Nucleic Acids Research Advance Access originally published online on March 6, 2007
Nucleic Acids Research 2007 35(6):1978-1991; doi:10.1093/nar/gkm025
Nucleic Acids Research, 2007, Vol. 35, No. 6 1978-1991
© 2007 The Author(s)
This is an Open Access article distributed under the terms of the Creative Commons Attribution Non-Commercial License (http://creativecommons.org/licenses/by-nc/2.0/uk/) which permits unrestricted non-commercial use, distribution, and reproduction in any medium, provided the original work is properly cited.
Biophysical studies of DNA modified with conformationally constrained nucleotides: comparison of 2'-exo (north) and 3'-exo (south) locked templates
Melissa Maderia1,
Shilpa Shenoy2,
Que N. Van3,
Victor E. Marquez1 and
Joseph J. Barchi, Jr1,*
1Laboratory of Medicinal Chemistry, Center for Cancer Research, National Cancer Institute at Frederick, Frederick, MD, 21702 USA, 2Molecular Targets Development Program and 3Laboratory of Proteomics and Analytical Technologies, SAIC-Frederick, Inc., Frederick, MD 21702 USA
*To whom correspondence should be addressed. Tel: +1 301 846 5905; Fax: +1 301 846 6033; Email: barchi{at}helix.nih.gov
Received November 16, 2006. Revised December 27, 2006. Accepted January 3, 2007.
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ABSTRACT
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The biophysical properties of oligodeoxyribonucleotides (ODNs)
selectively modified with conformationally locked
bicyclo[3.1.0]hexane pseudosugars (Maier,M.A., Choi,Y., Gaus,H.,
Barchi,J.J. Jr, Marquez,V.E., Manoharan,M. (2004) Synthesis
and characterization of oligonucleotides containing conformationally
constrained bicyclo[3.1.0]hexane pseudosugar analogs
Nucleic Acids Res., 32, 3642–3650) have been studied by various
techniques. Six separate synthetic ODNs based on the Dickerson
Drew dodecamer sequence (CGCGAAT*T*CGCG) were examined where
each one (or both) of the thymidines (T*) were substituted with
a bicyclic pseudosugar locked in either a
North (2'-
exo) or
South (3'-
exo) ring pucker. Circular dichroism spectroscopy,
differential scanning calorimetry and
1H NMR spectroscopy were
used to examine the duplex stability and conformational properties
of the ODNs. Replacement of one or both thymidines with North-locked
sugars (RNA-like) into the dodecamer did not greatly affect
duplex formation or melt temperatures but distinct differences
in thermodynamic parameters were observed. In contrast, incorporation
of
South-locked sugar derivatives that were predicted to stabilize
this standard B-DNA, had the unexpected effect of causing a
conformational equilibrium between different duplex forms at
specific strand and salt concentrations. Our data and those
of others suggest that although DNA can tolerate modifications
with RNA-like (North) nucleotides, a more complicated spectrum
of changes emerges with modifications restricted to South (DNA-like)
puckers.
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INTRODUCTION
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The design and construction of novel DNA oligomers with tunable
structural and hybridization properties have recently been the
topics of intense research interest. Nucleotide building blocks
with synthetic modification in either the furanose ring (
1)
or the nucleobase (
2) have been used for the design of novel
oligonucleotides (ONs) and oligodeoxyribonucleotides (ODNs).
Many of these constructs have been found to be useful biochemical
and pharmacological tools in antisense and antigene strategies.
Basic research in this area has produced an increasing number
of synthetically accessible nucleoside analogs and these building
blocks will continue to lead to new oligomers with exciting
biophysical and therapeutic features.
There are several structural features of ODNs that combine to form the characteristic global folds of DNA and RNA, including (a) base pair hydrogen bonding and stacking, (b) backbone torsion angle preferences and (c) the conformation of the ribo-or deoxyribofuranose ring. Regarding point (c), most nucleoside monomers exist in a dynamic equilibrium between two furanose puckering forms: The characteristic 3'-endo/2'-exo or North (N) and 2'-endo/3'-exo or South (S) ring conformations. When subjected to the constraints of an ODN duplex, the sugar rings adopt either of the two forms, B-DNA oligomers favoring S puckers while A-DNA and RNA favor N puckers. Furthermore, the crystal structures of enzymes involved in cellular nucleoside metabolism pathways in complex with their substrates reveal a distinct preference for a particular furanose pucker that is protein dependent. (3,4) Based on these findings, our laboratory (5–7) and others (8–11) have focused on the synthesis of novel nucleoside analogs that are biased toward one specific ring pucker as potential therapeutic agents. The concept of locking(12) the furanose ring pucker by various synthetic manipulations began about 13 years ago and gave rise to a range of different analogs (7,10,13,14). Notable examples in the field derive from the bridged nucleic acids (BNAs) concept (8), where analogs contain an added ring that bridges two atoms of the furanose. One of the most widely studied of these BNAs is one that contains a methylene bridge between the 2' oxygen and the 4' carbon that confers conformational restriction. These derivatives and ONs containing these monomers have been coined locked nucleic acids (LNAs) (15) since the conformation of the bicyclic furanose system is locked in the N quadrant of the pseudorotational cycle (16) (Figure 1). Extensive work has been carried out proving the added thermodynamic stability of LNA–RNA duplexes (17,18) as well as the triplex-forming ability of these constructs (19).

