7
26
C.M. Antonio-Cisneros et al. / Food Chemistry 173 (2015) 725–732
caused a 60% decoloration of CA under optimised conditions
Körbahti & Rauf, 2009). In spectroscopic studies, CA also under-
2.3. Characterisation of the composite
(
went degradation in its solid state by exposure to visible light
under anoxic conditions (Koperska, Łojewski, & Łojewska, 2011).
To date, the advancements in photocatalysis for the degradation
of target substances are undeniable, due to the development of
semiconductor materials. The photocatalytic removal of dyestuffs
from water has been reviewed (Ahmed, Rasul, Martens, Brown, &
Hashib, 2011; Akpan & Hameed, 2009), but the photocatalytic deg-
The morphology and surface composition of the composite
were determined using an Oxford Instruments INCAX-act Energy
350 EDS spectrometer coupled to a JEOL JSM 6610 LV scanning
electron microscope (SEM). The BET surface area was measured
by nitrogen adsorption at 77 K using an Autosorb-1 from Quanta-
chrome Instruments (Boynton Beach, FL) after out-gassing at
573 K for 12 h. The specific surface area was calculated using the
Brunauer–Emmett–Teller (BET) method, and the pore size distribu-
tion was estimated by the Barrett–Joyner–Halenda method (BJH).
The extent of micro- and mesoporosity was calculated using the
t-method. The specific surface area of the raw residues was deter-
mined by the adsorption of methylene blue using a molecular area
2
radation of CA on TiO /carbon materials has not yet been
addressed.
Combinations of TiO
the field of photocatalysis (Leary & Westwood, 2011). In recent
years, the application of these carbon–TiO materials in photoca-
2
and carbon are common composites in
2
2
talysis has gained widespread attention because (i) the solids are
easily recovered after use in a wide range of applications (Foo &
of 1.35 nm in the vertical orientation (Antonio-Cisneros, 2010).
The density of the dry materials was determined in triplicate using
tarred vessels. The point of zero charge (pHpzc) was measured by
methodology reported elsewhere (Bourikas, Vakros, Kordulis, &
Lycourghiotis, 2003).
Hameed, 2010) and (ii) synergistic effects occur between TiO
and carbon (Matos, Chovelon, Cordero, & Ferronato, 2009).
2
Only a few studies have been devoted to the preparation of
TiO /carbon materials using lignocellulosic residues, such as bam-
boo leaves (Huang et al., 2011), pine sawdust (Asiltürk & Sß ener,
012), maize corncob (Sabinas-Hernández, 2011), canola hull
Mahmoodi, Arami, & Zhang, 2011), corn straw powder (Chen
2
2.4. Adsorption and desorption experiments
2
(
Adsorption tests were performed at 25 °C in thermostatted
batch experiments. The solid materials, raw manihot residues, car-
bon, and TiO /carbon composite with a particle size of 0.25 mm
2
et al., 2012), and manihot residues (Antonio Cisneros, 2010) as car-
bon precursors.
Our goal was to measure the sensitivity of aqueous solutions of
CA to UV light under various conditions as well as the photolability
of CA on TiO immobilised on carbon obtained from dried stem res-
2
were dried for 24 h at 75 °C. Then, 100 mg of each material were
weighed into polycarbonate cylindrical cells with lids and con-
tacted at 25 °C with 3 mL of CA solutions with concentrations in
À1
idues of Manihot dulcis (sweet cassava). The present study focused
the range of 100–3000 mg L . The pH was not adjusted and was
on the LC–MS identification of intermediates produced by the irra-
measured to be 5.7 in deionised water. The solution obtained after
24 h, resulting from adsorption equilibrium, was separated from
the exhausted adsorbent, centrifuged (12,000 rpm) and then ana-
lysed with a Hach spectrophotometer at 495 nm (Hach Company,
Loveland, CO). The adsorbed amount a was determined by measur-
diation of CA in the presence of a TiO
2
/C800 composite rather than
on the assessment of the mineralisation of CA.
2
. Experimental
ing the final concentration C
formula a = (C )V/m, where C
À C
CA, V is the volume added (in litres), and m is the weighed mass
f
of CA in the solution and applying the
0
f
0
is the initial concentration of
2.1. Chemicals
(
in grams).
Carminic acid (C.I. 75470), also called crimson lake, cochineal,
Desorption measurements were carried out as follows. A satu-
natural red 4, or E120, was purchased from Sigma Aldrich (St.
Louis, MO; CAS 1260-17-9). The purity of CA, determined by HPLC
was 94%. Glycerol (87% GR) was purchased from Merck (Darms-
tadt, Germany). Titanium oxide aeroxide P25, batch number
rated sample was separated from the solution by filtration. Then,
it was dried at 90 °C for 12 h. Afterwards, the dried sample was
weighed and placed in contact with 3 mL of deionized water in
polycarbonate cylindrical cells at 25 °C for 24 h. The desorbed
amount ades was determined by measuring the concentration of
CA in the solution produced by desorption Cdes and applying the
formula ades = (CdesÁV)/m, where V is the volume added (in L) and
m is the weighed mass (in grams). To determine the equilibrium
1
036070711 (Degussa, Parsippany, NJ) was used for immobilisa-
tion on manihot carbon and was also used for comparative pur-
poses. The natural pH value of the CA solutions was 5.7.
2
2.2. Immobilization of TiO on carbon
2
concentrations, calibration curves with r = 0.999 were obtained
Raw residues of M. dulcis stems without the rind or pith
0.45 mm sieved particles) dried at 70 °C for 24 h were used as
the carbon precursor (Antonio Cisneros & Elizalde-González,
010). The TiO /carbon composite was fabricated as follows. A
glycerol suspension (10 mL) of manihot particles (10 g) was pre-
pared by mixing with a TiO aqueous slurry (10 mL). The resultant
for both the adsorption and desorption experiments.
(
2.5. Photolysis and photocatalytic experiments
2
2
For the irradiation experiments performed on the composite
and TiO (Degussa P25), a 15-mL temperature-controlled quartz
2
2
homogeneous suspension was maintained in a combustion boat at
room temperature for 24 h. The temperature regime of the car-
bonisation consisted of two heating ramps, viz. from room temper-
reactor from Ace Glass Inc. (Vineland, NJ) was used for the exper-
1
iments involving irradiation at 254 nm. A 2 -inch Pen-Ray light
8
source (5.5 W) from Ultra-Violet Products (Upland, CA) was
immersed into the reactor in a quartz jacket. The reactor was
equipped with a water jacket to filter out the IR irradiation of the
lamp and to control the temperature of the solution. A flow of chro-
matographic-grade dry air or nitrogen was allowed to bubble into
the bulk solution. The entire assembly was enclosed in a dark
chamber, and the lamp was switched on after 30 min to establish
adsorption equilibrium. In each experiment, 10 mg of the compos-
À1
ature to 50 °C at 4 °C min , then 1 h at 50 °C and from 50 °C to
À1
8
00 °C at 4 °C min . Then, the residues were maintained at the
maximum temperature for 4 h. The oven was then allowed to cool
to room temperature. A horizontal tubular furnace (Carbolite Fur-
naces Ltd, Hope Valley, UK) with a quartz reactor was used. A car-
2
bon sample not containing TiO , denoted C800, was used for
comparison and was obtained by carbonising raw manihot parti-
cles. The same horizontal tubular furnace and heating program
were used for the C800 sample as for the composite preparation.
À1
ite were added to 10 mL of a solution containing 300 mg L of CA.
Aliquots were collected at regular time intervals during irradiation