C O M M U N I C A T I O N S
Table 1. Thermodynamic Parameters for Complex Formationa
residues. Treatment of the duplex target with the bromide reagent
resulted in cleavage at essentially all of the dC residues of the dC8
target, but not those present in the duplex regions. After addition
of the W8K strand to the duplex, a second chemical probing
experiment indicated that none of the dC residues were susceptible
to cleavage (Supporting Information). This experiment indicates
that the W8K strand interacts with the dC8-target sequence as well
as with the T8-target sequence.
dC −W K
T −W K
WK triplex
8
8
8
8
8
∆H° (kcal/mol)
∆S° (cal/mol °K)
∆G°25 (kcal/mol)
-83.8 ( 0.5
-256 ( 2
-4.5 ( 0.4
-214 ( 2
-95.7 ( 1.9
-270 ( 6
-7.35 ( 0.07
-10.5 ( 0.1
-15.2 ( 0.3
19
KD
4.2 × 10-6
M
2.0 × 10-8
M
7.4 × 10-12
M
a Standard deviations reflect the reproducibilities of the van’t Hoff
analyses.
The orientation of the N- and C-termini of the W8K strand in
the three-stranded complex was determined by tethering a phenan-
throline residue to the N-terminus of the W8K strand. After addition
of CuSO4 and a thiol this reagent results in cleavage of DNA13 in
the vicinity of the Cu-phenanthroline. The results of this experiment
(Supporting Information) indicated that binding occurs with the
N-terminus oriented toward the 5′-terminus of the 11dC811 strand
(and toward the 3′-terminus of the 11T811 strand).
consistent with the gel shift data of Figure 2, which indicates that
formation of the dC8-W8K duplex is less favored than is the
formation of the T8-W8K duplex. The thermodynamic data indicate
differences in stabilities (∆∆G ∼ 3 kcal/mol). This difference may
reflect strand polarity. To form three interresidue H-bonds in the
dC8-W8K duplex, the dC8 strand must adopt the polarity that
appears to be less preferred (with the amino terminus of the W8K
strand oriented toward the 5′ terminus of the dC8 strand). The
formation of the triplex occurs with a ∆G°25 of -15.2 kcal/mol, a
value that is very similar to the sum of the ∆G°25 values for both
duplexes (-17.85 kcal/mol). This thermodynamic analysis confirms
that triplex formation by W8K occurs with binding to both of the
DNA target strands. Finally, the magnitude of the stabilization that
accompanies J-W triplex formation (absent competing W-C pairing)
is substantially greater than conventional DNA triplexes,16,17 or
hairpin triplexes18 of the same or in some cases longer-sequence
lengths.
The proposed J-W complex results from the W8K strand entering
the double-stranded complex through the major groove of the target
base pairs (see Figure 1a). An alternative binding mode would have
it enter through the minor groove. Since this initial study uses a
homopolymer and the acceptor/donor hydrogen bonding pattern for
the W-T interaction is symmetrical, the base pairing orientation
must be discerned on the basis of the interactions with the dC strand.
We prepared shorter (14-mer) target strands containing either a
central dC8 or d(C2isomC4C2) sequence. 5-Methyl-isocytidine
(isomC) should form three stabilizing hydrogen bonds with the W
residue if it enters from the minor groove, but should be destabilized
if oriented to enter from the major groove (Figure 3). We could
not prepare the fully substituted isomC8 due to acid depyrimidination
during assembly, although earlier work14 reported on the synthesis
of isomC10 sequences. While a mixture of the 8-mer dC8 the W8K
strand resulted in clearly definable A260 vs temperature transition,
and a Tm value of 23.3 °C,15 the d(C2isomC4C2) sequence gave no
discernible transition, suggesting destabilizing interactions between
the W and isomC residues. This experiment suggests that the type
of triplex formed is similar to that illustrated in Figure 1a with the
J-W strand entering from the major groove.
Experiments related to the second question regarding the ability
of related sequences to undergo strand invasion are presently under
study. The disruption of a Watson-Crick dA8‚dT8 target will require
an energetic cost of ∼7.1 kcal/mol20 with a remaining ∼8 kcal/
mol of stabilization energy. Effective strand invasion will likely
require sequences longer than 8-mers.