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Figure 1. Pseudorotational cycle for nucleoside furanose ring puckers. Ring puckers for standard nucleosides are typically either in the Northern or Southern hemispheres (illustrated by blue cones). Depictions of the N and S conventions along with the structure of an LNA monomer are shown. The pseudorotational positions for the N-MCT and S-MCT analogs are shown on the left half of the wheel.
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In 1993, our laboratory published the first synthesis of a locked
(dideoxy) nucleoside analog based on the carbocyclic bicyclo[3.1.0]hexane
(methanocarba (MC) nucleoside) systems (
7,
20) shown in
Figure 1.
An advantage of this system is that both
N- and
S-locked (
21)
platforms can be prepared by shifting the position of the fused
cyclopropane ring (
Figure 1). A range of nucleoside monomers
based on this template have been synthesized and used to query
the preferred substrate ring pucker of specific enzymes (
3,
22,
23).
In addition, a single-stranded DNA containing several
N-locked
MC thymidine (
N-MCT) units has also been shown to hybridize
efficiently with a complementary RNA strand (
20).
Based on the hybridization efficiency of many N-locked ONs with RNA, there is great therapeutic potential for synthetic ONs in antisense and antigene technologies where regulation of specific gene translation may slow or halt the progression of disease. Recent work has shown that ONs containing N-locked LNA units can substitute for small interfering RNAs (siRNAs) in the process of post-transcriptional gene silencing (24,25) adding to the usefulness of these analogs. In addition, binding of ODNs to proteins such as transcription factors often leads to structural adjustments in the helical parameters that may induce bends or kinks in the duplex. During bending of B-DNA, there is an obligatory adjustment of the sugar pucker from S toward N to relieve torsional and angular strain (26–28). The ability to pre-organize ONs/ODNs to specific global folds that mimic these adjustments may lead to surrogates that could perturb protein production at the level of transcription. Recent data from our lab suggests that the addition of bicyclo[3.1.0]hexane nucleoside analogs to a standard B-DNA duplex can cause bending toward the minor groove (29).
In order to gain a better understanding of how structural variations in the sugar moiety can contribute to both the local and global structural fold of ODNs, both S- and N-MCT analogs were inserted into a structurally well-characterized self-complementary B-DNA sequence (Dickerson Drew dodecamer, DD) known to contain only S-disposed sugar rings. The conformational and thermodynamic changes resulting from inserting either a single modified thymidine or two modified thymidine residues in positions 7 and/or 8 of the CGCGAAT*T*CGCG sequence is the subject of this work.
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MATERIALS AND METHODS
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Synthesis of modified DNA
Thymidine monomers containing the bicyclo[3.1.0]hexane system
were synthesized as described earlier (
30,
31) and incorporated
into the DD by procedures that required modification of the
coupling for the addition of the
N-monomers due to some unexpected
side reactions during the oligomer synthesis (
32). Samples were
purified by HPLC as described in (
32) and further purified by
EtOH precipitation. The precipitant was resuspended in water
and lyophilized three times, then taken up in 10 mM phosphate
buffer containing 0.1 mM EDTA and varying concentrations of
Na
+ (100, 500, or 1000 mM) at pH 7.0. DNA concentrations were
determined by measuring the UV absorbance at 260 nm and fitting
to Beer's Law using

