trolled with Chelex-treated phosphate buffer (100 mM, pH 7.4)
for all other experiments.
shielded conductivity detector. Standard curves were deter-
mined with ClϪ concentrations from 0–150 µM. Chloramine
decomposition was achieved by steady state radiolysis experi-
ments with a 60Co source (dose rate, 37.5 Gy minϪ1). Samples
were prepared in 10% tert-butyl alcohol solutions and degassed
with N2 immediately before irradiation. The HOCl used
for chloramine formation in these experiments was purified
to reduce the initial ClϪ concentration by the method of
Henderson et al.44
Pulse radiolysis
Pulse radiolysis experiments were carried out at the University
of Notre Dame using an 8 MeV Titan Beta model TBS-8/16-1S
linear accelerator. Pulse lengths were typically 2–10 ns with
absorbed doses of 2–8 Gy (J kgϪ1). Dosimetry was carried out
using N2O-saturated KSCN solutions as described previously.17
A full description of the pulse radiolysis setup and the data
acquisition system has been detailed elsewhere.17–19
Determination of chloramine molar absorption coefficients and
stability studies
All solutions were prepared with 10% tert-butyl alcohol and
thoroughly degassed with N2. Under these conditions the
The UV absorbance of chloramine solutions at 252 nm
was determined on a Perkin Elmer Lambda 40 UV/visible
spectrometer. The chloramine concentrations were determined
by the use of 5-mercapto-2-nitrobenzoic acid (TNB) as
described previously.2,10 Experiments to investigate the stability
of the chloramides showed 65% conversion of HOCl to
chloramide for (Gly)2, or 45% for (Ala)2; these values were used
to calculate the chloramide concentrations in the stock solu-
tions used for pulse radiolysis. The molar absorption coef-
ficients could not be determined accurately due to interfering
absorbances from the amides themselves, and other products.
ؒ
oxidising HO radicals were converted to relatively unreactive
ؒ
CH2C(CH3)2OH radicals (G = 2.7), leaving the strongly
reducing hydrated electrons (eϪaq) as the major primary product
(G = 2.7). In addition to eϪaq, about 20% of the primary species
ؒ
comprised reducing H atoms (G = 0.6). The contributions of
eϪaq and H atoms to the observed kinetics were investigated by
ؒ
degassing with N2O instead of N2, as this converts eϪ to
aq
ؒ
ؒ
the unreactive CH2C(CH3)2OH radicals (via HO formation),
leaving H atoms as the primary reactive species.
ؒ
Stock chloramine solutions were prepared in H2O and the
concentrations were determined by UV/visible spectroscopy
using the molar absorption coefficients given in Table 1.
Typically a small molar excess (1.1–1.2) of the substrate (amine
or amide) was added over the HOCl to ensure complete con-
sumption of the HOCl without the formation of dichlorinated
products (which are known to be formed at higher HOCl :
amine ratios).10 Stock solutions were kept in the dark at 4 ЊC
and aliquots were added via syringe to the bulk 10% tert-butyl
alcohol solution. The quenchers (hydroquinone (QH2) and
methyl viologen (MV2ϩ)) used to study the reactivity of the
secondary radicals were also prepared as concentrated stock
solutions and kept in the dark at 4 ЊC (under N2 or Ar) before
stepwise addition to the bulk sample. When Trolox was used
as the quencher, individual samples (in 10% tert-butyl
alcohol) were prepared for each Trolox concentration, as the
low solubility of Trolox prevented preparation of a con-
centrated stock solution. A fixed concentration of chloramine
was added to each Trolox-containing solution via syringe, and
the samples were purged with N2.
Acknowledgements
This work was supported by the Australian Research Council,
Grants A00001441 and F00001444. David Pattison would like
to thank the Sydney Free Radical Group for providing a travel
grant to undertake this research. He is also grateful to the
Radiation Laboratory of the University of Notre Dame and
the U.S. Department of Energy for the opportunity to use their
pulse radiolysis, and other laboratory, equipment. The authors
would also like to acknowledge Mr Kurt Belting and Dr Igor
ˇ
Stefanic for technical assistance. K.-D. Asmus is currently
on sabbatical leave from the Department of Chemistry and
Biochemistry of the University of Notre Dame.
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The reactions were monitored by optical absorbance at the
absorbance maxima of the species of interest: for eϪaq, λ = 720
nm, ε = 19000 MϪ1 cmϪ1; QϪ , λ = 427 nm, ε = 7200 MϪ1 cmϪ1
;
ؒ
Trolox-O , λ = 440 nm, ε = 5400 MϪ1 cmϪ1; MVϪ , λ = 600 nm,
ؒ
ؒ
ε = 12820 MϪ1 cmϪ1 19,42,43
.
Analysis of the kinetic traces was carried out using Origin 4.1
(Microcal). A single exponential fitting procedure was used to
analyse pseudo-first-order eϪ decay curves. However, for
aq
secondary quencher growth curves, a fitting expression that
corrected for long-term decays due to radical–radical reactions
was used. Absolute errors for kinetic radiation chemical
experiments are generally considered to be about 10%. These
errors also apply to the current data unless otherwise stated.
All experiments were carried out at approximately 22 ЊC.
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Determination of Cl؊ concentrations
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Chloride ion concentrations were determined by means of
high performance ion chromatography using a Dionex LC20
chromatography enclosure coupled with a Dionex GP40
gradient pump and a Dionex ED40 electrochemical detector.
The ClϪ ions were separated by isocratic elution (retention time,
3.6 min) with a buffer containing 2.7 mM Na2CO3 and 0.3 mM
NaHCO3 (flow rate, 1.5 mL minϪ1) on an IonPac AS12A
(4 mm) analytical column with an IonPac AG12A (4 mm)
guard column. An anion self-regenerating suppressor (ASRS-
ULTRA (4 mm)) was used to minimise the background
conductivity (<15 µS). Ion peaks were detected with a CD25
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1466
J. Chem. Soc., Perkin Trans. 2, 2002, 1461–1467