Pressure Dependence of Peroxynitrite Reactions
Inorganic Chemistry, Vol. 40, No. 3, 2001 531
however, one can show46 from measured kD/kN and k-C/kN
47
Table 1. Experimentally Determined Volumes of Activation
∆Vq
∆(∆Vq)b,c
rate-constant ratios that the decomposition rate should be
insensitive to the medium viscosity;48 hence, the observed
insensitivity to viscosity is consistent with a radical mechanism
(for ONOOH). Using EPR spectroscopy, Augusto and co-
obs
b
reactant
pHa
(cm3 mol-1
)
(cm3 mol-1
)
ONOOH
ONOOH
4.5
4.5
4.5
7.2
7.2
7.2
7.2
+6
+14d
+12
+10
+11
-7
•-
4-
4-
workers have measured the formation of the CO3 radical in
ONOOH + Fe(CN)6
+13
+14
+16
∼0
- 49,50
ONOOH + Fe(CN)6
near-quantitative yield from ONOOCO2
,
based upon
4-
ONOOH + Mo(CN)8
limiting oxidation yields for its “indirect” reactions.49 Earlier
research in our13 and Goldstein and Czapski’s51 laboratories has
established that the reactive form of the adduct has chemical
properties and reactivity characteristics consistent with those
of the CO3•- + NO2• radicals, and Goldstein and Czapski have
also shown that product yields from “indirect” one-electron
oxidations by ONOOCO2- decreased markedly with increasing
medium viscosity; this is consistent (in this case) with a radical
mechanism.52 Finally, Lehnig has observed chemically induced
dynamic nuclear polarization (CIDNP) in the 15N NMR
ONOOH + Ni(cyclam)2+
ONOOCO2- + Fe(CN)6
-22
+18
4-
a In 0.15 M phosphate; other conditions for individual reactions as
listed in the text. b Error limits are (10-15%. c Defined as ∆Vq
-
D
∆Vq (Scheme 2). d Contained 5.0 mM added NO3
.
-
N
during cage escape than during internal rearrangement. This
result suggests that solvent restructuring constitutes a substantive
energetic barrier to separation of the radical pair; although
reasonable, this conclusion is not in accord with the frequently
invoked assumption that, since the viscosity of water is nearly
constant over this pressure range, kD will be pressure indepen-
dent. This behavior markedly contrasts that of the direct
bimolecular reaction between ONOOH and Ni(cyclam)2+, the
product yield for which is near stoichiometric and pressure
independent, i.e., ∆(∆Vq) = O (Table 1).
spectrum of NO3 during decomposition of O15NOOH and
-
O15NOOCO2-, which can be interpreted as indicating for-
mation of 15NO3 within the radical pairs {NO2 ,OH•} and
-
•
{NO2 ,CO3•-}.53 Thus, it seems appropriate to discuss the
•
pressure dependencies of the reactions of ONOOH and
ONOOCO2- within the context of the radical pair mechanisms,
i.e., Scheme 2. (Note that the rate-limiting step for the
ONOOCO2- reactions is adduct formation, whereas protonation
is a pre-equilibrium step preceding rate-limiting peroxo O-O
bond homolysis in the reactions of ONOOH.)
Interpretation of the Pressure Dependencies of Reaction
Rate Constants. (i) Bimolecular Reactions. The experimentally
measured bimolecular rate constant (kobs) for the formation of
ONOOCO2 is given by kobs ) k2/{(1 + [H+]/Ka)(1 +
-
Interpretation of the Pressure Dependencies of Product
Yields. According to Scheme 2, the product yields that are
attained when all of the radicals escaping the cage are scavenged
by reductants are dictated by the partitioning of the caged radical
pair between cage escape (kD) and rearrangement to NO3- (kN).
The pressure dependence of the rate-constant ratios can be
expressed as ∂ln(kD/kN)/∂P ) (∆VqN - ∆VqD)/RT (≡-∆(∆Vq)/
RT, where ∆(∆Vq) is the difference in volumes of activation
for cage escape and rearrangement within the cage). From the
pressure dependence of the maximal product yields (Ym), given
by the expression Ym ) kD/(kN + kD), one can calculate ∂ln(kD/
Kb/[H+])},8 where k2 is the intrinsic rate constant for reaction
between ONOO- and CO2, Ka ) 2 × 10-7 M is the acid
dissociation constant for ONOOH, and Kb ) 1 × 10-6 M is
the constant for the CO2 hydration-dehydration equilibrium,
CO2 + H2O h H+ + HCO3-. Under the experimental
conditions (pH 7.2), this equation reduces to kobs ≈ k2[H+]/Kb.