= 110 700 l/mol · cm (Schepartz
Lab Biopolymer Calculator at
http://paris.chem.yale.edu/extinct.html).
The wild-type DD sequence was synthesized by the Laboratory
of Molecular Technology Oligonucleotide Synthesis core facility
at the NCI Frederick (Dr Leo Lee, Head, Frederick, Maryland).
Differential scanning calorimetry
Differential Scanning Calorimetry (DSC) data were acquired on a VP-DSC differential scanning calorimeter (Microcal, Inc., Northampton, MA). In a typical experiment, a 25–40 µM DNA (0.51 ml cell volume) solution was scanned from 10 to 90°C at a rate of 1°C/min. A 16-s filter period was used for all data acquisitions. A total of eight alternating scans (four up- and four down-scans) were recorded per experiment. A buffer versus buffer scan was obtained with 10 mM phosphate buffer containing 0.1 mM EDTA and NaCl (0.1, 0.5 or 1.0 M) placed in both of the calorimetric cells. This reference scan was subtracted from each corresponding experimental scan. The resulting thermogram was plotted as heat capacity (Cp) versus temperature. From the pre- and post-transition baselines, a cubic baseline was extrapolated under each melting transition. Values for Tm and
Hcal were obtained after baseline subtraction, and by fitting the thermograms to a two-state model, according to the manufacturer's protocols (OriginLab, Northampton, MA).
Cp was obtained as the difference between the pre- and post-transition baselines, prior to baseline subtraction, using a step at peak with no baseline subtraction. The Gibbs free energy of binding at 25°C (
Gb25) was derived from
Cp,
Hcal, and Tm values using the following equations (33)
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where
CT is total strand
concentration (29–40 µM) determined as described
above and
R is 1.987 cal/mol · K.
Tm and
T were in absolute
temperature values (K).
Scal was determined by taking the difference
between
Gb Tm and
Hcal at the
Tm.
Circular dichroism
Circular dichroism (CD) spectra were recorded on a JASCO J-715 spectrometer using a quartz cell with a 1-mm optical path length. Data were recorded in the range of 190–350 nm at 1.0 nm bandwidth, 100 mdeg of sensitivity, 0.1 nm resolution, 1 s response time, a speed of 50 nm/min and an average of two scans. A Haake D1 constant temperature bath interfaced to a Jasco controller was used to adjust the sample temperature between 5 and 65°C. Sample concentrations were 90–135 µM DNA in a total volume of 250 µl of phosphate buffer (pH 7.0), with varying concentrations of Na+.
NMR spectroscopy
1H NMR spectra were acquired on a Varian Inova spectrometer operating at 500 MHz using an inverse triple resonance Nalorac (IDTG) variable temperature probe with z-gradients. DNA concentrations for NMR studies were 2 mM, 0.2 mM or 0.04 mM for the modified DNA species and 0.9 mM for the wild-type dodecamer DNA in pH 7.0 phosphate buffer containing 100 mM Na+ and 10% D2O. One-dimensional spectra were acquired with 128 transients using the water macro from the Varian RNAPack suite of pulse sequences. Suppression of the H2O signal was performed with WATERGATE using a sinc shape for the 90° selective pulse on water. Spectra were acquired with a 12 000 Hz sweep width, an acquisition time of 2.7 s and a preacquisition delay of 1 s. Other parameters (power levels, offsets and pulse widths) were optimized for each individual sample. Spectra were acquired at intervals of 5°C from 5 to 65°C and were referenced to external 2,2-Dimethyl-2-silapentane-5-sulfonate sodium salt (DSS). Assignments of the imino protons were obtained by collecting standard COSY, TOCSY and NOESY spectra for each oligomer and using established ON sequential assignment techniques. The assignments were facilitated by comparison with spectra obtained for the wild-type DD. Raw NMR data were processed on a Sun Ultra10 440 MHz offline workstation using NMRPipe (34).
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RESULTS
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Six modified DD ODNs (
Figure 2) were synthesized and studied
by a variety of biophysical techniques. The self-complementary
single-stranded ODNs contained either an
N- or
S-MCT nucleotide
in either a single substitution at position T7 or T8, or a double
substitution at both positions T7 and T8. N and S superscripts
indicate the puckering of each thymidine substitution. After
annealing, the resulting double-stranded helix would have an
N- or
S-MCT at positions T7/T19 (designated T7
N or T7
S,
Figure 2),
T8/T20 (designated T8
N or T8
S) and T7,8/T19,20 (designated T7
NT8
N or T7
ST8
S) paired with normal 2'-deoxyadenosines. Our assumptions
were the following: The presence of one or two residues restricted
in the
South conformation in an all
South
DNA should, in effect, stabilize the duplex whereas perturbations
to the local and/or global duplex structure may result from
inclusion of nucleotides locked in the
North conformation.
Various experiments were conducted to address the following
questions: (
1) Do the
S-modifications help stabilize the duplex?
(
2) Do the
N-modifications prevent formation of a stable duplex?
(
3) If a duplex is formed, do these perturbations remain localized
to the site of modification? The following data supplied some
intriguing answers to these questions.

