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ferrous iron, which is some 0.6 ˚ out of the plane of the domed porphyrin ring. A second His residue, His E7 (the
distal histidine), is too far away from the iron atom to coordinate with it in the deoxy state.
A comparison of the deoxy- and oxy-haemoglobin structures reveals a number of important differences.
Whereas in the T (deoxy) state the Fe atom is out of the haem plane, on oxygenation it moves into the plane of the
now undomed porpyrin, pulling the proximal His F8 and the F-helix, to which it is attached, with it ( Figure 13.6 ),
FIGURE 13.6
The triggering mechanism for the T to R transition in haemoglobin.
as we will see shortly, thereby triggering the T to R transition. The major differences between R and T confor-
mations are at the
a 1 b 2 (and the corresponding
a 2 b 1 ) subunit interfaces which consist of the C helix of
a
-subunits. These fit to one another in two distinct conformations, which
correspond to a 6 ˚ relative shift at the interface. In the T state His FG4 is in contact with Thr C6, whereas in the
R state the same His is in contact with Thr C3, one turn further back along the C helix ( Figure 13.7 ) . Another series
of very important differences concern a network of salt bridges at subunit
-subunits and the FG interface of the
b
e
subunit interfaces which stabilize the T
state, but are broken in the more relaxed R state.
FIGURE 13.7
The a 1 b 2 interface in (a) human deoxy haemoglobin and (b) oxy-haemoglobin.
(Adapted from Voet & Voet, 2004 . )
 
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