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1.
A constrained model building procedure is used to generate nucleic acid structures of the familiar A-, B-, and Z-DNA duplexes. Attention is focused upon the multiple structural solutions associated with the arrangements of nucleic acid base pairs rather than the optimum sugar-phosphate structure. The glycosyl (chi) and sugar torsions (both the ring puckering and the exocyclic C5'-C4' (psi) torsion) are treated as independent variables and the resulting O3'...O5' distances are used as closure determinants. When such distances conform to the known geometry of phosphate chemical bonding, an intervening phosphorus atom with correct C-O-P valence angles can be located. Four sequential torsion angles--phi', omega', omega and phi--about the C3'-O3'-P-O5'-C5' bonds are then obtained as dependent variables. The resulting structures are categorized in terms of conformation, ranked in potential energy, and analyzed for torsional correlations. The numerical results are quite interesting with implications regarding nucleic acid models constructed to fit less than ideal experimental data. The multiple solutions to the problem are useful for comprehending the conformational complexities of the local sugar-phosphate backbone and for understanding the transitions between different helical forms. According to these studies, unique characterization of a nucleic acid duplex involves more than the determination of its base pair morphology, its sugar puckering preferences, or its groove binding features.  相似文献   

2.
Abstract

In 3′,5′ deoxyribonucleoside diphosphates, in addition to the nature of the base and the sugar puckering, there are six single bond rotations. However, from the analysis of crystal structure data on the constituents of nucleic acids, only three rotational angles, that are about glycosyl bond, about C4′-C5′ and about C3′-O3′ bonds, are flexible. For a given sugar puckering and a base, potential energy calculations using non-bonded, electrostatic and torsional functions were carried out by varying the three torsion angles. The energies are represented as isopotential energy surfaces. Since the availability of the real-time color graphics, it is possible to analyse these isopotential energy surfaces. The calculations were carried out for C3′ exo and C3′ endo puckerings for deoxyribose and also for four bases. These calculations throw more light not only on the allowed regions for the three rotational angles but also on the relationships among them. The dependence of base and the puckering of the sugar on these rotational angles and thereby the flexibility of the 3′,5′ deoxyribonucleoside diphosphates is discussed. From our calculations, it is now possible to follow minimum energy path for interconversion among various conformers.  相似文献   

3.
Abstract

The nucleoside constituents of nucleic acids prefer the anti conformation (1). When the sugar pucker is taken into account the nucleosides prefer the C2′endo-anti conformation. Of the nearly 300 nucleosides known, about 250 are in the anti conformation and 50 are in the syn-conformation, i.e., anti to syn conformation is 5:1. The nucleotide building blocks of nucleic acids show the same trend as nucleosides. Both the deoxy-guanosine and ribo- guanosine residues in nucleosides and nucleotides prefer the syn-C2′endo conformation with an intra-molecular hydrogen bond (for nucleosides) between the O5′- H and the N3 of the base and, a few syn-C3′endo conformations are also observed. Evidence is presented for the occurrence of the C3′endo-syn conformation for guanines in mis-paired double helical right-handed structures with the distorted sugar phosphate C4′-C5′ and P-O5′ bonds respectively, from g+ (gg) and g- to trans. Evidence is also provided for guanosine nucleotides in left-handed double-helical (Z-DNA) oligo and polynucleotides which has the same syn-C3′endo conformation and the distorted backbone sugar-phosphate bonds (C4′-C5′ and P- O5′) as in the earlier right-handed case.  相似文献   

4.
Abstract

There are seven significantly variable torsion angles in each monomer unit of a polynucleotide. Because of this, it is computationally infeasible to consider the energetics of all conformations available to a nucleic acid without the use of simplifications. In this paper, we develop functions suggested by and regression fit to crystallographic data which allow three of these torsion angles, α (03′-P-05′-C5′), δ (C5′-C4′-C3′-03′) and ε (C4′-C3′-03′-P), to be calculated as dependent variables of those remaining. Using these functions, the seven independent torsions are reduced to four, a reduction in complexity sufficient to allow an examination of the global conformational energetics of a nucleic acid for the remaining independent torsion angles. These functions are the first to quantitatively relate a dependent nucleic acid torsion angle to several different independent angles. In all three cases the data are fit reasonably well, and in one case, α, the fit is exceptionally good, lending support for the suitability of the functions in conformational searches. In addition, an examination of the most significant terms in each of the correlation functions allows insight into the physical basis for the correlations.  相似文献   