Acknowledgment. This work was supported by a grant from
the NIH (GM53201).
Supporting Information Available: Synthetic schemes and pro-
cedures, and a variety of gel and thermodynamic analyses (PDF). This
Thermal denaturation of the J-W triplex formed from the duplex
target of Figure 1b and the W8K strand resulted in two transitions
(Supporting Information). The midpoint of the first transition
occurred near 43 °C, while the midpoint of the second occurred
near 70 °C. The latter transition was present in the absence of the
W8K strand and is interpreted and reflecting the helix-to-coil
transition for the duplex target. The early transition then reflects
the J-W triplex to DNA duplex + W8K transition. Since these
transitions were clearly separated, it was possible to perform a van’t
Hoff analysis on a series of transitions obtained at varying total
concentrations and obtain thermodynamic parameters characterizing
the J-W triplex (Table 1).
We examined three different transitions involving the two 8-mer
duplexes dC8-W8K, T8-W8K, and the 11dC811-11T811-W8K
triplex. For the three complexes, ∆G values of -7.35, -10.5, and
-15.2 kcal/mol, respectively, were obtained. The ∆G°25 values for
the two duplexes and the corresponding calculated KD values are
References
(1) Moser, H. E.; Dervan, P. B. Science 1987, 238, 645-650.
(2) Francois, J. C.; Saison-Behmoaras, T.; Helene, C. Nucleic Acids Res. 1988,
16, 11431-11440.
(3) Cooney, M.; Czernuszewicz, G.; Postel, E. H.; Flint, S. J.; Hogan, M. E.
Science 1988, 241, 456-459.
(4) Griffin, L. C.; Dervan, P. B. Science 1989, 245, 967-971.
(5) Gianolio, D. A.; McLaughlin, L. W. Nucleosides Nucleotides 1999, 18,
1751-1769.
(6) Li, J.-S.; Fan, Y.-H.; Zhang, Y.; Marky, L. A.; Gold, B. J. Am. Chem.
Soc. 2003, 125, 2084-2093.
(7) Horne, D. A.; Dervan, P. B. J. Am. Chem. Soc. 1990, 112, 2435-2437.
(8) Jayasena, S. D.; Johnston, B. H. Nucleic Acids Res. 1992, 20, 5279-
5288.
(9) Gowers, D. M.; Fox, K. R. Nucleic Acids Res. 1999, 27, 1569-1577.
(10) Branda, N.; Kurz, G.; Lehn, J. M. Chem. Commun. 1996, 2443-2444.
(11) Nielsen, P. E.; Egholm, M.; Berg, R. H.; Buchardt, O. Science 1991, 254,
1497-1500.
(12) Ross, S. A.; Burrows, C. J. Nucleic Acids Res. 1996, 24, 5062-5063.
(13) Chen, C. H. B.; Sigman, D. S. J. Am. Chem. Soc. 1988, 110, 6570-
6572.
(14) Jurczyk, S.; Kodra, J. R.; Rozzell, J. D.; Benner, S. A.; Battersby, T. R.
HelV. Chim. Acta 1998, 81, 793-811.
(15) The Tm for the corresponding T8 duplex was 34.6 °C.
(16) Pilch, D. S.; Brousseau, R.; Shafer, R. H. Nucleic Acids Res. 1990, 18,
5743-5750.
(17) Singleton, S. F.; Dervan, P. B. J. Am. Chem. Soc. 1992, 114, 6957-
6965.
(18) Bervers, S.; Schutte, S.; McLaughlin, L. W. J. Am. Chem. Soc. 2000,
122, 5905-5915.
(19) KD values estimated from the measured ∆G°25 values.
(20) SantaLucia, J., Jr.; Allawi, H. T.; Seneviratne, P. A. Biochemistry 1996,
35, 3555-3562.
Figure 3. Destabilizing/missing H-bond interactions between W and isomC.
JA038081X
9
J. AM. CHEM. SOC. VOL. 126, NO. 1, 2004 71