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Figure 2. Structures used in this study. The bicyclo [3.1.0] hexane nucleosides that were incorporated into the DNA are shown along with an illustration and nomenclature of the extra protons of these systems (in red).
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Circular dichroism
CD was used to qualitatively assess the conformations populated
by the ODNs in
Figure 2. To fully explore the duplex behavior
of the analogs, we performed CD measurements at several temperatures
and salt concentrations. The CD spectra of all ODNs exhibited
characteristics typical of B-type duplex DNA with some minor
differences (
Figure 3). Typical CD signatures for B-DNA include
a positive long wave (275–280 nm) band and negative shorter
wave (

250 nm) band of almost equal magnitude often followed
by a second zero cross-over point and a small negative band
at

210 nm (
35). In CD spectra of A-DNA and RNA, the long-wave
positive band shifts to lower wavelength and has significantly
higher magnitude than the short-wave negative band; a concomitant
increase in the negative band at 210 nm is also observed. The
native DD, T7
S, T8
S and T7
ST8
S all have typical B-DNA signatures
at 25°C (
Figure 3A) with the
S-modified ODNs displaying
higher magnitude negative bands at 210 nm. The significance
of this band with respect to the CD signatures of RNA and RNA-like
ODNs (A-DNA) has been under-appreciated according to some (
36)
but in our case it is difficult to evaluate since all modified
ODNs showed an increase in this band. Overall, except for the
negative band at 210 nm, the CD features of all the
S-modified
ODNs showed little change from the native DD. On the other hand,
the spectra of each of the
N-modified duplexes tend slightly
toward a more A-like signature as evidenced by the increased
magnitude and hypsochromic shift of the first positive band
as well as an increase in magnitude of the negative band at
210 nm. These features were shown to increase in the order T7
N 
T8
N < T7
NT8
N, with the double mutant showing the most significant
change in both positive and negative band magnitudes as well
as a more enhanced hypsochromic shift of the positive long-wavelength
band (
Figure 3B). The overall shape, cross-over points, wavelength
at maximum ellipticity change and band maxima are similar to
those shown previously for the DD (
37). Temperature-dependent
CD spectra also revealed that at temperatures above the
Tm,
the spectra acquired features that were reminiscent of other
single-stranded ODNs (data not shown).
Differential scanning calorimetry
DSC was used to understand the thermodynamic consequences resulting
from incorporation of the bicyclo[3.1.0]hexane-modified bases
into the DD. DSC provides an accurate measurement of the thermodynamic
quantities describing the melting or dissociation of DNA duplexes
such as the change in heat capacity (
Cp) that accompanies the
transition, the melting transition temperature (
Tm), and the
calorimetric enthalpy of dissociation (
Hcal). From these values,
the Gibbs free energy of binding (
Gb25) and the entropy of dissociation
(
Scal) can be derived. Previous studies of the native DD have
shown that increased concentrations of Na
+ ions lead to the
stabilization of a duplex structure, while at