5.
H Broch  D Vasilescu 《Biopolymers》1979,18(4):909-930
This paper reports a systematic PCILO study of the conformation of the nucleic acid backbone. The authors principally studied the ω′ and ω phosphodiester torsion angles of the disugar triphosphate model as a simultaneous function of (1) the sugar nature, ribose or deoxyribose, (2) the different combinations of the sugar ring puckers C(2′)-endo-C(2′)-endo, C(3′)-endo-C(3′)-endo, C(3′)-endo-C(2′)-endo, and C(2′)-endo-C(3′)-endo, and (3) the different conformations around the ψ(C4′–C5′) exocyclic bond. The dependence of the (ω′,ω) conformational energy maps upon these different factors, is discussed. The results are in very good agreement with the observed structures of ribonucleic (RNA10, RNA11, A′-RNA12, tRNAPhe) and deoxyribonucleic acids (D-DNA, C-DNA 9.3, B-DNA 10, A-DNA 11). Thus the validity of this model, the disugar triphosphate unit, is ensured. The main conclusions that can be drawn from this systematic study are the following:
  • 1 The torsion around P-05′ (angle ω) is, as a general rule, more flexible than the torsion around P-03′ (angle ω′).
  • 2 There is no notable difference between the ribose–triphosphate units and the deoxyribose–triphosphate units for the C(3′)-endo–C(3′)-endo and C(3′)-endo–C(2′)-endo sugar puckers.
  • 3 The deoxyribose–triphosphate units with C(2′)-endo–C(2′)-endo and C(2′)-endo–C(3′)-endo sugar puckers show much more ω′ flexibility than the ribose–triphosphate units with the same sugar puckers and cis position for the 2′hydroxyl group.
  • 4 The preferred values of ω′ are independent of the sugar nature (ribose or deoxyribose) and of ψ values; they are correlated with the sugar pucker of the first sugar-phosphate unit:
    • C(3′)-endo-C(3′)-endo and C(3′)-endo-C(2′)-endo puckers ? ω′ ? 240° (g? region)
    • C(2′)-endo-C(2′)-endo and C(2′)-endo-C(3′)-endo puckers ? ω′ 180° (t region)
  • 5 The preferred values of ω are independent of the nature and the puckering of the sugars; they are correlated with the rotational state of the torsion angle ψ(C4′–C5′): ψ ? 60° (gg) ? ω ? 300° (g?), ψ ? 180° (gt) or 300° (tg) ? ω ? 60° (g+)
  相似文献   

