole)
Finally we understand
the atom-atom ….
force law! … ….
Bonding Potential
Electron pair becomes more stable
with increasing overlap.
Nuclear repulsion becomes
dominant
All from Coulomb’s Lawand
Schrödinger Kinetic Energy of Electrons
(This curve provides the potential for studying molecular vibration.)
Atom-Atom Distance
Ene
rgy
Newton Opticks (1717)
Query 31
There are therefore Agents in Nature able to make the Particles of Bodies stick together by very strong Attractions. And it is the business of experimental Philosophy to find them out.
shop
.rpg
.net
Overlap&
Energy-Match
What if partner is lower in energy than A?
A B
Ele
ctro
n E
nerg
y
separate separate
1/√2 (A+B)
1/√2 (A-B)
together
<
>
“Splitting” Overlap?B
*
*) approximately
Why use any of an“Inferior” Orbital?
The 1s “core” AOs did indeed remain pure and unmixed during creation
of molecular orbitals for CH3CHFOH :
1 1s (F)Core 1
2 1s(O)Core 2
3 1s(C1)Core 3
4 1s(C2)Core 4
Why use any of an“Inferior” Orbital?
but the valence-level AOs were heavily mixed.
The compact 1s “core”AOs did indeed remain pure and unmixed during creation
of molecular orbitals for CH3CHFOH,
5 “1s(valence)”
2s of F
2sp hybrid of O
2s of C
(aA + bB)2 = a2 A2 + b2
B2 + 2abAB
Why use any of an“Inferior” Orbital?Suppose the energy of the A orbital is much
higher (less favorable) than that of the B orbital.
Can one profit from shifting electron density towardthe internuclear AB region (from the “outside” region)
without paying too much of the high-energy“cost” of A?
Yes, because for a small amount (a) of A in the MO,the amount of A2 probability density (a2) is REALLY small,
while the amount of AB shifting (2ab) is much larger.
e.g. a = 0.03, b = 0.98 means a2 = 0.001, b2 = 0.96, 2ab = 0.06(Incidentally, this is normalized, since the integral of AB is ~0.6, and 0.6 x 0.06 is ~0.04 = 1 - 0.96)
Influence of Overlapon “MO” Energy ofa One-Dimensional Double Minimum
Case II:
Poor Energy Match
Degenerate
EnergyRising
EnergyFallingIncreasing Overlap
Splitting dueonly to
OriginalWell Offset
Fights Well Difference
Note Small Energy
Mismatch
still
Mixing non-degenerate
AOsNegligible
Mixing
StillBiased
What if partner is lower in energy than A?What are the ultimate energies?
A B
Ele
ctro
n E
nerg
y
separate separate
1/√2 (A+B)
1/√2 (A-B)
together
<
>
?C
A-C
A+C
largerenergyshifts
smallerenergyshifts
looks mostly like C inshape & energy
looks mostly like A
B
A given overlapyields this
splitting forperfect E-match
How much smaller is the bonding shift when energy is mismatched?
C
A
Ele
ctro
n E
nerg
y
separate separatetogether
Averageof A and C
Energy-mismatch
B
How much smaller is the bonding shift when energy is mismatched?
C
A
Ele
ctro
n E
nerg
y
separate separatetogether
With E-mismatch larger splitting
for same overlapA given overlap
yields thissplitting for
perfect E-match Energy-mismatch
B
How much smaller is the bonding shift when energy is mismatched?
C
A-C
A+C
A
Ele
ctro
n E
nerg
y
separate separatetogether
(shift up a bit for >,< normalization)Splitting is less
sensitive to lesser contributor of
mismatch / overlap
For a given overlap,bonding shift is reduced
by energy mismatch.(Still A+C ends lower than
A+B, because C starts lower.)
e.g. when mismatch is relatively large, a given
amount of overlap doesn’t make much
difference
Important Generalizations
Mixing two overlapping orbitals gives one composite orbital that is lower in energy than either parent
and one that is higher in energy than either parent.
The lower-energy combination looks more like the lower-energy parent,
both in shape and in energy (ditto for higher-).
For a given overlap, increasing energy mismatch decreases the amount of mixing and
decreases the magnitude of energy shifts.
Which Bond is Stronger A-B or A-C?
A B
Ele
ctro
n E
nerg
y
separate separate
C
Compared to What?
••
••
••
••
A-B stronger if forming Ions (A+ B-)
together
A-C electrons clearly lower in energy,but…
Which Bond is Stronger A-B or A-C?
A B
Ele
ctro
n E
nerg
y
separate separate
C
Compared to What?
••
••
A-B stronger if forming Ions (A+ B-)
••
A-C stronger if forming Atoms (A C)• •
together
mismatch aids Heterolysis
mismatch hinders Homolysis
•
Experimental Evidence
Is All This True?
H-H vs. H-F
*
Homolysis to A• •Bkcal/mole
136104 HF Bondis Stronger
Heterolysis to A+ B-
kcal/mole (gas phase)
400 373HF Bondis Weaker
BigonF
BigonH
"Hydrofluoric Acid "
antibondingmolecular orbital
:
empty
(match) (mismatch)
Hybridization Reality Check:
Structure and Dynamics of
XH3BH3 CH3 NH3
End of Lecture 13Oct. 3, 2008
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