248 Matthieu Menager et al.
Scheme 2. Photodecomposition pathways for Cyanox in silica and soil (18).
transient absorbance at preselected wavelength was monitored by a
detection system consisting of a pulsed xenon lamp (150 W), mono-
chromator and a 1P28 photomultiplier. A spectrometer control unit
was used for synchronizing the pulsed light source and programmable
shutters with the laser output. This also housed the high-voltage power
supply for the photomultiplier. The signal from the photomultiplier
was digitized by a programmable digital oscilloscope (HP54522A). A
32-bit RISC-processor kinetic spectrometer workstation was used to
analyze the digitized signal.
Analyses. UV–visible spectra were recorded on a Cary 300 scan
(Varian) spectrophotometer. LC ⁄ MS studies were carried out with Q-
TOF-Micro ⁄ water 2699 from the CRMP center at University Blaise
Pascal. It is equipped with an electrospray ionization source (ESI) and
a Waters photodiode array detector. Each single experiment permitted
the simultaneous recording of both UV chromatogram at a preselected
wavelength and an ESI-MS full scan. Data acquisition and processing
were performed with the MassLynx NT 3.5 system. Chromatography
was run using a Nucleosil column 100-5 C18 ec (250 · 4.6 mm, 5 lm).
Samples (5–10 lL) were injected either directly or after evaporation of
an appropriate volume of the solvent for better detection. The flow rate
was 0.3 mL min)1 and the injected volume was 50 lL. The elution was
accomplished with acidified water (acetic acid 0.4%) and acetonitrile
using the following gradient mode: % acetonitrile (time): 2 (initial); 10
(10 min); 70 (35 min); 2 (42 min).
the cleavage of the P–O-methyl and P–O-aryl bonds together
with the oxidation of the P=S to the oxon group and the
hydrolysis of the cyano moiety (17).
From the photochemical point of view, some studies were
performed on solid support such as silica and soil and in
acetone solution (18). Under illumination, the half-life was
estimated to be 2 and 4 days on soil and silica, respectively,
while it was evaluated to be 120 min in acetone solution.
Photo-oxidation reaction leading to the formation of the
oxon derivative and the scission of the P–O bond generating
4-cyanophenol, as a major product, are reported to be
the main observed processes (Scheme 2). To our knowl-
edge, no detailed studies in aqueous solutions have been
undertaken.
The present work was conducted in order to get a better
insight into the photochemical behavior of CYA in aqueous
solutions. The main goal was the study of the photochemical
kinetic aspect by elucidating the nature of the by-products. The
use of both conventional and time-resolving techniques will
permit us to propose a detailed mechanism for the disappear-
ance of CYA and the photogeneration of the products.
The consumption of CYA and the formation of the by-products were
monitored by an analytical HPLC using an HP1050 apparatus equipped
with a photodiode array detector. The experiments were performed by
UV detection at either 230 or 250 nm and by using a reverse-phase
MachereyNagelcolumn(NucleodurC8, 250 mm · 4.6 mm, 5 lm). The
following gradient program was used by employing acidified water
MATERIALS AND METHODS
Materials. CYA or (O-(4-cyanophenyl) O,O-dimethyl phosphoto-thio-
ate) (98%) was purchased from Aldrich. Cyanophenol was from
Jansen Chimica. Acrylamide and hydroquinone (>99%) were pro-
vided by Aldrich. They were all used as received without further
purification. All other reactants were of the highest grade available.
The solutions were prepared with deionized ultra pure water which was
purified with the Milli-Q device (Millipore) and its purity was
controlled by its resistivity.
(acetic acid 0.4%) (1) and acetonitrile (2) at 1 mL min)1
.
Time (min)
Initial
3
13
20
30
% A
% B
95
5
80
20
80
20
5
95
95
5
Steady-state irradiations. For kinetic as well as analytical purposes,
aqueous solutions were irradiated with a parallel beam using a xenon
arc lamp (1600 W) equipped with a Schoeffel monochromator. The
bandwidth was 10 nm. Solution in a quartz cell (1 cm optical path
length) was deoxygenated by argon or nitrogen bubbling or oxygen-
ated by oxygen bubbling for 20 min prior to irradiation. The cell was
then closed using a septum. The initial concentration of the solution
was checked by HPLC analysis after bubbling. The irradiations at
254 nm were obtained with PHILIPS TUV 6 W lamp delivering a
pH measurements were carried out with a JENWAY 3310 pH-
meter equipped with an Ag ⁄ AgCl glass combination electrode 9102
Orion. The pH of the solutions was adjusted using dilute solutions of
HCl or NaOH. The accuracy achieved was within 0.01 pH units.
RESULTS
parallel beam. Potassium ferrioxalate was used as
a chemical
actinometer as reported in the literature (19). The pH of the
solutions was adjusted using dilute solutions of HClO4 or NaOH.
For analytical purposes, irradiations were performed in a device
equipped with germicide lamps (up to 6) emitting at 254 nm and a
100 mL cylindrical quartz reactor. A similar setup was used for the
irradiation at 313 nm. Solar irradiation was performed in a quartz
reactor (d = 1.5 cm) in Clermont-Ferrand (France, latitude 420ꢁ
above sea level).
Steady-state irradiation studies
The absorption spectrum of CYA in aqueous solution shows
two well-defined bands (Fig. 1). The short wavelength absorp-
tion band, attributed to a p–p* transition, presents an
absorption maximum at 232 nm with a molar absorption
coefficient of 14 000 mol)1 L cm)1
.
The second band
Laser flash photolysis. Transient absorption experiments in the
20 ns to 400 ls time scale were carried out on a nanosecond laser flash
photolysis spectrometer from Applied Photophysics (LKS.60). Exci-
tation (k = 266 nm) was from the fourth harmonic of a Quanta Ray
GCR 130-01 Nd:YAG laser (pulse width ꢀ5 ns), and was used in a
right-angle geometry with respect to the monitoring light beam. A
3 cm3 volume of an argon-saturated solution was used in a quartz cell,
and was stirred after each flash irradiation. Individual cell samples
were used for a maximum of five consecutive experiments. The
(kmax = 266 nm and ꢀ = 1200 mol)1 L cm)1) is owing to an
n-* transition and clearly extends to 320–330 nm permitting a
non-negligible overlap with the solar emission spectrum. Thus,
CYA may be degraded to a certain extent by direct excitation
from solar light. It is worth noting that no obvious degrada-
tion of aqueous solution of CYA in the dark and at room
temperature was observed within the 0.1–2.0 mmol L)1 range.