6.
Abstract

Utilizing a new method for modeling furanose pseudorotation (D. A Pearlman and S.-H. Kim, J. Biomol. Struct. Dyn. 3, 85 (1985)) and the empirical multiple correlations between nucleic acid torsion angles we derived in the previous report (D. A Pearlman and S.-H. Kim, previous paper in this issue), we have made an energetic examination of the entire conformational spaces available to two nucleic acid oligonucleotides: d(ApApApA) and ApApApA The energies are calculated using a semi-empirical potential function. From the resulting body of data, energy contour map pairs (one for the DNA molecule, one for the RNA structure) have been created for each of the 21 possible torsion angle pairs in a nucleotide repeating unit. Of the 21 pairs, 15 have not been reported previously. The contour plots are different from those made earlier in that for each point in a particular angle-angle plot, the remaining five variable torsion angles are rotated to the values which give a minimum energy at this point. The contour maps are overall quite consistent with the experimental distribution of oligonucleotide data. A number of these maps are of particular interest: δ (C5′-C4′-C3′-03′)χ (04′-C1′-N9- C4), where the energetic basis for an approximately linear δ-χ correlation can be seen; ζ (C3′- 03′-P-05′)-δ, in which the experimentally observed linear correlation between ζ and δ in DNA (220° < ζ <280°) is clearly predicted; ζ-ε (C4′-C3′-03′-P), which shows that e increases with decreasing ζ <260°; α (03′-P-05′-C5′)-γ (05′-C5′-C4′-C3′) where a clear linear correlation between these angles is also apparent, consistent with experiment; and several others. For the DNA molecule studied here, the sugar torsion Ô is predicted to be the most flexible, while for the RNA molecule, the greatest amount of flexibility is expected to reside in a and y. Both the DNA and RNA molecules are predicted to be highly polymorphic. Complete energy minimization has been performed on each of the minima found in the energy searches and the results further support this prediction. Possible pathways for B-form to A-form DNA interconversion suggested by the results of this study are discussed. The results of these calculations support use of the new sugar modeling technique and torsion angle correlations in future conformational studies of nucleic acids.  相似文献   

7.
A compilation of crystal structure data on deoxyribo- and ribonucleosides and their higher derivatives is presented. The aim of this paper is to highlight the flexibility of deoxyribose and ribose rings. So far, the conformational parameters of nucleic acids constituents of ribose and deoxyribose have not been analysed separately. This paper aims to correlate the conformational parameters with the nature and puckering of the sugar. Deoxyribose puckering occurs in the C2′ endo region while ribose puckering is observed both in the C3′ endo and C2′ endo regions. A few endocyclic and exocyclic bond angles depend on the puckering and the nature of the sugar. The majority of structures have an anti conformation about the glycosyl bond. There appears to be a puckering dependence on the torsion angle about the C4′C5′ bonds. Such stereochemical information is useful in model building studies of polynucleotides and nucleic acids.  相似文献   

8.
A uniform notation and convention is suggested to describe the torsional angles in nucleic acids and their derivatives. The torsional angle χ, relating the stereochemistry of the base with respect to the sugar, shows more variation for the β-purine glycosides than for the β-pyrimidine glycosides. This variation is attributed to the fact that the β-purine derivatives may form intramolecular O(5′)-H…N(3) hydrogen bonding. The χ values for the α-purine and α-pyrimidine glycosides show preference for the –syn-clinal (or anti) conformation. The mode of puckering of the sugar also influences the χ value. The various possible conformations for the furanose ring are described by the torsional angles τ0 τ1, τ2, τ3, τ4, about the five ring bonds. From an analysis of the torsional angles (ω, ?, ψ, ψ′, ?′, ω′) about the sugar phosphate bonds in the x-ray structures of the known nucleosides, nucleotides, phosphodiesters, nucleic acids, and related compounds, and from a consideration of molecular models, it is found that the possible conformations for the backbone of helical nucleic acids is strikingly limited. Most importantly, the preferred conformation of the nucleotide unit in poly nucleotides and nucleic acids turns out to be the same as that found for the nucleotide in the crystal structure. It is observed that base “stacking” is a consequence of the restricted backbone conformation. The torsional angles are illustrated in the form of conformational “wheels”. Interrelation between the torsion angles about successive pairs of sugar-phosphate bonds are presented in the form of conformational maps: ω,?; ?,ψ; ψ.ψ′; ψ′,?′; ?′,ω′; ω′,ω. The ω′,ω map shows the perferred conformations about the inter-nucleotide bonds of right- and left-handed helices and the possible conformations of phosphodiesters. The preferred conformation of the pyrophosphate and triphosphate is that in which the phosphate oxygens display a staggered arrangement when viewed along the P–P axis. A plausible structure and conformation for the ATPM2? backbound complex is presented. This structure differs from that proposed by SzentGyorgi in that the metal (only transition metals are considered here) is not bound to the NH2 nitrogen of adenine, but rather is simultaneously bound to N(7) of the ring and three phosphates (α, β, γ), or N(7) of the ring and two phosphates (β, γ). The remaining metal coordination may be satisfied by solvent–metal or enzyme–metal bonds.  相似文献   