Since, in this case, the second acid dissociation constant (Ka′)
for phosphate, H2PO4 h H+ + HPO42-, is equal to [H+], it
-
follows that kobs ≈ k2Ka′/Kb, and ∆Vqobs ≈ ∆Vq(k2) + ∆V°(Ka′)
- ∆V°(Kb). The volumes of reaction for proton dissociation
from H2PO4- and CO2 hydrolysis are ∆V°(Ka′) ) -24 and -27
cm3 mol-1, respectively.54 Thus, the effects of pressure upon
kN)/∂P, hence ∆(∆Vq). Results obtained for radical scavenging
4-
of ONOOH decomposition products by Fe(CN)6
and
the two equilibria are mutually compensating and, from ∆Vq
Mo(CN)84-, and for ONOOCO2 decomposition products by
Fe(CN)64-, are listed in Table 1. For ONOOH decomposition,
∆(∆Vq) is independent of the identity of the scavenging ion
and the reaction pH; this case is expected for the mechanism
given in Scheme 2. In all cases, the values are large positive
numbers, which indicates that greater volume expansion occurs
-
obs
) -22 cm3 mol-1, one calculates ∆Vq(k2) = -25 cm3 mol-1
.
This value is consistent with a reaction that involves association
of a neutral molecule with an ion for which there is no
significant change in charge density, hence, only minor con-
tributions from solvent electrostriction. It therefore supports
proposals that CO2-catalyzed reactions of ONOO- involve
intermediary formation of a discrete ONOOCO2 adduct.8,55
-
•
•
-
(46) Under the usual reaction conditions (see text), the NO2 and CO3
free radicals are effectively scavenged, so that k-D ≈ 0. Application
of the steady-state approximation to the caged radical pair (Scheme
2) then gives ko ) kC(kD + kN)/(k-C + kD + kN), where ko is the
pH-independent first-order rate constant for ONOOH decomposition.
In water, kN/kD = 1.5 (determined from product yields for the “indirect”
reactions) and kN/k-C = 1,47 so that kobs = 0.6 kC. Assuming that kD
exhibits Debye-Stokes-Einstein behavior and the other microscopic
rate constants are insensitive to viscosity, increasing the viscosity by
20-fold would increase kN/kD to ∼30 for which kobs = 0.5 kC, i.e.,
causing the observed rate constant to decrease by less than 20%.
(47) Merenyi, G.; Lind, J.; Goldstein, S.; Czapski, G. J. Phys. Chem. A
1999, 103, 5685-5691.
The rate law for reaction of Ni(cyclam)2+ with peroxynitrite
is d[Ni(cyclam)3+]/dt ) k2′[ONOOH][Ni(cyclam)2+];16 the
combination of a small ∆Hq with a large negative ∆Sq suggests
that reaction occurs by an inner-sphere mechanism involving
ONOOH coordination prior to electron transfer.56 Following
algebraic arguments analogous to those described above, for
reaction of ONOOH with Ni(cyclam)2+ at pH 7.2 we obtain
the relationships kobs ≈ k2′Ka′/Ka and ∆Vq ≈ ∆Vq(k2′) +
obs
∆V°(Ka′) - ∆V°(Ka). Using ∆Vq ) -7 cm3 mol-1 and
obs
(48) Additional factors which can reduce the magnitude of experimentally
determined viscosity effects in this system (microheterogeneity,
reactions of secondary radicals) are discussed in ref 52.
∆V°(Ka) ) -7 cm3 mol-1 27
,
one obtains ∆Vq(k2′) ≈ +10 cm3
mol-1. This large positive value may reflect loss of coordinated
(49) Bonini, M. G.; Radi, R.; Ferrer-Sueta, G.; Ferreira, A. M. D. C.;
Augusto, O. J. Biol Chem. 1999, 274, 10802-10806.
(54) Isaacs, N. S. Liquid-Phase High-Pressure Chemistry; Wiley: New
York, 1981.
(55) Houk, K. N.; Condroski, K. B.; Pryor, W. A. J. Am. Chem. Soc. 1996,
118, 13002-13006.
(56) See, e.g.: Drljaca, A.; Hubbard, C. D.; van Eldik, R.; Asano, T.;
Basilevsky, M. V.; le Noble, W. J. Chem. ReV. 1998, 98, 2167-2289.
(50) See also: Meli, R.; Nauser, T.; Koppenol, W. H. HelV. Chim. Acta
1999, 82, 722-725.
(51) Goldstein, S.; Czapski, G. J. Am. Chem. Soc. 1998, 120, 3458-3463.
(52) Goldstein, S.; Czapski, G. J. Am. Chem. Soc. 1999, 121, 2444-2447.
(53) Lehnig, M. Arch. Biochem. Biophys. 1999, 368, 303-18.