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H. Katsumata et al. / Ultrasonics Sonochemistry 17 (2010) 200–206
201
role in producing oxidants because of its high molar absorptivity
and quantum yield. For example, several attempts have been made
to apply ferrioxalate as a photochemical method in the treatment
of polluted water, using artificial or solar light [25,26].
Concentration of Fe(II) formed during the degradation process
was determined by the phenanthroline (phen) method. The absor-
bance of Fe(II)-phen complex was taken at 510 nm (e510
=
nm
1.118 ꢂ 104 L molꢀ1 cmꢀ1). The hydroxyl radical concentration
was estimated using a deoxyribose method [27]. Deoxyriobose
(3.5 mM) was reacted with OHꢀ radicals generating by the opti-
mized ultrasound/ferrioxalate/UV system. The reaction was
stopped by addition of 5 mL thiobarbituric acid (1% w/v in
50 mM NaOH) and 5 mL of trichloroacetic acid (2.8% w/v). The mix-
ture was heated at 80 °C for 30 min. The product of the reaction
was quantified at 532 nm using a Shimadzu UV-1650PC double-
beam spectrometer. The concentration of OHꢀ radicals was equated
with thiobarbituric acid active substances using an extinction coef-
In the present study, we have investigated the degradation and
mineralization of fenitrothion in water using of US/ferrioxalate/UV
process. The initial concentrations of Fe(III) and oxalate affected on
the degradation were evaluated. The progress of mineralization of
fenitrothion was monitored by total organic carbon (TOC) content
and ionic chromatography. Furthermore, the intermediate prod-
ucts of fenitrothion during this sono-photocatalytic process have
been identified by gas chromatography–mass spectrometry (GC/
MS). The degradation pathway was proposed on the basis of inter-
mediates formed.
ficient, e .
532 nm, of 153 mMꢀ1 cmꢀ1
The intermediate products during degradation of fenitrothion
were extracted with dichloromethane (2 mL ꢂ 3). The combined
organic fraction was dried by Na2SO4, and concentrated under N2
flow. A GC/MS (Shimadzu GC–MS 5050A) was used for separation
and detection of the intermediate products. The GC was equipped
with a HP-5 capillary column (30 m ꢂ 0.25 mm i.d.) in helium car-
rier gas (1.5 mL minꢀ1) and with splitless injection system. The GC
oven temperature was programmed to hold 50 °C for initial 3 min,
to increase from 50 to 280 °C at a rate of 15 °C minꢀ1 and to hold at
280 °C for 3 min. The injector and interface temperatures were
kept at 280 °C. Mass spectra were obtained by the electron-impact
(EI) mode at 70 eV using the full scan mode.
2. Experimental
2.1. Reagents
Fenitrothion was supplied by Wako Pure Chemical Industries
(Osaka, Japan) and was used as received. Analytical grade ferric
chloride hexahydrate (FeCl3ꢁ6H2O) and sodium oxalate were pur-
chased from Nacalai Tesque (Kyoto, Japan). All other chemicals
and solvents were of the purest grade commercially available
and were used without further purification. All aqueous solutions
were prepared with ultrapure water obtained from an ultrapure
water system (Advantec MFS Inc., Tokyo, Japan) resulting in a
resistivity > 18 MX cm.
3. Results and discussion
2.2. Ultrasonic degradation procedure
3.1. Effect of variables on the degradation of fenitrothion
Sonochemical experiments were conducted in duplicates using
an ultrasonic generator (150 W, 20 kHz, ultrasonic homogenizer
UH-150, SMT Co. Ltd., Tokyo, Japan) equipped with a titanium
oscillator (12 mm of diameter). Experiments were conducted in a
200 ml Pyrex glass cell. One hundred milliliter of fenitrothion solu-
tion and the precise amounts of iron(III) and oxalate was added
into the reaction cell. The pH of the sample solution was adjusted
with HCl and/or NaOH solution. The initial concentration of feni-
trothion in all experiments was 10 mg Lꢀ1 (3.6 ꢂ 10ꢀ5 mol Lꢀ1).
Reaction temperature was kept at 25 1 °C with a water bath.
The sample solution was irradiated with a black light (Toshiba
Lighting & Technology Co.). The beam was parallel and the distance
between lamp and the reactor wall was 10 cm. The lamp was
warmed up for 10 min to reach constant output. In this case, the
short UV radiation (k < 300 nm) was filtered out by the vessel wall.
The intensity of the light was measured by a UV radio meter (UVR-
400, Iuchi Co.) with a sensor of 320 to 410 nm wavelength. The
radio meter was set up at the same position as the reactor.
Effect of ligand on the degradation of fenitrothion by US/Fe(III)/
UV system was examined. Ligands studied were oxalate, malonate
and acetate. These results are shown in Fig. 1. The degradation per-
centage of fenitrothion was 55% after 30 min in the absence of li-
gands because much precipitation of Fe(OH)3 was observed
during the process. Malonate and acetate gave a no ligand effect
for the degradation of fenitrothion although iron precipitation
was not observed. This would be because of low quantum yield
for ferrous ion reproduction [28]. On the other hand, oxalate gave
a positive effect for the degradation of fenitrothion, that is, fenitro-
thion degradation was 65% after 30 min in the presence of oxalate.
2.3. Analyses
The progress in the degradation of fenitrothion was followed
with a HPLC (GL Science Co., Tokyo, Japan) equipped with a GL-
7450 UV detector (GL Science Co.) and a Inertsil ODS-2 separation
column (150 mm ꢂ 4.6 mm i.d., GL Science Co.). The elution was
monitored at 250 nm. The mobile phase was a mixture of acetoni-
trile and water (65/35, v/v), and was pumped at a flow rate of
1.0 mL minꢀ1
.
The progress of mineralization of fenitrothion was monitored
by measuring the TOC. TOC of the sample solution was measured
with a Shimadzu TOC analyzer (TOCꢀVE) based on CO2 quantifica-
tion by non-dispersive infrared analysis after high-temperature
catalytic combustion. The formation of anions was analyzed by io-
nic chromatography using a Metrohm Compact IC 7611 equipped
with a Shodex anionic column (IC SI-90 4E).
Fig. 1. Effect of ligand kind on the degradation of fenitrothion by use of US/Fe(III)/
UV system, (d): absence of ligand; (N): malonate; (j): oxalate; (.): acetate
([Fe(III)]0 = 1 ꢂ 10ꢀ5 M; [ligand]0 = 5 ꢂ 10ꢀ5 M; pH 6.0; ultrasonic power = 150 W;
light intensity = 1.0 mW cmꢀ2).