4334 J. Phys. Chem. A, Vol. 101, No. 24, 1997
Scannell et al.
and filtered, and the the solvent was removed by rotary
evaporation. The solid was recrystallized twice from C2H5OH
held fixed at a number (20-50) of preselected values. The best
fit was selected from the case where the sum of the squares
was minimized and through visual inspection of the 20-50 fits.
This procedure was repeated three times for each reported fit,
“fixing” each of the three parameters in turn and allowing the
remaining two to relax. For all of the cases reported here, this
procedure converged on the same best fit values (to within the
stated uncertainties) regardless of which parameter was “fixed”
and which were allowed to relax. We estimate the uncertainty
in Ered to be (0.08 V and in λ to be (5 kcal/mol.
1
(5.6 g, 92%): mp 111-112 °C (lit.27 mp 113 °C); H NMR
(CDCl3): δ 5.57 (s, 1H), 3.35 (s, 3H), 3.28 (s, 3H), 2.19 (s,
3H). 13C NMR (CDCl3): δ 162.29, 152.52, 151.32, 101.12,
31.57, 27.80, 20.07. Low resolution MS: m/z (relative intensity)
154 (M+, 100), 97 (21), 82 (62), 55 (66).
Cyclobutyldimethylthymine Dimers (csDMTD, tsDMTD).
1,3-Dimethylthymine (8.5 L, 1 mM aqueous solution) was
frozen in batches into sheets (ca. 4 mm thick) and irradiated
for 2 h using a 450 W medium-pressure Hg-vapor lamp fitted
with a Vycor filter. During irradiation the solution was kept
frozen on a bed of dry ice. After 2 h, the solution was thawed,
and the solvent was removed by rotary evaporation. The
residue, a yellow oil, was dissolved in CH3OH and spotted onto
a preparatory TLC plate (2000 µm). The plate was developed
first in 60:40 EtOAc:hexane and then in 85:15 EtOAc:hexane.
The silica gel containing the cis-syn dimer, the lower band (Rf
) 0.06), and the trans-syn dimer, the middle band (Rf ) 0.15),
were isolated and individually washed with CH3OH (ca. 15 mL).
The silica gel was removed by vacuum filteration, and the
solvent was subsequently removed by rotary evaporation. The
resulting solids were individually recrystallized twice from CH3-
OH.
cis-syn-Cyclobutyldimethylthymine Dimer (csDMTD) (0.108
g, 4%): mp 249-253 °C (lit.28 mp 251 °C,); 1H NMR
(CDCl3): δ 3.69 (s, 2H), 3.11 (s, 6H), 2.97 (s, 6H), 1.47 (s,
6H). 13C NMR (CDCl3): δ 169.39, 152.37, 60.51, 47.49, 35.69,
28.07, 19.24. Low resolution MS: m/z (relative intensity) 154
(100), 97 (38), 70 (74), 69 (47) (the M+ peak is not visible
because the compound splits into its constituent halves under
the MS conditions).
trans-syn-Cyclobutyldimethylthymine Dimer (tsDMTD)
(0.22 g, 9%): mp 258-262 °C (lit.29 mp 255 °C). 1H NMR
(CDCl3): δ 3.32 (s, 2H), 3.14 (s, 6H), 3.06 (s, 6H), 1.56 (s,
6H). 13C NMR (CDCl3): δ 169.54, 151.75, 64.35, 36.14, 27.76,
24.92, 12.02. Low resolution MS: m/z (relative intensity) 154
(100), 140 (24), 97 (15), 70 (79), 69 (78) (the M+ peak is not
visible because the compound splits into its constituent halves
under the MS conditions).
