Fig. 2 Plot of variation of Tm3?2 and Tm2?1 of poly(dA)·2poly(dT) as a
function of increasing pyrene–neomycin and neomycin concentrations.
Solution conditions: same as Fig. 1.
Fig. 4 Pyrene–neomycin docked in the Watson–Hoogsteen groove of a TAT
DNA triplex. (Atom colors: pyrene–neomycin; purple: poly(dA); white:
poly(dT); green: poly(dT)—the third strand.)
triplex melts at 32 °C. In the presence of 4 mM neomycin and 4
mM pyrene–neomycin, triplex Tm rises to 43 and 58 °C,
respectively. These results show that pyrene–neomycin can
stabilize the triplex much more effectively than neomycin at
these low concentrations (rdb = 0.26). This is quite remarkable
since pyrene itself is not a good triplex stabilizer. Addition of 4
mM 1-aminopyrene and 4 mM neomycin to a DNA triplex leads
to a small DTm3?2 increase (a biphasic transition, Fig. 1c, Fig.
2). Covalent attachment of the two yields a single transition
with a DTm about 10 °C higher than the sum of the two (added
together). With all three ligands, duplex melting points were
unchanged (71°C), signifying that both neomycin and pyrene–
neomycin (at these concentrations) have no effect on the
stabilization of this DNA duplex. At higher pyrene–neomycin
concentrations, a larger increase in Tm is observed, but the
DDTm values (from neomycin) do not increase significantly,
suggesting saturation of the drug binding site at rdb ~ 0.13.
A slightly different picture emerges with the RNA triplex.
DTm plots of poly(rA)·2poly(rU) with different ligands,
1-aminopyrene, pyrene–neomycin, and neomycin from 0–4 mM
concentration are shown in Fig. 3. Without any ligand, Tm3?2
is 32 °C; while in the presence of 4 mM pyrene–neomycin,
Tm3?2 rises to 41 °C and Tm2?1 rises from 49 to 55 °C.
Pyrene–neomycin then stabilizes RNA triplex as well as the
duplex, but the DTm3?2 values are slightly less than those
induced by neomycin. Duplex stabilization by both ligands is,
however, quite comparable. The inability of pyrene to inter-
calate/stabilize an RNA triplex is perhaps responsible for this
lower stabilization observed with the conjugate (1-aminopyrene
has no effect on the RNA duplex/triplex, Fig. 3). Appropriately
designed conjugates could then, in principle, be made to
differentiate such higher order DNA/RNA nucleic acid struc-
tures, and help us explore the structural variations responsible
for their recognition.
Computer modeling of pyrene–neomycin docked in a TAT
triplex suggests that pyrene can intercalate between the base
pairs while neomycin stays bound to the Watson–Hoogsteen
groove (Fig. 4). Ring I may be embedded inside the groove with
amino groups H-bonded to the anti-parallel T strand, whereas
the ribose can provide the optimum conformation and size for a
good fit into the triplex groove. Rings I and IV are responsible
for bringing the two pyrimidine strands together. Because of
this possible dual binding mode of triplex recognition, pyrene–
neomycin conjugate shows significant ability to stabilize DNA
triple helices. Such chromophores should then be effective
model ligands for surveying the groove recognition properties
of a triplex bound neomycin. These results are now being
extended to the stabilization of mixed sequences/hybrid struc-
tures and will be reported in due course.
Financial support for the work was provided by Clemson
University and Greenville Hospital System. The support of
NMR facility by NSF grant (CHE-9700278) is gratefully
acknowledged. We thank Dr Ljiljana Micovic for help with
modeling studies.
Notes and references
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Fig. 3 Plot of variation of Tm3?2 and Tm2?1 of poly(rA)·2poly(rU) as a
function of pyrene–neomycin and neomycin. 10 mM sodium cacodylate,
0.1 mM EDTA, pH 6.8. (a) Triplex + neomycin, (b) triplex + pyrene–
neomycin, (c) duplex + pyrene–neomycin, (d) duplex + neomycin, (e)
triplex + 1-aminopyrene, (f) duplex + 1-aminopyrene. [RNA] = 30 mM
base triplet.
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CHEM. COMMUN., 2002, 70–71
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