nm) in the absence and presence of xylenes, toluene, or the
corresponding aldehydes were determined by using a time-
resolved fluorescence spectrofluorophotometer. The rate
ylsemiquinone radical anion. The ESR spectrum of AcrPh•
was persistent for several hours in deaerated acetonitrile. The
hyperfine splitting constants and the maximum slope line
widths (∆Hmsl) were determined from a computer simulation
of the ESR spectra. The ∆Hmsl value thus determined
increases linearly with an increase in the concentration of
-
1
constants of fluorescence quenching k
q
() K τ ) by pho-
q
toinduced electron transfer are determined from the slopes
of the linear Stern-Volmer plots of τ
MeCN ) vs the quencher concentration. The k
0
/τ (τ
0
) 37 ns in
values thus
13
+
q
AcrPh in MeCN. Such line width variations of the ESR
determined are listed in Table 2.
spectra can be used to investigate the rate processes involving
the radical species. The rate constants (kex) of the electron-
+
•
transfer exchange reactions between AcrPh and AcrPh were
0
determined using eq 1, where ∆H msl is the maximum slope
line width of the ESR spectra in the absence of AcrPh ,
Table 2. Fluorescence Quenching Rate Constants of AcrH+
+
with Xylenes, Toluene, and Aldehydes in Deaerated MeCN at
i
respectively, and P is a
2
98 K
7
0
1
.57 × 10 (∆H - ∆H msl)
msl
k )
(1)
ex
+
(
1 - P )[AcrPh ]
i
statistical factor which can be taken as nearly zero (see
1
4
Supporting Information). The reorganization energies (λ)
of the electron-transfer reactions are obtained from the kex
1
1
-1 -1
values using eq 2 (Z ) 10
M
s ), where the effect of
-
1
-1
-1
[
(k ) - (kdiff) ] ) Z exp(λ/4k T)
(2)
ex
B
diffusion (kdiff ) 2.0 × 10 M-1 s-1 in MeCN and 1.2 ×
10
1
010
M
-1
s
-1
in chloroform, respectively) is taken into
1
+
The AcrH * fluorescence was quenched efficiently by
account and k is the Boltzmann constant. The λ value in
chloroform is determined as 0.27 eV which is smaller than
the value in MeCN (0.34 eV).
B
1
+
electron transfer from xylenes to AcrH *, whereas no
7
quenching was observed by p-tolualdehyde (k
q
, 1 × 10
value decreases in the following order:
p-xylene > o-xylene > m-xylene > o-tolualdehyde > toluene
m-tolualdehyde . p-tolualdehyde (not observed). This
-
1
-1
M
s ). The k
q
Since the λ values (0.27, 0.34 eV) are much smaller than
0
the driving force of the back electron transfer (-∆G
et
)
•
0
15
>
2.36 eV) from AcrH (E vs SCE ) -0.43 V) to the
p-xylene radical cation (E ) 1.93 V), the back electron
ox
0
16
order is consistent with the order of the monooxygenated
and dioxygenated product yields in Table 1. Thus, the faster
the photoinduced electron transfer, the larger is the product
red
transfer is deeply in the Marcus inverted region, where the
back electron transfer rate is expected to slow as the λ value
1
7
yield. However, the k
q
value for p-xylene determined in
decreases. The slower back electron transfer rate with
decreasing the solvent polarity leads to an increase in the
product yield as observed experimentally.
9
-1 -1
chloroform (4.2 × 10 M s ) is smaller than the value in
acetonitrile in Table 2, in contrast to the improved product
yield in chloroform as compared to that in the more polar
solvent acetonitrile (vide supra). The improved product yield
in chloroform may result from a decrease in the reorganiza-
tion energy of the electron transfer with a decrease in the
solvent polarity, which results in a slower back electron
The further improvement of the product yield by employ-
+
+
ing AcrPh instead of AcrH can also be ascribed to the
slower back electron transfer rate for the former than the
latter. In the Marcus inverted region, the back electron
transfer becomes slower as the driving force increases. Since
•
0
•
0
18
transfer from AcrH to the p-xylene radical cation in Scheme
(vide infra). Since the deprotonation of the p-xylene radical
the E ox value of AcrPh (E ox vs SCE ) -0.55 V) is more
•
0
15
1
negative than the value of AcrH (E ox vs SCE ) -0.43 V),
the driving force of the back electron transfer from AcrPh•
cation, which leads to the oxygenated product, competes with
the back electron transfer, the slower back electron transfer
results in the larger product yield.
The reorganization energies are evaluated by determining
the rate constants of electron-transfer self-exchange reactions
between 9-phenyl-10-methylacridinium ion (AcrPh ) and the
corresponding one-electron reduced radical (AcrPh ) in
acetonitrile and chloroform. The AcrPh radical was produced
by the electron-transfer reduction of AcrPh by tetrameth-
(14) Cheng, K. S.; Hirota, N. InVestigation of Rates and Mechanisms of
Reactions; Hammes, G. G., Ed.; Wiley-Interscience: New York, 1974; Vol.
VI, p 565.
(15) Fukuzumi, S.; Koumitsu, S.; Hironaka, K.; Tanaka, T. J. Am. Chem.
Soc. 1987, 109, 305.
+
0
0
(
16) The E ox value of p-xylene, which corresponds to the E red value of
•
the radical cation, was determined by the second harmonic ac voltammetry
(SHACV) measurements. The SHACV method is known to provide a
superior approach to the direct evaluation of the one-electron redox potentials
in the presence of a follow-up chemical reaction; Arnett, E. M.; Amarnath,
K.; Harvey, N. G.; Cheng, J.-P. J. Am. Chem. Soc. 1990, 112, 344.
(17) (a) Marcus, R. A. Annu. ReV. Phys. Chem. 1964, 15, 155. (b) Marcus,
R. A. Angew. Chem., Int. Ed. Engl. 1993, 32, 1111.
•
+
(
13) Poulos, A. T.; Hammond, G. S.; Burton, M. E. Photochem.
Photobiol. 1981, 34, 169.
Org. Lett., Vol. 2, No. 23, 2000
3649