Chemistry Reference
In-Depth Information
The H
uckel matrix elements are:
<
¼ a p
H zh z ¼ p b s h cos
H zz
ð
:
Þ
g
2
224
:
H h z h z ¼ a h þ
2 b hh a h
8
<
H xx
¼ a p
p
p b s h sin
H yh y ¼
g
ð
2
:
225
Þ
:
H h x h x ¼ a h
b hh a h
8
<
H yy ¼ a p
p
H yh y ¼
p
b s h sin
g
ð
2
:
226
Þ
:
H h y h y ¼ a h b hh a h
uckel theory. 29
The three lowest roots of the secular equations give the H
where b hh is neglected as usual in H
uckel energy
of the 3a 1 1e x 1e y valence electron configuration of NH 3 as a function of
angle
g
:
(
E
ðgÞ¼
2 « 1
ð
A 1
Þþ
2 « 1
ð
E x
Þþ
2 « 1
ð
E y
Þ
ð
2
:
227
Þ
¼
3 a p
þ
3 a h
D
2
D
1
3
where:
<
2
1
=
2
2
1
=
2
4H zh z
12 b s h cos 2
D 1 ðgÞ¼½ða p a h Þ
þ
¼½ða p a h Þ
þ
g
>
0
:
2
1
=
2
2
1
=
2
6 b s h sin 2
4H xh x
D
ðgÞ¼½ða p
a h Þ
þ
¼½ða p
a h Þ
þ
g
>
0
3
ð
:
Þ
2
228
Taking the first
g
-derivatives of the
D
s, the stationarity condition for the
energy is:
dE
d
d
D 1
d
2 d
D 3
d
1
D
1
D
6 b s h sin 2
g ¼
g
g ¼
g
1
¼
0
ð
2
:
229
Þ
3
29 In the second of Equations (2.224) the minus sign accounts for the need of positive overlap
between the z AO of nitrogen and the symmetrical sum h z of hydrogen AOs.
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