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2 .
.
y
+
+
+
+
1
.
.
x
+
+
4
3
φ 1
_
+
+
+
_
_
_
+
φ 3 ~ y
φ 2 ~ x
_
_
+
+
_
+
φ 4
Figure 7.4 Coordinate system and H
uckel MOs for cyclobutadiene
With reference to the coordinate system of Figure 7.4, we first
choose c 4 ¼ c 1 as additional arbitrary constraint. We then immedi-
ately obtain
1
2 ðx 1 x 2 x 3 þx 4 Þ/ x
f 2 ¼ f 2x ¼
ð 7
:
80 Þ
a function having the same transformation properties as the
x-coordinate (left diagram in the second row of Figure 7.4). yz is a
nodal plane for this MO. Next, we choose c 4 ¼ c 1 as additional
arbitrary constraint, therefore obtaining
1
2 ðx 1 þx 2 x 3 x 4 Þ/ y
f 3 ¼ f 2y ¼
ð 7
:
81 Þ
a function having the same transformation properties as the y-co-
ordinate (right diagram in the second row of Figure 7.4). zx is now a
nodal plane for this MO.
f 2y are the pair of HOMOs
belonging to the doubly degenerate energy level
f 2x and
«
¼ «
;
which
2
3
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