10 mM Na
+ and
DNA concentrations

50 µM, a biphasic transition in the
melt curves was obtained with the tentative assignment of the
first intermediate as a hairpin loop structure (
37). Therefore,
the effect of Na
+ concentration was also examined. A summary
of the thermodynamic parameters calculated from the calorimetric
data is listed in
Table 1. An enthalpy–entropy compensation
plot (–
H versus –
T
S) showed a linear correlation
(
r2 = 0.99) and an observed slope of 1.14 (
Figure 4A). This
compensation demonstrated that the enthalpy and entropy terms
were approximately equal in magnitude for all the ODN species,
but that the enthalpies were favorable enough to offset the
unfavorable dissociation entropies, resulting in moderately
strong free energies of duplex formation for all ODN species
(
Table 1,
Figure 4B).
DSC of N-modified DDs
The thermodynamic properties of the native DD duplex in 100
mM Na
+ were consistent with those obtained earlier (
37). Incorporation
of either one or two
N-MCT units slightly destabilized the duplex
with
Tms of 60.7 to 62.9°C, while the
Tm of the native DNA
measured 65.3°C (
Table 1,
Figure 5). The T7
N DNA was the
most enthalpically stable species in that series with progressively
lower negative values of
Hcal for the T8
N and T7
NT8
N molecule,
respectively. In the case of T7
N, although its enthalpy of duplex
formation was almost 2-fold greater than that of the native
DD species, the accompanying entropy change was less favorable,
thereby yielding a comparable free energy change (
Gb25(native)
= –11.56 versus
Gb25(T7
N) = –12.33). Overall, the
thermodynamic data were relatively similar for the native and
N-modified species. The data indicated that stable duplexes
were formed upon incorporation of the
N-modified bases and that
only minor disruptions in conformation were produced by substituting
the central residues with RNA-like furanose surrogates.
As expected, at 0.5 M Na
+ an increase in the
Tm value of all
N-modified DNA species was observed. There was also an associated
increase in the calorimetric enthalpy and the change in heat
capacity, leading to a more stabilized DNA species in 0.5 M
Na
+ compared to 0.1 M Na
+. At 0.5 M Na
+, the native DNA was
slightly more stable (
Gb25 of –12.01 kcal) than the modified
DNA species (
Gb25 = –10.04 to –11.80). Increasing
the salt concentration to 1.0 M resulted in a concomitant increase
in the
Tm values for the DNA species (
Figure 5A–D). However,
the high salt concentration led to a paradoxical decrease in
the calorimetric enthalpy for the native DD back near the value
obtained at 0.1 M Na
+ with a compensating increase in entropic
stabilization. In addition, the change in heat capacity also
decreased for all species, particularly for the native, T7
N and T8
N species (
Figure 5A–C). Interestingly, the T7
N species seemed to be the most stable ODN overall and at all
salt concentrations. All DSC data were fit to a single transition
(two-state model) and reasonably low errors to the fit were
obtained. Data obtained earlier (
38) had postulated the presence
of a hairpin structure at low salt and DNA concentrations at
a
Tm higher than that of the duplex. Although we did not examine
the ODNs under these conditions, both the calorimetric and NMR
data (see below) obtained here did not indicate the presence
of any hairpin structures.
DSC of S-modified ODNs
As discussed above, there was nothing extraordinary in the CD data of the S-modified DDs and it was thought these analogs would stabilize the canonical, B-DNA duplex described previously for the DD. The most striking difference was in the melting behavior (Tm) of each duplex. Biphasic-type transitions were observed for all S-modified ODNs in standard duplex milieus (0.1 M Na+) where low melting species at temperatures between 30 and 36°C were observed followed by higher temperature transitions (Figure 6). In addition, these lower melting transitions were small with a decreased enthalpy of duplex dissociation on the order of 2–8 kcal/mol, almost 6-fold lower than that of the native DD. Interestingly, whereas biophysical measurements at varying strand concentrations of the N-modified ODN species did not alter the population of structures present (data not shown), the presence and stability of the low-melting species in the S-modified ODN species was concentration dependent. At concentrations that are typical for DSC (30–50 µM) or UV (1–10 µM) measurements, multiple species were observed. At higher concentrations that are standard in NMR spectroscopy of ODN species (1–2 mM), only the higher melting duplex form was observed (vide infra).
For all
S-modified ODNs, the second melting transitions all
had higher
Tm values than that of the native DD by at least
1.7°C (
Table 1,
Figure 6). These data suggested that inclusion
of the
S-modified base pairs into the DD stabilized the major
duplex conformation formed, although additional species were
present at equilibrium with incorporation of the
S-MCT nucleotides
into the strand. At higher salt concentrations (0.5 and 1.0
M NaCl) the higher melting transitions were enhanced dramatically,
evidently at the expense of the lower temperature transitions
which virtually disappeared. Hence, the calorimetric enthalpy
increased 4–10-fold by increasing the salt concentration
from 0.1 to 1.0 M Na
+ for each
S-modified species and as much
as 4-fold over the
Hcal of the native DD. In direct contrast
to the cooperative unfolding events of the
N-modified ODN species,
the melting transitions were broad for the
S-modified ODN species
at the 0.5 and 1.0 M Na
+. This suggested that multiple unfolding
intermediates were present. Given such broad transitions at
the 0.5 and 1.0 M Na
+, the derived melting temperatures most
probably reflected an average of multiple similar species melting
at or near the same
Tm value. Therefore, the
Tm values for the
S-modified ODNs appeared to remain fairly constant with increasing
salt, with the exception of the T7
ST8
S species which showed
a 4–5°C drop in
Tm from 0.1 to 1.0 M Na
+ concentrations.
As with the N-modified species, the duplex formation/dissociation of the South counterparts revealed an enthalpy–entropy compensation (Figure 4B). However, in the case of the T7ST8S species (in 0.5 and 1.0 M Na+; Table 1 and Figure 4B) greater entropy compensation resulted in a less favored
Gb25 of duplex formation as compared to the T7S or the T8S species. This suggested that the incorporation of the modified carbocyclic sugars in the T7ST8S may have caused perturbation of structure and prevented the proper annealing of the duplex. This finding was supported by NMR results where the T7ST8S imino protons showed larger chemical shift changes as compared to the other modified ODN species.
Nuclear magnetic resonance (NMR)
1H NMR: global melting of DNA
Proton NMR spectroscopy at variable temperatures was used to assess structural features and duplex stability of the modified ODN species. Assignments of imino protons and the entire proton network of all ODNs were determined based on standard 2D NMR data ((39) and Barchi and Maderia, unpublished results). At 5°C, each ODN from Figure 2 revealed all six imino protons (from base pairs G2, G4, T7, T8, G10 and G12) of those anticipated for a duplex formed from this self-complementary sequence (38,40), while warming to 25°C caused the imino proton assigned to G12 to fade, perhaps due to fraying at the end of the helix. All imino protons resonated between 12 and 14 ppm, chemical shifts that are indicative of duplex formation. Imino protons resonating in the 10–11 ppm range, which would serve as evidence for hairpin structures (40), were not observed at any temperature. Figures 7 and 8 show the temperature profiles of the imino resonances for the N- and S-modified ODNs, respectively. In general, trends for the disappearance of each proton followed those observed in previous studies of the DD (33). For example, the protons of base pairs closer to the ends of the duplex were only observed at low temperatures whereas those toward the center of the duplex persisted until close to the melting temperatures.

