804 Martin D. Shetlar and Janet Chung
freezing process. Four lamps, contained in two Spectroline X-Series
lamp housings, were placed across the top of the pan containing the
solutions; irradiation was done with the pan resting on top of the dry
ice slabs. The fluence rate at the surface of the frozen aqueous layer in
the pan averaged ca 25 J m)2 s)1, as measured using a Spectronics
DM-254N Ultraviolet Meter (Westbury, NY).
various structures in Scheme 2, including those at bridgehead
nitrogens, denote chiral centers.)
It should be noted that IIIb, IXb and Xb each exists in two
enantiomeric forms. The structures shown in Scheme 2 are for
the 5S,6R (IIIb), 5S,6R (IXb) and 5S,6S (Xb) forms. (The other
(6-4) adduct, in which the 2¢-pyrimidone ring and the OH
group are trans with respect to one another, has not been
observed for Thy and closely related compounds. However,
the analogous adduct has been observed when Ura is irradi-
ated in the frozen state [19].) Structure IVb corresponds to one
of two possible Dewar valence isomers with the same 5S,6R
configuration as IIIb; the one displayed as IVb has a 5S,6R,6¢R
configuration, while the second would have a 5S,6R,6¢S
stereoconfiguration. There is a corresponding pair of Dewar
adduct enantiomers for the the 5R,6S enantiomer of IIIb,
namely 5R,6S,6¢R and 5R,6S,6¢S. As the 5S,6R,6¢R configu-
ration is the mirror image of the 5R,6S,6¢S configuration and,
similarly, the 5S,6R,6¢R configuration is the mirror image of
the 5R,6S,6¢S configuration (corresponding to the generalized
structure of IVb, in which stereochemistry is not considered),
there are two diastereomers of IVb, each having two enantio-
meric forms. Performance of similar analyses for the general-
ized structures corresponding to XIb and XIIb, the (5-4) Dewar
valence isomers, indicates that the situation is the same for
these compounds.
Acetone-photosensitized reactions of MeT in aqueous solution
containing 20% vol ⁄ vol acetone were done with 2 mM MeT. About
170 mL of the solution was placed in a 180 mL quartz tube with a
24 ⁄ 40 outer taper seal joint (Southern New England Ultraviolet Co.,
Hampton, CT). This joint was stoppered with a Pyrex adaptor that
converted a 24 ⁄ 40 inner taper seal joint to 19 ⁄ 38 outer taper seal; an
appropriately sized rubber septum was fitted over the 19 ⁄ 38 joint and
an 8 inch long needle was pushed through the septum. To the end of
this needle was attached a length of Teflon tubing that extended to
near the bottom of the irradiation vessel; an additional bleed needle
was also inserted through the septum. The tube was positioned in the
space between two Pyrex filtered 15 Watt Spectronics UVB (BLE-
1T158) lamps housed in a Spectroline XX-15A lamp holder. The lamp
holder was placed in an upright position, setting at ca 15ꢀ angle to a
supporting wall. The solution was bubbled with nitrogen (99.997%
purity; Puritan Medical Supply, Overland Park, KS) for 20 min and
then irradiated for 120 min under bubbling N2, passed through a glass
frit into an intermediate vessel partially filled with 80% ⁄ 20% vol ⁄ vol
water ⁄ acetone.
Exploratory studies of the photochemistry of MeT. Prior to
preparative studies, preliminary studies were conducted to determine
appropriate concentrations of MeT for use in larger scale studies. The
results of these studies, described in Appendix S1, indicate that
solutions 0.2 mM in MeT gave the best results of the concentrations
examined and this concentration was used in the preparation of parent
solutions for irradiation.
HPLC analysis of an irradiated MeT system: an example. Figure 1
displays the HPLC chromatogram obtained via injection of 100 lL of
250-fold concentrate of a 0.2 mM solution that had been irradiated for
32 min on dry ice as described in Materials and Methods. It was run
on Column A using the following water ⁄ methanol gradient (Gradient
A): 0 min, 10% methanol (MeOH); 3.5 min, 10%; 9 min, 20%;
13 min, 20%; 15 min, 10%; 20 min, 10%, flow rate: 5 mL min)1. The
percent conversion of parent MeT to products was estimated by HPLC
to be 62.3%. From spectra obtained using the ‘‘on the fly’’ spectral
capture capability of the diode array detector, it could be concluded
that Peaks 2, 7, 8 and 10 probably correspond to the four CBDs (31).