9.
Solution structure of the nogalamycin-DNA complex   总被引:2,自引:0,他引:2  
X L Zhang  D J Patel 《Biochemistry》1990,29(40):9451-9466
The nogalamycin-d(A-G-C-A-T-G-C-T) complex (two drugs per duplex) has been generated in aqueous solution and its structure characterized by a combined application of two-dimensional NMR experiments and molecular dynamics calculations. Two equivalents of nogalamycin binds to the self-complementary octanucleotide duplex with retention of 2-fold symmetry in solution. We have assigned the proton resonances of nogalamycin and the d(A1-G2-C3-A4-T5-G6-C7-T8) duplex in the complex and identified the intermolecular proton-proton NOEs that define the alignment of the antitumor agent at its binding site on duplex DNA. The analysis was greatly aided by a large number of intermolecular NOEs involving exchangeable protons on both the nogalamycin and the DNA in the complex. The molecular dynamics calculations were guided by 274 intramolecular nucleic acid distance constraints, 90 intramolecular nogalamycin distance constraints, and 104 intermolecular distance constraints between nogalamycin and the nucleic acid protons in the complex. The aglycon chromophore intercalates at (C-A).(T-G) steps with the long axis of the aglycon approximately perpendicular to the long axis of the flanking C3.G6 and A4.T5 base pairs. The aglycon selectively stacks over T5 and G6 on the T5-G6-containing strand with the aglycon edge containing OH-4 and OH-6 substituents directed toward the C3-A4-containing strand. The C3.G6 and A4.T5 base pairs are intact but buckled at the intercalation site with a wedge-shaped alignment of C3 and A4 on the C3-A4 strand compared to the parallel alignment of T5 and G6 on the T5-G6 strand in the complex. The nogalose sugar in a chair conformation, the aglycon ring A in a half-chair conformation, and the COOCH3-10 side chain form a continuous domain that is sandwiched within the walls of the minor groove and spans the three base pair (G2-C3-A4).(T5-G6-C7) segment. The nogalose ring is positioned in the minor groove such that its nonpolar face is directed toward the G6-C7 sugar-phosphate backbone while its polar face containing OCH3 groups is directed toward the G2-C3 sugar-phosphate backbone in the complex. The intermolecular contacts include a nonpolar patch of aglycon (CH3-9) and nogalose (CH3-3') methyl groups forming van der Waals contacts with the base-sugar residues in the minor groove and intermolecular hydrogen bonds involving the amino groups of G2 and G6 with the ether oxygens OCH3-3' and O7, respectively, on the nogalose sugar.(ABSTRACT TRUNCATED AT 400 WORDS)  相似文献   

10.
yDNA is a base‐modified nucleic acid duplex containing size‐expanded nucleobases. Base‐modified nucleic acids could expand the genetic alphabet and thereby enhance the functional potential of DNA. Unrestrained 100 ns MD simulations were performed in explicit solvent on the yDNA NMR sequence [5′(yA T yA yA T yA T T yA T)2] and two modeled yDNA duplexes, [5′(yC yC G yC yC G G yC G G)2] and [(yT5′ G yT A yC yG C yA yG T3′)?(yA5′ C T C yG C G yT A yC A3′)]. The force field parameters for the yDNA bases were derived in consistent with the well‐established AMBER force field. Our results show that DNA backbone can withstand the stretched size of the bases retaining the Watson‐Crick base pairing in the duplexes. The duplexes retained their double helical structure throughout the simulations accommodating the strain due to expanded bases in the backbone torsion angles, sugar pucker and helical parameters. The effect of the benzo‐expansion is clearly reflected in the extended C1′‐C1′ distances and enlarged groove widths. The size expanded base modification leads to reduction in base pair twist resulting in larger overlapping area between the stacked bases, enhancing inter and intra strand stacking interactions in yDNA in comparison with BDNA. This geometry could favour enhanced interactions with the groove binders and DNA binding proteins., 2016. © 2015 Wiley Periodicals, Inc. Biopolymers 105: 55–64, 2016  相似文献   