Fluorescence Quenching Experiments. A stock solution
of the fluorescent sensitizer is prepared by sonicating the desired
compound (1-3 mg) in spectroscopic grade CH3CN (100 mL)
for 30 min. This process results in a sensitizer concentration
of about 10-2 M. This solution (2.5 mL) is placed in a quartz
cuvette, sealed with a septum, lined with Teflon tape to prevent
contamination, and then purged with Ar for 15 min. A stock
solution of the quencher (200 mM) is prepared by dissolving
the appropriate amount in spectroscopic grade CH3CN and
sonicating the resulting solution for 30 min. Aliquots (12.5 µL)
of the quencher solution are injected into the sealed cuvette
containing the sensitizer. This results in the increase of the
quencher concentration in the cuvette by 1 mM steps. The
fluorescence scan of the sensitizer is recorded at each step (0-6
mM). The excitation wavelength of the sensitizer (330 nm) is
chosen in order to ensure that none of the light is absorbed by
the quencher. The fluorescence quenching rate constants kq were
determined from a Stern-Volmer analysis.30
Results and Discussion
Three types of structural variations were the focus of the
present study. First, it was of interest to determine to what
degree methyl substitution influences the Ered of the pyrimidine
derivatives. To this end we examined 1,3-dimethyluracil
(DMU) and 1,3,6-trimethyluracil (TMU) and compared their
behavior with that of 1,3-dimethylthymine (DMT), which has
been previously examined. The syntheses of these substrates
follow well-known procedures which are described in the
Experimental Section. Second, it was of interest to determine
the effects of saturating the 5,6-double bond in the pyrimidines.
To this end 1,3-dimethyl-5,6-dihydrouracil (DMTH2), 1,3-
dimethyl-5,6-dihydrothymine (DMTH2), and 1,3,6-trimethyl-5,6-
dihydrouracil (TMUH2) were synthesized and examined. Fi-
nally, the trans-syn-cyclobutane dimer of dimethylthymine
(tsDMTD) was examined in order to explore the effect of
stereochemistry on the ability of the bases to accept electrons.
The trans-syn dimer has the same bonds and connectivity as
the previously studied cis-syn dimer (csDMTD). However the
two diastereomers differ in the relative spatial arrangement of
the thymine rings. In the cis-syn both thymine rings are on the
same face of the cyclobutane ring and in the trans-syn they are
on the opposite face. Structures of all of the substrates are
shown in Table 1.
Analysis of fluorescence quenching rate constants was used
to determine the reduction potentials of the substrates. Similar
methods have been previously employed by us31,32 and others.33-35
This technique holds several advantages over the more typical
electrochemical methods. First, the measurements can be made
in homogeneous solutions in the absence of added salts. Second,
the potentials of very unstable organic radical ions can be
measured with reasonable accuracy. Of course, fluorescence
quenching is less direct than any equilibrium-based measure-
ment. The accuracy of the values thus derived are dependent
on the accuracy of the model which relates the kinetic
information to the desired thermodynamic quantities. However,
as the goal here is to identify how small structural alterations
affect Ered, the absolute values of Ered are of less importance
than how they change and in what direction.
Electron transfer from the excited state sensitizers (S*) to the
pyrimidine derivatives (Q) follows the kinetic scheme given in
eq 1.36 The quenching of S* involves a diffusive encounter of
k3
9
S + Q
9
hν8 S* + Q {kkdiff } (SQ)* {kkct } (S+•Q-•)*
8 S+• + Q-•
(1)
-diff
-ct
S* with Q. (kdiff) to form the so-called precursor complex,
followed by a charge transfer step (kct) to form the successor
complex.
Fluorescence quenching rate constants, kq, for a series of
sensitizers with each of the substrates were determined by
Stern-Volmer analysis.30 The sensitizers employed are the
same as the series that was used in a previously published
study.31 The list of sensitizers and their photophysical properties,
Data Analysis. The procedures for fitting the kq data to the
Rehm-Weller relationship is described in some detail else-
where.31 Basically a simplex minimization algorithm was used
to minimize the sum of the squares of the differences between
the experimental data and a theoretical curve that was generated
from the parameters Ered, λ, and kmaxKdiff. In order to determine
the uniqueness of the fits, only two of the parameters were
adjusted in the algorithm while the remaining parameter was