EFFECT OF CONFORMATIONAL CONSTRAINTS ON GATED ELECTRON-TRANSFER KINETICS - A MULTIFACETED STUDY ON COPPER(II I) COMPLEXES WITH CIS-CYCLOHEXANEDIYL-[14]ANES(4) AND TRANS-CYCLOHEXANEDIYL-[14]ANES(4)/
Ca. Salhi et al., EFFECT OF CONFORMATIONAL CONSTRAINTS ON GATED ELECTRON-TRANSFER KINETICS - A MULTIFACETED STUDY ON COPPER(II I) COMPLEXES WITH CIS-CYCLOHEXANEDIYL-[14]ANES(4) AND TRANS-CYCLOHEXANEDIYL-[14]ANES(4)/, Inorganic chemistry, 34(24), 1995, pp. 6053-6064
A multifaceted study has been conducted on the electron-transfer react
ions of the copper(II/I) complexes formed with 2,3-cis- and cyclohexan
ediyl-1,4,8,11-tetrathiacyclotetradecane (designated as cis- and tmns-
cyhx-[14]aneS(4)). Each system has been studied by (i) H-1-NMR line br
oadening in D2O to determine the electron self-exchange rate constants
at zero driving force, (ii) rapid-scan cyclic voltammetry in 80% meth
anol-20% water (w/w) to determine the rate constants for conformationa
l changes and heterogeneous electron transfer, and (iii) stopped-flow
spectrophotometry using a total. of eight oxidizing and reducing count
erreagents to determine the cross-reaction electron-transfer rate cons
tants from which self-exchange rate constants can be calculated for va
rious driving forces. The crystal structures of both Cu(II)L complexes
and of Cu-I(trans-cyhx-[14]aneS(4)) have also been determined. From t
he NMR measurements, the electron self-exchange rate constants have be
en evaluated [at 25 degrees C, mu = 0.10 M (NO3-)] as k(11(ex)) = (5.0
+/- 0.5) x 10(4) and less than or equal to 10(3) M(-1) s(-1) for Cd-I
I/I(cis-) and Cu-II/I(trans-cyhx-[14]aneS(4)), respectively. Applicati
on of the Marcus relationship to the numerous cross-reaction rate cons
tants yields variable behavior which is consistent with a dual-pathway
mechanism for which the following self-exchange rate constants have b
een resolved [25 degrees C, mu = 0.10 M (ClO4-)]: for Cu-II/I(cis-cyhx
-[14]aneS(4)), k(11(A)) = 5 x 10(4), k(11(B)) less than or equal to 10
M(-1) s(-1); for Cu-II/I(trans-cyhx-[14]aneS(4)), k(11(A)) = 2 x 10(3
), k(11(B)) less than or equal to 10 M(-1) s(-1). The reduction reacti
ons proceed by the most favorable pathway (pathway A) involving a meta
stable Cu(I)L intermediate (P) while the limiting oxidation reactions
proceed by an alternate pathway (pathway B) involving a less stable Cu
(II)L intermediate (Q). The change in pathway is mediated by the rate
constant (k(RP)) for the formation of the Cu(I)L(P) intermediate from
the stable Cu(I)L(R) complex. This latter rate constant has been estim
ated from both cyclic voltammetric measurements (CV, 80% methanol) and
Cu(I)L homogeneous oxidation kinetics (Ox, H2O) as follows [25 degree
s C]: for Cu-I(cis-cyhx-[14]aneS(4)), k(RP) = 4.4 x 10(2) (CV) and 1.1
x 10(2) s(-1) (Ox); for Cu-I(trans-cyhx-[14]aneS(4)), k(RP) = 1.5 x 1
0(2) (CV) and 32 s(-1) (Ox). The values obtained from homogeneous oxid
ations are believed to be the more reliable. The crystal structures re
veal that both Cu(II)L complexes are square pyramidal with the four su
lfur donor atoms occupying the basal plane and a coordinated water mol
ecule (or anion) at the apex. The Cu-I(trans-cyhx-[14]aneS(4)) complex
is in a flattened tetrahedral geometry in which all four sulfur donor
atoms remain coordinated. These structures imply that, for each Cu(II
I)L system, two sulfur donor atoms must invert during the overall elec
tron-transfer process. It is postulated that these donor atom inversio
ns may represent the primary barrier for the conformational change rep
resented in the R --> P step. The self-exchange rate constant represen
tative of the electron-transfer step itself, corrected for the separat
e conformational change step, is estimated to be on the order of 10(6)
M(-1) s(-1) for both systems, equivalent to the largest self-exchange
rate constants known for rigid Cu(II/I)L systems. Crystal data [Mo K
alpha radiation (lambda = 0.710 73 Angstrom)] are as follows. For [Cu-
II(cis-cyhx-[14]aneS(4))(H2O)](ClO4)(2) (1): CuS4C14H28Cl2O9, triclini
c system, space group P $(1) over bar$$, a = 9.734(4) Angstrom, b = 10
.155(3) Angstrom, c = 13.058(4) Angstrom, alpha = 91.73(2)degrees, bet
a = 91.52(3)degrees, gamma = 117.75(3)degrees, V = 1140.6(7) Angstrom(
3), Z = 2, R = 0.049, R(w) = 0.050, T = -110 degrees C. For [Cu-II(tra
ns-cyhx-[14]aneS(4))(H2O)](ClO4)(2) (2a): CuS4Cl4H28Cl2O9, triclinic s
ystem, space group P $(1) over bar$$, a = 9.177(5) Angstrom, b = 10.64
1(5) Angstrom, c = 13.037(4) Angstrom, alpha = 87.26(3)degrees, beta =
88.13(4)degrees, gamma = 69.19(3)degrees, V = 1188.5(8) Angstrom(3),
Z = 2, R = 0.050, R(w) = 0.056, T = -110 degrees C. For [Cu-II(trans-c
yhx-[14]aneS(4))Cl]. 1/2CuCl(4) . H2O (2b): Cu1.5C14H28S4Cl3O, orthorh
ombic system, space group Pbcn, a = 28.206(7) Angstrom, b = 10.115(3)
Angstrom, c = 14.707(2) Angstrom, V = 4196(2) Angstrom(3), Z = 8, R =
0.038, R(w) = 0.042, T = 22 degrees C. For [Cu-I(trans-cyhx-[14] aneS(
4))]ClO4 . 1/4H(2)O (3): CuS4C14H26.5ClO4.25, monoclinic system, space
group P2(1)/n, a = 10.135(2) Angstrom, b = 16.044(2) Angstrom, c = 12
.675(2) Angstrom, beta = 105.10(1)degrees, V = 1989.9(5) Angstrom(3),
Z = 4, R = 0.038, R(w) = 0.038, T = -110 degrees C.