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Figure 7. NMR spectra of the imino 1H region of the N-MCT modified oligos at various temperatures. The assignments are as follows: filled diamond T8, filled square T7, filled triangle G2, circle G4, star G10 and double dagger, G12.
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Figure 8. NMR spectra of the imino 1H region of the S-MCT modified oligos at various temperatures. The assignments are as follows: filled diamond T8, filled square T7, filled triangle G2, filled circle G4, star G10 and double dagger, G12.
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1H chemical shifts: effect of temperature
Differences in
1H NMR chemical shifts are exquisite indicators
of structural/conformational changes. By monitoring the changes
in the chemical shifts (


) of the protons as a function of temperature,
information can be obtained about changes in the chemical environment
upon dissociation of the duplex. With increasing temperature,
the imino protons primarily shifted upfield and broadened (
Figures 7 and
8). In general, the T7 and T8 imino protons showed a larger
change in chemical shift from 5 to 65°C (


0.4 ppm for
N-ODNs;

0.8 for
S-ODNs) compared to the G2, G4 and G10 imino protons
(

0.15 ppm, for
N-ODNs and

0.4 ppm for
S-ODNs) which was consistent
with changes observed in the native DD. Non-exchangeable protons,
such as the H6 aromatic proton of thymidine and the T7 and T8
methyl protons, which are near the center of the duplex at the
site of modification exhibited less than 0.08 ppm changes in
chemical shifts as a function of temperature from 5 to 65°C
in both native and all six T-modified DNA species. This data
suggests that the global unfolding of the DNA was not greatly
affected by modification of the sugars of the thymidine residues.
1H chemical shifts: comparisons to native DD
At 5°C, the chemical shift of each imino proton of the native DNA was compared to those of the imino protons of each T-modified DNA species (Figure 9). Upon incorporation of an N-modified thymidine at position 7 (T7N), there was a difference of –0.40 ppm in the chemical shift of the T8 imino proton, but little differences (
< 0.1 ppm) were observed for other imino protons (Figure 9A). For the T8N DNA, there was a 
of –0.23 ppm in the chemical shift of T7 compared to the native imino proton as well as a +0.34 ppm difference for the
of the T8 imino proton. There were only slight changes in the chemical shifts of the guanosine imino protons (less than 0.1 ppm) in the T8N DNA. However, the double TN modification (T7NT8N ODN) showed changes in chemical shifts for the T7 and T8 imino protons that are similar to the native DD, with the largest difference in chemical shift assigned to the G10 imino proton at 
= 0.17 ppm. These same trends were also observed at 25°C (Figure 9B).
A contrasting picture emerged from the
S-modified oligos. For
the T7
S structure, at 5°C, the T7 imino proton experienced
a –0.42 ppm shift while for the T8 imino proton the shift
was only 0.08 ppm (
Figure 9A). For T8
S, very little change was
observed for most imino protons in contrast to the T8
N ODN which
showed both upfield and downfield changes for the T7 and T8
imino protons, respectively. The most startling change was seen
for the T7
ST8
S compared to its
N counterpart. Very little change
was observed in the


