Table 1 Thermal melting data (Tm) from UV–melting curves (260 nm) and free enthalpy of duplex formation from van’t Hoff plots of DNA or
RNA duplexes with the sequence indicated in Fig. 1
na
DNA Tm
RNA Tm
DG25uc (DNA)
DG25uc (RNA)
DDGd (DNA)
DDGd (RNA)
b
b
0
1
2
3
a
45.0
42.5
46.9
49.9
57.1
47.1
51.9
53.2
213.2
212.7
213.9
214.9
218.1
215.6
216.9
217.7
—
—
+0.5
21.2
21.0
b
+2.5
21.3
20.8
c
conditions: 10 mM NaH2PO4, 0.15 M NaCl, pH 7.0; Tm [uC], estimated error: ¡ 0.5 uC. Tm values at 1.2 mM. [ kcal mol21].
DDG 5 DGn+1 2 DGn.
d
to the unmodified duplex, the same situation in the RNA series is
still associated with a reduction in Tm by ca. 4 uC. It emerges,
however, that introduction of any Bph-pair after the first one
leads to a similar increase in thermal stability in both backbone
series, indicating a similar mode of interaction of the additional
hydrophobic pairs.
Table 2 Thermal melting data (Tm) from UV–melting curves (260 nm)
of DNA or RNA duplexes with one Bph-residue in a bulge position, or
of a DNA–RNA hybrid containing one Bph-pair
a
Tm
Entry Structure
Duplex
1
2
3
a
DNA bulge 59-d(GATGAC Bph GCTAG)-39 45.9 (45.0)
39-d(CTACTG’ 2 ‘CGATC)-59
RNA bulge 59-r(GAUGAC Bph GCUAG)-39 49.1 (57.1)
39-r(CUACUG’ 2 ‘CGAUC)-59
We measured CD spectra of the RNA duplexes in order to
screen for major changes in duplex structure upon introduction of
rBph-pairs (Fig. 2). As expected, the unmodified RNA duplex
shows the typical fingerprint of an A-conformation. Introduction
of one or three rBph-pairs does not significantly change this
pattern. The duplex with n 5 1 leads to a slight red shift of the
ellipticity maximum, which is not the case for the duplex with three
rBph-pairs and for the corresponding DNA duplexes.22 Thus
introduction of only one Bph-pair seems to be associated with a
more pronounced structural effect in the RNA series compared to
the DNA series.
DNA–RNA 59-d(GATGACBphGCTAG)-39
hybrid 39-r(CUACUGBphCGAUC)-59
conditions: c 5 1.2 mM in 10 mM NaH2PO4, 0.15 M NaCl,
36.1 (43.5)
pH 7.0. estimated error in Tm: ¡ 0.5 uC; in parenthesis: Tm data of
parent, non-modified duplex.
corresponds to L of the loss in Tm relative to a pure RNA duplex.
Thus we conclude that any accommodation of a Bph-residue in a
duplex that contains at least one RNA strand leads to reduced
thermal stability relative to a pure DNA duplex.
In order to determine the effect on duplex stability of a
hydrophobic residue in an internal bulge position, in DNA relative
to RNA and to determine the effect of one Bph-pair insertion into
a DNA–RNA hybrid, we measured the thermal stabilities of the
duplexes listed in Table 2. Introduction of a Bph-unit in a DNA
bulge stabilises the duplex relative to the unmodified duplex by
0.9 uC, while the same sequence arrangement in the RNA leads to
a destabilisation by 8.0 uC (Table 2, entries 1 and 2). The increase
in stability in the former case is an indication for intercalation
of the Bph-residue into the base-stack. In the case of RNA,
intercalation is either associated with a significant energetic penalty
or does not occur. The introduction of a complete Bph-pair into
a DNA–RNA hybrid (Table 2, entry 3) again leads to a decrease
in Tm, relative to the unmodified duplex, by 7.4 uC, which
It appears that interstrand stacking recognition of a single Bph-
pair is associated with a net penalty in free energy of duplex
formation of 2.0 kcal mol21 in RNA relative to DNA. A possible
explanation for this could lie in the different conformational
families (A vs. B) in which the geometry and the extent of overlap
of the aromatic units of both strands lead to less efficient stacking
in the case of RNA. Another reason could be the reduced
flexibility and dynamics of the RNA backbone relative to DNA.
Indeed, it has been shown before that classical aromatic inter-
calators tend to stabilise double stranded DNA more than RNA
duplexes.23 Along the same lines it was shown recently that an
oligodeoxynucleotide containing a covalently attached pyrenyl
intercalator, pairs preferentially to a DNA relative to an RNA
complement.24 In the context of more complex nucleic acid
structures it was also shown that the i-motif, consisting of pairwise
intercalated C–C+ nucleotide-pairs, is significantly more stable in
DNA as compared to RNA.25
In conclusion, the data presented here show that interstrand
intercalation of hydrophobic base-pairs that can adopt stabilities
of natural base-pairs in DNA, can be significantly less stable in
RNA duplexes or DNA–RNA hybrids.
These results are of interest in the following context. They
indicate that a hydrophobic base-pair that is not a shape mimic
of a natural base-pair, and that takes its interaction energy mainly
from interstrand stacking, may compromise the process of
transcription and translation due to significant changes in base–
base affinity, by changing from the DNA to the RNA backbone
and consequently from a B to an A-helical structure. Thus, this
finding is of importance for the future design of hydrophobic base-
pairs aiming at expanding the genetic alphabet. Furthermore, the
fact that an additional hydrophobic base in a bulge position within
Fig. 2 CD spectra of RNA-duplexes from Table 1 (n 5 0, 1, 3), c 5
3.6 mM, in 10 mM NaH2PO4, 0.15 M NaCl, pH 7.0, T 5 20 uC.
2024 | Chem. Commun., 2005, 2023–2025
This journal is ß The Royal Society of Chemistry 2005