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Figure 6.14 The simplest reaction scheme for exogenous ligand binding to a
haemoglobin exhibiting endogenous hexacoordination. The axial ligands to the iron
in the starting material, Hb(6c), are the proximal histidine and X (e.g. Tyr B10 in CtrHb
or His E10 in Synechococcus 7002 GlbN). The pentacoordinate state with free distal site is
represented with Hb(5c). L represents an exogenous ligand (e.g. O 2 ). The rate constants
are k X (s 1 ) for the dissociation of X, k þX (s 1 ) for its association, k þL (M 1 s 1 ) for the
binding of L, and k L (s 1 ) for its dissociation. Equilibrium constants are K X ¼k þX /k X for
the association of X and K L ¼
k þL /k L for the association of L.
histidine in order to bind an exogenous ligand. This additional step in the
binding process renders the evaluation of affinities and rate constants partic-
ularly complex. The simplest overall reaction is represented with two equi-
libria as in Fig. 6.14 .
Depending on the relative values of the rate constants and the concen-
tration of ligand L, certain simplifications can be made to the equation rep-
resenting the observed changes in concentrations with time, and different
kinetic regimes can be distinguished. Two common assumptions are that
the dissociation of L is very slow (except of course when flashed off ),
and that L is in excess so that its concentration remains practically constant
throughout the course of the experiment ( Hargrove, 2000 ). Under those
conditions, the second step is considered irreversible ( k L
0) and the prod-
k 0 þ L is a pseudo first-order rate constant. Solving the set of
differential equations yields three eigenvalues, l 1 , l 2 and l 3 . The first two are
given by
uct k þ L
[L]
¼
q
k X þ
1
2
2
k 0 þ L
l 1 , 2 ¼
k X þ
k þ X þ
ð
k þ X þ
k 0 þ L
Þ
4 k X k 0 þ L
and the third,
3 , is 0 by conservation of mass ( Beard & Qian, 2008 ). For
example, if k þ X and k X k 0 þ L , the kinetics present a slow phase
corresponding to the product of k 0 þ L by the rapid equilibrium fraction of
Hb(5c). Additional complexity is introduced when the pseudo first-order
approximation does not hold, and all scenarios are possible, depending on
the protein and the chosen conditions for the experiment. Within the
pseudo first-order regime and if the solution conditions (i.e. temperature,
l
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