11.
The potential energy calculations on the sugar-phosphate unit for different puckerings of the sugar are reported in this paper. The results obtained here essentially confirm our earlier predictions made by using criteria of contact distances (hard-sphere potential) and are also supported by observed conformation in crystal structures. The minimum energy conformations of the sugar phosphate unit, along with the preferred orientations of the base with respect to the sugar given in the previous paper, determine the probable conformations of the monomer unit of a polynucleotide (or nucleic acid) chain.  相似文献   

12.
D Hare  L Shapiro  D J Patel 《Biochemistry》1986,25(23):7445-7456
We report below on features of the three-dimensional structure of the d(C-G-T-G-A-A-T-T-C-G-C-G) self-complementary duplex (designated 12-mer GT) containing symmetrical G X T mismatches in the interior of the helix. The majority of the base and sugar protons in the 12-mer GT duplex were assigned by two-dimensional nuclear Overhauser effect (NOESY) spectra in H2O and D2O solution. A set of 92 short (less than 4.5-A) proton-proton distances defined by lower and upper bounds for one symmetrical half of the 12-mer GT duplex were estimated from NOESY data sets recorded as a function of mixing time. These experimental distances combined with nucleotide bond length parameters were embedded into Cartesian space; several trial structures were refined to minimize bond geometry and van der Waals and chirality error. Confidence in this approach is based on the similarity of the refined structures for the solution conformation of the 12-mer GT duplex. The G and T bases pair through two imino-carbonyl hydrogen bonds, and stacking is maintained between the G X T wobble pair and adjacent Watson-Crick G X C pairs. The experimental distance information is restricted to base and sugar protons, and hence structural features such as base pair overlap, glycosidic torsion angles, and sugar pucker are well-defined by this combination of NMR and distance geometry methods. By contrast, we are unable to define the torsion angles about the bonds C3'-O3'-P-O5'-C5'-C4' in the backbone of the nucleic acid.  相似文献   

13.
Abstract

The crystal structure of 5′-amino-5′-deoxyadenosine (5′-Am.dA) p-toluenesulfonate has been determined by X-ray crystallographic methods. It belongs to the orthorhombic space group P212121 with a=7.754(3)Å, b=8.065(l)Å and c=32.481(2)Å. This nucleoside shows a syn conformation about the glycosyl bond and C2′-endo-C3′-exo puckering for the ribose sugar. The orientation of N5′ atom is gauche-trans about the exocyclic C4′-C5′ bond. The amino nitrogen N5′ forms a trifurcated hydrogen bond with N3, O9T and 04′ atoms. Adenine bases form A.A.A triplets through hydrogen bonding between N6, N7 and N1 atoms of symmetry related nucleoside molecules.  相似文献   

14.
The two helical parameters n and h where n is the number of nucleotide residues per turn and h is the height per nucleotide residue have been evaluated for single stranded helical polynucleotide chains comprising C(3') -endo and C(2') endo class of nucleotides. The helical parameters are found to be especially sensitive to the C(4')-C(3') (sugar pucker) and the C(4')-C(5') torsions. The (n-h) plots display only one important helix forming domain for each class of nucleotides characterized by the sugar pucker and the C(4')-C(5') torsion. A correlation between the (n-h) plots and the known RNA (A,A') and DNA (A,B,C) helical forms has been established. It is found that all forms of helices except the C-DNA possess a favorable combination of P-O torsions. The analysis of the (n-h) plots suggests that C-DNA can have a conformation very similar to B-DNA. Although the (n-h) plots predict the stereochemical possibility of both right-handed and left-handed helices, nucleic acids apparently prefer right-handed conformation because of the energetics associated with the sugar-phosphate backbone and the base.  相似文献   