Similarly, Peak 3, the very small Peak 5 and Peak 6 displayed spectra
similar in profile to the spectrum of the Thy (6-4) adduct (4). The peak
labeled 9 has a spectrum that is ‘‘double humped’’ in nature with kmax
at 275 and 309 nm. The two peaks labeled 11a and 11b both had kmax
values at 275 nm. By comparison of the integrated peak areas for
Peaks 3 and 6 at 315 nm (assuming equal e315 values), it can be
estimated that ca 2.45 times as much product elutes in Peak 3 as
compared to Peak 6. A very rough estimate of the fraction of total
product, existing as the compounds eluting in Peaks 3 and 6, can be
made by dividing the sum of the peak areas corresponding to these
substances, measured at 230 nm, by the total peak area of all products.
This fraction has a value of 0.13.
‘‘On the fly spectra’’ of Peak 1a–f indicate that many of the
corresponding compounds have maxima between 270 and 280 nm. It
should be emphasized that the absorbance scale for the HPLC trace in
Panel B in Fig. 1 (detection at 271 nm) has a much smaller range than
that given in Panel A (detection at 225 nm). Thus, the actual sizes of
Peaks 1a–f and 11a,b as manifested by peak area or height, are much
smaller than those of the other numbered product peaks shown in
Panel A.
Preparative scale irradiation and isolation of products in the MeT
system for structural characterization. For preparative runs, we
generally irradiated 1000 or 2000 mL of solution in 500 mL batches.
For these runs, the parent solution was irradiated for 64 min,
thawed, refrozen and reirradiated for an additional 64 min. When
this solution was analyzed by HPLC, the percent conversion of
parent MeT to products was 66.9%. This irradiation protocol
increased the yield of the material eluting in Peak 3 by 3.5-fold and
the yield of material in Peak 6 by 1.8-fold (based on area peaks
measured at 315 nm) as compared to the systems irradiated for
32 min.
MATERIALS AND METHODS
General aspects. MeT, Thd and Thy were obtained from Sigma (St.
Louis, MO). HPLC solvents were from Fisher (Fair Lawn, NJ), while
NMR solvents were provided by Aldrich (Milwaukee, WI). Prepara-
tive separations were accomplished on a Shiseido Capcell UG120
10 · 250 mm column (5 mm particle size; Yokohama, Japan) (Column
A), while analytical HPLC separations were usually carried out on a
Capcell UG120 4.6 · 150 mm column (5 mm particle size) (Column
B). Other columns used were Column C, a Microsorb Phenyl column
(4.6 · 250 mm, 5 mm particle size; Varian, Walnut Creek, CA), a
Microsorb Amino column (4.6 · 250 mm, 5lm particle size) (Column
D) and a Capcell Phenyl column (4.6 · 150 mm, 5 lm particle size)
(Column E). The HPLC system used was a Rainin binary gradient
pumping system (Emeryville, CA) coupled to a Hewlett-Packard
1040A diode array detector (Palo Alto, CA). Before injection, all
HPLC samples were subjected to spin filtration on Costar Spin-X
microcentrifuge tubes containing a 0.2 lm nylon filter (Corning
Incorporated, Corning, NY). Rotatory evaporations were accom-
plished on a Buchi R-200 Rotovapor (New Castle, DE) coupled to a
¨
mechanical pump; two dry ice traps were placed in series between
sample and pump.
NMR spectra were run at 600 MHz on a Varian INOVA NMR
spectrometer (Palo Alto, CA). Electrospray ionization (ESI) mass
spectra were run on either a Waters Micromass ZQ4000 instrument
(Beverly, MA) or a Sciex API300 triple quadrupole electrospray
instrument (Toronto, Canada).
Unfiltered Spectronics BLE IT155 lamps, with output mainly at
254 nm and housed in Spectroline XX-15A lamp housings (Westbury,
NY), were used for irradiations of solutions in the ice phase;
Spectronics BLE IT158 lamps, with output centered at 312 nm and
contained in the same housings, were used to photosensitize reactions
in solutions containing acetone or to convert (6-4) and (5-4) adducts to
Dewar valence isomers.
Irradiation methods. Irradiations of MeT in the frozen state at
254 nm were done on either 250 or 500 mL batches of aqueous 0.2 mM
solution, while those for Thd were similarly done with 2 mM Thd. Each
batch was placed in a 13 inch · 9 inch nonstick baking pan (Bradshaw
International, Rancho Cucamonga, CA) and frozen on two
25 cm · 25 cm dry ice slabs ()78.5ꢀC) placed side by side. During
freezing the pan was covered with a 15 inch · 10 inch Pyrex baking
dish; this minimizes frosting of the surface of the solution during the