172
F. Ronzani et al. / Journal of Catalysis 303 (2013) 164–174
Table 5
with the quantum yields of conversion of 1 (/conv), approximated
by calculating the ratio of the converted molar amount of 1 and
the photon flux absorbed by the sensitizer. The same trends are ob-
Calculated free energy for the electron-transfer reactions from
singlet or triplet excited states of the studied photosensitizers. Redox potentials are
a-terpinene to the
expressed vs. SCE for compounds in acetonitrile solutions.
D
ꢀ
G values obtained from
ꢀ DE00 Redox poten-
h
i
e02
aꢀ
the Rehm–Weller equation: DG ¼ 96:4 E0ðD=D ꢀ E0ðSens=Sens
tained considering kp or /conv
.
ꢀþ Þ
ꢀꢀ Þ
tial of 1: E0ð1=1 ¼ 1:60 V vs. SCE [101].
ꢀþ Þ
For the homogeneous solution experiments, the reactivity order
was ANT-COOH > DBTP-COOH > RB; the same trend was found for
the silica-supported sensitizers. Anthraquinone both in solution
and supported on silica was the most efficient photosensitizer,
with rate constants at least one order of magnitude higher than
for the other catalysts. DBTP, consistent to that observed in terms
of quantum yields of singlet oxygen production, was at least 1.5
times more efficient than RB. Notably, kp for DBTP–Si was only
20% lower than that for DBTP-COOH in homogeneous solution. In
contrast, the drops in activity for silica-supported RB and ANT-
COOH vs. their soluble forms were significant with about 40% for
RB–Si and 80% for ANT–Si, respectively. For RB-derived photosen-
sitizers, the rate constants strongly depended on the support and
RB–PSref was found four times more efficient than RB–Si. In addi-
tion, the rate constant did not increase consistently with higher
amounts of RB–PSref (entries 3 and 4): this behavior may be caused
by physical quenching of singlet oxygen by the solid sensitizer or
by unfavorable absorption of light due to scattering and diffraction
phenomena. For RB, silica was clearly not the most suitable sup-
port, while polystyrene was found advantageous for this reaction.
The kP and /conv values suggest that the reaction rates and effi-
ciencies depended on the mechanism. Compared to the DBTP- and
RB-derived sensitizers, ANT-based materials have a much higher
0
Sens
D
E00 (S1)
D
G (S1)
D
E00 (T1)
DG (T1)
ꢀꢀ
ESens=Sens
(kJ molꢀ1
)
(kJ molꢀ1
)
(kJ molꢀ1
)
(kJ molꢀ1
)
(V)
ANT
RB
ꢀ0.86
ꢀ1.20
[102]
284
213
ꢀ52.6
261
164
ꢀ26.7
55.0
100.1
DBTP ꢀ0.92
288
ꢀ50.8
–
–
RB for singlet oxygen production, without any evidence of elec-
tron transfer. Since the energy of the DBTP triplet state is not
easily determined, it is difficult to conclude on its properties.
With ANT, electron- or H-transfer are possible and further radi-
cal-chain mechanisms are favored on thermodynamic grounds:
D
Hf (reaction 7) = ꢀ31.9 kcal molꢀ1 and
DHf (reaction
8) = ꢀ18.8 kcal molꢀ1 [81]. This result confirms previous reactiv-
ity of ANT sensitizers with sulfides where high amounts of sul-
fonic and sulfuric acids were obtained and attributed to an
electron-transfer mechanism [75]. Moreover, although anthraqui-
none is a common photosensitizer, capable of producing singlet
oxygen by energy transfer upon irradiation (Table 2) [95,96],
anthraquinone-2-sulfonate was also shown to produce superox-
ide radical anion Oꢀ2ꢀ by electron transfer [95,96] in addition to
1O2 [97,98]. The question of anthraquinone sensitized superoxide
radical anion formation was raised [75,99,100], but should be
possible considering the reduction potential of ANT and O2
capability of photooxidizing a-terpinene (1): electron-transfer-in-
duced oxidative cleavage yielding 3 as a main product (Scheme 5)
must thus be much faster than photooxygenation to 2. For the
reactions involving 1O2 generation through energy transfer and
its cycloaddition to 1, the DBTP-based materials were at least twice
faster than their RB-derived counterparts, in line with what was
(E0AQ=AQꢀꢀ ¼ ꢀ0:86 V and EO0
¼ ꢀ0:57 V vs. SCE in ACN, respec-
2=Oꢀꢀ
2
tively) [99,100].
expected from the respective values of UD
.
As commonly observed with supported photocatalysts, the
reaction efficiency decreased: this may be due to higher physical
quenching of singlet oxygen by the suspended solid support.
3.5. Kinetic studies
Selected reaction rate constants (k) for the photosensitized oxi-
dation of 1 were determined by UV–Vis spectroscopy over the first
30 min of each experiment (Table 6), because in case of ANT-
derived sensitizers, the formation of strongly absorbing secondary
products, in particular 4, impacted on the values for longer
irradiation times. Under all experimental conditions, pseudo-
zero-order reactions were established. In addition, the reaction
rates were of the same order of magnitude.
4. Conclusions
The preparation, characterization, and use of novel silica-
immobilized organic photocatalysts based on rose bengal (RB),
antraquinone (ANT), and a newly developed cyanoanthracene
derivative (DBTP) were described. The efficiency of the solid-
The simple rate constant values (k) do not consider the different
absorption properties of the three sensitizers. In particular, their
molar absorption coefficients and the position of their absorption
maxima relative to the emission spectra of the lamps differ signif-
icantly (Figs. 2 and 3). Thus, approximate values of the rate con-
stants normalized by the photon flux absorbed by the sensitizer
(kP) were calculated and additionally compiled in Table 6, together
supported sensitizers for the photooxidation of a-terpinene 1
was compared to that of their soluble counterparts. In ACN, a high-
er singlet oxygen quantum yield (UD = 1.03) was measured for
DBTP than for RB and ANT (UD = 0.71 and 0.76, respectively)
relative to perinaphthenone. Although formation of ascaridole 2
by singlet oxygen addition to 1 has been extensively studied, the
fate of the by-products (followed by GC–MS and UV–Vis analysis)
Table 6
Kinetic constants for photosensitized conversion of 1 (k = kinetic constant directly calculated forms the evolution of UV absorption signals; kP = approximate values of kinetic
constants normalized by the estimation of the photon flux absorbed by the Sens; /conv = approximate values of quantum yields of conversion of 1).
Entrya
Sens
Sens (mmol)
k (10ꢀ2 M minꢀ1
)
kP (10ꢀ2 M Einsteinꢀ1
)
/
(10ꢀ6 mol1 Einsteinꢀ1
)
conv
2
3
4
5
RB
0.030
0.003
0.015
0.038
0.015
0.014
0.030
0.003
5.00 1.00
1.44 0.03
2.80 0.03
0.81 0.02
5.75 0.08
4.10 0.07
6.70 0.40
1.30 0.03
7.0 0.2
3.8 0.1
4.4 0.1
1.1 0.1
13.0 0.2
10.0 0.2
840 40
105
19
39
5
170
120
5
2
3
1
5
5
RB–PSref
RB–PSref
RB–Si
DBTP-COOH
DBTP–Si
ANT-COOH
ANT–Si
7
10
11
12
6300 100
880 15
180
4
a
Entry numbers refer to Table 2.