15.
Abstract

A new program, CONAN has been designed for CONformational ANalysis of oligonucleotide duplexes with natural and modified bases. It allows to model both regular DNA fragments with different types of symmetry and irregular ones including bends, junctions, mismatched pairs and base lesions. Computations and minimization of the energy are performed in a space of internal structural variables chosen to build start structure easier and conveniently analyze the results obtained. These internal structural variables determine mutual base-base and base-sugar arrangement and sugar puckering. The analytical closure procedure is applied both to sugar rings and to backbone fragments between adjacent sugars. For more effective energy minimization, analytical gradient is calculated. The CONAN was applied to the search for low-energy conformations of poly(dA-dT)·poly(dA-dT) and poly(dG-dC)·poly(dG-dC) duplexes. Extended regions of low-energy A and B conformations are revealed and characterized. These regions contain structures with different relative values of helical twist, τ, for pur-pyr and pyr-pur steps, namely, conformations with τ(pur-pyr)>τ(pyr-pur) and with τ(pur-pyr)<τ(pyr-pur). Two types of sugar puckering were found for B-form low-energy conformations, the first type with all C2′-endo sugar residues and the second one—;with C2′-endo purines and O1′-endo pyrimidines. The calculated conformations are compared with X-ray diffraction data for crystals and fibers and NMR data for solution.  相似文献   

16.
An oligonucleotide P3′?N5′ phosphoramidate (5′-amino-DNA) attracts much attention because of its potential for application to DNA sequencing; however, its ability to hybridize with complementary strands is low. To overcome this drawback of the 5′-amino-DNA, we have designed and successfully synthesized a novel nucleic acid analogue having a P3′?N5′ phosphoramidate linkage and a constrained sugar moiety, 5′-amino-3′-C,5′-N-methylene bridged nucleic acid (5′-amino-3′,5′-BNA). The binding affinity of the 5′-amino-3′,5′-BNA towards complementary DNA and RNA strands was investigated by UV melting experiments. The melting temperature (Tm) of the duplex comprising the 5′-amino-3′,5′-BNA and its complementary strand was much higher than that of the duplex containing the corresponding 5′-amino-DNA.  相似文献   

17.
Abstract

The solution distribution of combinations of the sugar ring puckering domains, C2′endo(S), C3′endo(N), and C4′-C5′ rotamers, +sc(g+), ap(t), -sc(g?), in α and β-anomers in ribo- and deoxyribo- pyrimidine nucleic acid components can be determined from vicinal coupling constants (M. Remin, J. Biomol. Str. Dyn. 2, 211 (1984). A general correlation pattern with a conformational constant λ, reflecting an intrinsic physical property of the sugar - side chain ensemble, is developed and expressed in terms of four principles:

I) The +sc rotamer contributes to the C3′endo population to a higher extent (1 - Yt) than to C2′endo,(l-Yt-Yg-/Xs).

II) The ap rotamer contributes to both C2′endo and C3′endo populations to the same extent (Yt).

III) The—sc rotamer contributes only to the C2′endo population, (Yg-/Xs).

IV) The molar fractions Xs, Yt and Yg- of conformations C2′endo, ap and—sc, respectively, are strongly correlated, λ = (Yg-/Xs)/Yt ≈ 0.5, and therefore Yt is a basic variable parameter which determines all others in the correlation pattern.

In α-anomers, regardless of the type and conformation of the sugar ring and base, the molar fraction Yt = 0.37 ± 0.02. This finding means that different α-anomers show one correlation pattern free of the influence of the base. In β-anomers, structure and conformation of the base are important factors which modulate (through Yt) the correlation pattern, conserving its fundamental features. Yt is considerably increased by a syn-oriented pyrimidine base, but decreases when the base is anti. The transition from anti to syn orientation of the base is followed by destabilization of (C2′endo, +sc) in favor of (C3′endo, ap). The principles of conformational correlations rationalize a variety of correlations observed in the past.  相似文献   