for T7
NT8
N ODN while the T7 imino proton
of T7
ST8
S shifted by greater than –0.8 ppm and T8 shifted
by –0.23 ppm relative to the native DD. The changes were
consistent from 5 to 25°C (
Figure 9A and B). Based on the
DSC data described above, this result is perhaps not surprising.
There seem to be extensive local structural rearrangements taking
place due to the presence of the modified nucleotides. These
may be due to accommodations made for the cyclopropane ring
of the modified carbocyclic sugar in the unusual 1'-O4' position
(see discussion).
Changes in the chemical shift of the non-exchangeable protons between the native DNA and those from the modified DNAs are shown in Figure 10. The local environment around the aromatic H6 proton and methyl group of the T7 residue in each N-modified ODN was slightly modified with the largest 
observed for the methyl group of the T8 residue in the T7N and T8N ODNs (–0.23 and –0.21 ppm, respectively, Figure 10A). Significant shifts were seen for the H6 protons of the T8 residue in both the T7N (–0.49 ppm) and T7NT8N (0.48 ppm) ODNs. For the S-MCT-modified structures, the T7S ODN displayed the largest change in chemical shift, and this occurred in the T8 residue: H6 and the CH3 group shifted by 0.22 and 0.18 ppm, respectively (Figure 10B). Interestingly, the double-modified duplex, T7ST8S, showed very little change in the chemical shifts of the aromatic protons, which suggested that the magnetic environment of this duplex was similar to that of the native DD. These changes were consistent with temperature (5–25°C, data not shown).
Concentration-dependent NMR of S-modified DNA
In an attempt to obtain more information regarding the various
transitions obtained from the DSC data of the
S-modified ODN
species, NMR spectra were collected at the concentrations used
to acquire the calorimetric data, i.e. 40 and 200 µM.
Interestingly, new peaks in the imino proton region of the spectra
were observed at these concentrations.
Figure 11 shows the imino
proton regions of the spectra for the T7
S (
Figure 11A) and T7
ST8
S (
Figure 11B) ODNs with the additional peaks indicated by arrows.
As before, there were no new resonances in any other region
of the spectra that may indicate hairpin structures. No attempt
was made to assign these new peaks to a particular structure,
but this information corroborated the observed DSC behavior
of the
S-modified DNA species at low single-strand concentrations.
As described above, when the DSC data was run at higher salt
concentrations which is known to stabilize duplexes, clean transitions
were observed at temperatures that were similar to the
Tm's
of the native DD. To confirm the presence of only one stable
species, NMR spectra of the actual lyophilized DSC samples of
the
S-modified DNAs at these salt concentrations were collected
at various temperatures. Resonances observed in the imino region
of the spectra (12–14) were similar to those observed
for the major species at other DNA and salt concentrations (not
shown).
 |
DISCUSSION
|
|---|
The bicyclo[3.1.0]hexane system has emerged as an extremely
useful template for the study of nucleosides and nucleic acids
with a rigidified five-membered ring employed as a surrogate
for a standard (deoxy)ribose system. In this article, we presented
several biophysical measurements on a series of Dickerson dodecamer
DNA sequences where one or two thymidines have been substituted
with nucleotides constructed on this template. The template
effectively locks the ring pucker of the fused cyclopentane
ring into either the Northern (
N) or Southern (
S) hemisphere
of the pseudorotational cycle. The concept of conformational
locking furanose rings in this manner has greatly
clarified many aspects of nucleoside and ON/ODN biochemistry
for a variety of systems (
21,
41–44). These data confirm
the utility of this template as a unique biochemical tool for
probing structure–activity relationships in ON biology.
Since the ribose rings of the native DD are puckered primarily in the standard B-type (S) conformation, it was anticipated that these substitutions may either stabilize or disrupt the local/global structure accordingly. Our thought experiment was to use the S-locked nucleotides as a control unit to stabilize an otherwise B-duplex by pre-organization of the proper sugar ring conformation prior to duplex formation. The N-type analogs were thought to disrupt the otherwise B-type helix and introduce a possible nucleation point for transmission of N-like conformational information along the sequence (45). Results from CD, NMR and DSC measurements all combined to paint a descriptive picture of the effect of either modified nucleoside on duplex formation and stability. As is shown here and in previous reports (46,47), the incorporation of N-locked analogs only minimally perturbed the DD system with regard to duplex formation and thermodynamics. However, we can now conclude that replacing the middle thymidine nucleotides with S-locked analogs leads to a more complex equilibrium of species rather than the idealized (and overly simplistic) assumption of an all B-DNA stabilization in a manner that was predicted a priori. The data has made the interpretation of the effects of incorporating the S-locked analogs significantly more difficult, especially in light of the concentration dependence of the aforementioned equilibrium. However, the major conformation formed was a duplex with a slightly higher thermodynamic stability compared to the native DD.
An encouraging conclusion to the data described here was that all of the modified ODN species can form stable duplexes under either standard conditions or with slightly elevated salt concentrations. Thus, incorporation of N-locked nucleotides into an otherwise B-DNA (S-puckered sugars) does not greatly affect duplex formation, at least for the constructs described here. In addition, although the sequence of the DD is self-complimentary and under certain conditions has a tendency to form hairpin structures (37), there was no indication of these folds for any of the ODN species studied. However, we have shown earlier that N-modified ODNs have a propensity to bend at the central residues more than the native DD (29). A recent detailed molecular modeling study of the three N-locked DNAs (48) was in solid agreement with the experimental results in (29). Hence, it may be surmised that along with their ability to form stable helices, these analogs serve to adjust the local structural environment (bend) in response to conformational restriction in the 2'-exo puckering regime.
The data described here suggests that incorporation of the S-modified nucleotides into the DD complicate the conformational equilibrium of the ODN species. These were designed to pre-organize a canonical, all B-DNA to a standard duplex fold. However, multiple transitions were observed at particular low salt and strand concentrations. We have not fully characterized the lower temperature transition from these ODN species but as suggested above, it is not a hairpin structure (49). NMR analysis showed that multiple species are present but they are limited to solutions that are of low micromolar strand concentrations at salt concentrations of 100 µM. At higher salt concentrations, these lower temperature melting species seem to be replaced solely by duplex structures that melt as broad transitions at a higher temperature and with a large change in
Hcal. The specific disposition of this duplex may be important to its characteristic change in heat capacity. It may be surmised that the S-modified nucleotides actually do stabilize a B-like helix and that the more hydrated environment associated with this type of helix requires a larger enthalpic change upon melting (see Table 1). Concomitantly, the melting of the putative well-ordered hydration sphere of this type of helix would be accompanied by an unfavorable entropic contribution (Table 1, Figure 4). The validity of these proposals may be supported by recalling that the modified nucleotides are carbocyclic in nature, lacking the 4'-oxygen atom that may be important for DNA hydration; disruption by intervening carbon atoms could lead to destabilization. Equally important is the presence of additional atoms in the modified templates which may differentially influence the steric environment around the fused cyclopropane. Figure 12 shows a comparison of the central base pairs of the DD highlighting the cyclopropane rings of the T7S and T8S and the potential steric clashes they may engender with neighboring H5', H5'' protons. These interactions could potentially cause adjustments in the backbone torsion angles that may serve to destabilize the initial folding of a stable helical conformation. In addition, both solid state and solution structural information on S-locked monomers (51,52) and DNA where an S-locked abasic site was incorporated (53) suggested that the rotamer distribution about the anomeric C-N bond (angle
) prefers a syn orientation rather than anti. Thus, it is perhaps not surprising that forcing a south conformation into the DD is not as well accommodated as a north-locked template. We may conclude that the S-modified ODNs resemble the native DD at low strand and Na+ concentrations; higher concentrations and additional salt is necessary to overcome thermodynamically unfavorable barriers and allow formation of highly stabilized duplexes.

