123
APPENDIX VI
Derivation of the relaxation times for a system of coupled reactions using the Castellan’s method
Consider the reaction scheme (charges omitted)
Fe ⇄ FeOH + H (VI.1)
2 FeOH ⇄ D (VI.2)
D + FeOH ⇄ T + H (VI.3)
Following an external perturbation of the system equilibrium, reaction (VI.1) reaches the equilibrium much faster than reactions (VI.2) and (VI.3), so the
€ FeOH
[
]
Fe[ ]
= KH H[ ]
ratioremains constant for each [H] value (in excess) considered. This fact has enabled us to reduce the reaction system to the simpler form
cD 2M ⇄ D (VI.4) c-D cT D + M ⇄ T (VI.5) c-T
where [M] = [Fe] + [FeOH].
Let’s denote the exchange rates of reactions (VI.4) and (VI.5) as rD and rT, respectively.
rD = cD [M] 2 = c
-D [D] (VI.6)
rT = cT [D][M] = c-T [T] (VI.7)
According to Castellan (Castellan, 1963), the coupling coefficients of the reaction system (VI.4)-(VI.5) are defined as:
Appendix VI 124 € g11 = 4 M
[ ]
+ 1 D[ ]
(VI.8) € g12 = g21 = 2 M[ ]
− 1 D[ ]
(VI.9) € g22 = 1 M[ ]
+ 1 D[ ]
+ 1 T[ ]
(VI.10)The two relaxation times, 1/τk, of the system of coupled reaction (VI.4)-(VI.5) depend on
the equilibrium concentrations according to the determinant equation (VI.11)
€ rDg11− 1
τ
k rDg12 rTg21 rTg22− 1τ
k = 0 (VI.11)which provides the expressions for 1/τk in the form (VI.12)
€
1
τk
= TR ± TR2 − 4DET
2 (VI.12)
where TR is the trace and DET is the determinant of equation (VI.11). The k = 1 value corresponds to 1/τf (fast) and k = 2 corresponds to 1/τs (slow). Instead of considering
separately the two expressions (VI.12), we have applied the properties
(VI.13)
(VI.14)
where TR = rDg11+rTg22 and DET = rDrT(g11g22−g12g21).
Introduction of equations (VI.6)-(VI.10) into equations (VI.13) and (VI.14) yields equations (VI.15) and (VI.16)
Appendix VI 125 € 1 τf + 1 τs = 4
(
χD+χT)
[ ]
M +(
χ−D+χ−T)
(VI.15) € 1 τf × 1 τs = 6χDχT[ ]
M 2 + 4χDχ−T[ ]
M +χ−Dχ−T (VI.16)Since the concentration of the total monomer, [M] over the explored range of concentrations is much higher than that of the aggregated species, one can replace [M] by CM.
Equations (VI.15) and (VI.16) are reported in the text (equation 4.7 and 4.8 of chapter 4) with this approximation.