18.
D J Patel  L Shapiro  D Hare 《Biopolymers》1986,25(4):693-706
The base and sugar protons of the d(G-G-T-A-T-A-C-C) duplex have been assigned from two-dimensional correlated (COSY) and nuclear Overhauser effect (NOESY) measurements in D2O solution at 25°C. The nucleic acid protons have been assigned from NOEs between protons on adjacent bases on the same and partner strands, as well as from NOEs between the base protons and their own and 5′-flanking H1′, H2′, H2″, H3′, and H4′ sugar protons. These assignments are confirmed from coupling constant and NOE connectivities within the sugar protons of a given residue. Several of these NOEs exhibit directionality and demonstrate that the d(G-G-T-A-T-A-C-C) duplex is a right-handed helix. The relative magnitude of the NOEs between the base protons and the sugar H2′ protons of its own and 5′-flanking sugar demonstrate that the TATA segment of the d(G-G-T-A-T-A-C-C) duplex adopts a B-DNA type helix geometry in solution, in contrast to the previous observation of a A-type helix for the same octanucleotide duplex in the crystalline state.  相似文献   

19.
This paper reports on a combined two-dimensional NMR and energy minimization computational characterization of the conformation of the N-(deoxyguanosyl-8-yl)aminofluorene adduct [(AF)G] positioned across adenosine in a DNA oligomer duplex as a function of pH in aqueous solution. This study was undertaken on the d[C1-C2-A3-T4-C5-(AF)G6-C7-T8-A9-C10-C11].[G12-G13-T14 -A15-G16-A17-G18- A19-T20-G21-G22] complementary undecamer [(AF)G 11-mer duplex]. The modification of the single G6 on the pyrimidine-rich strand was accomplished by reaction of the oligonucleotide with N-acetoxy-2-(acetylamino)fluorene and subsequent deacetylation under alkaline conditions. The HPLC-purified modified strand was annealed with the unmodified purine-rich strand to generate the (AF)G 11-mer duplex. The exchangeable and nonexchangeable protons are well resolved and narrow in the NMR spectra of the (AF)G 11-mer duplex so that the base and the majority of sugar nucleic acid protons, as well as several aminofluorene ring protons, have been assigned following analysis of two-dimensional NOESY and COSY data sets at pH 6.9, 30 degrees C in H2O and D2O solution. The NOE distance constraints establish that the glycosidic torsion angle is syn at (AF)G6 and anti at A17, which results in the aminofluorene ring being positioned in the minor groove. A very large downfield shift is detected at the H2' sugar proton of (AF)G6 associated with the (AF)G6[syn].A17[anti] alignment in the (AF)G 11-mer duplex. The NMR parameters demonstrate formation of Watson-Crick C5.G18 and C7.G16 base pairs on either side of the (AF)G6[syn].A17[anti] modification site with the imino proton of G18 more stable to exchange than the imino proton of G16. Several nonexchangeable aminofluorene protons undergo large downfield shifts as do the imino and H8 protons of G16 on lowering of the pH from neutrality to acidic values for the (AF)G 11-mer duplex. Both the neutral and acidic pH conformations have been defined by assigning the NOE constraints in the [C5-(AF)G6-C7].[G16-A17-G18] segment centered about the modification site and incorporating them in distance constrained minimized potential energy calculations in torsion angle space with the DUPLEX program. A series of NOEs between the aminofluorene protons and the DNA sugar protons in the neutral pH conformation establish that the aminofluorene ring spans the minor groove and is directed toward the G16-A17-G18 sugar-phosphate backbone on the partner strand.(ABSTRACT TRUNCATED AT 400 WORDS)  相似文献   

20.
Abstract

Structural analysis of 3′-deoxycytidine and comparison with 2′-deoxynucleosides reveals no noticeable effect on the conformation of the molecule due to the lack of 3′-oxygen atom. There are two crystallographically independent molecules and both adopt the anti conformation with C3′-endo sugar puckering. A ‘head-to-tail’ packing of the molecules along the b axis results in a virtual ‘2′-5′ polycytidylic acid chain.  相似文献   

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