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Figure 12. Side-by-side view of (A) T7ST8S (with residues labeled) and (B) the native dodecamer to illustrate the position and potential contacts of the additional atoms in the bicyclo[3.1.0]hexane systems compared to standard furanose rings. Only residues G4-T8 (3'-5') and C9-A5 (5'-3') are displayed for clarity. Backbone atoms are cyan; H5', H5'' of selected residues are dark blue; carbon and hydrogen atoms of the cyclopropane ring are shown in red and green, respectively.
|
|
The results obtained here for the
N-locked DNAs complement the
already highly studied systems of locked nucleic
acid oligomers constructed with the 2'–4' bridged bicyclic
nucleosides developed earlier (
8,
54). These constructs have
been employed as hybridizing partners with RNA to potentially
elicit a biological response akin to that of antigene therapy
(
8,55) or RNAi technology (
24). Similar hybridization with RNA
is achievable with the MCT ONs and it remains to be seen if
this technology could be used for gene silencing in a similar
manner or via other mechanisms. From our previous results that
showed that the T7
NT8
N system can induce bending in the DD (
29),
we feel it is conceptually possible to design ODNs with specific
bending properties that would mimic those induced by transcription
factor binding to particular DNA sequences. Hence, a judiciously
prepared
N-modified oligo may inhibit this binding through highly
specific substitution of the transcribing sequence. However,
this will require the high-resolution structural characterization
of each ODN separately to define the atomic coordinates of specific
modified sequences. Work in this area is currently in progress.
 |
ACKNOWLEDGEMENTS
|
|---|
We thank Professor Alex MacKerrell, University of Maryland,
Baltimore, for model structures of the DD and /S/-modified DNA
used for
Figure 12. This project has been funded in whole or
in part with federal funds from the National Cancer Institute,
National Institutes of Health, under contract N01-CO-12400.
The content of this publication does not necessarily reflect
the views or policies of the Department of Health and Human
Services, nor does mention of trade names, commercial products,
or organizations imply endorsement by the U.S. Government. This
Research was supported in part by the Intramural Research Program
of the NIH, National Cancer Institute, Center for Cancer Research.
Funding to pay the Open Access publication charge was also provided
under contract N01-CO-12400.
Conflict of interest statement. None declared.
 |
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