The A and B conformations of DNA and RNA subunits. Potential energy calculations for dGpdC

In order to obtain a molecular picture of the A and B forms of a DNA subunit, potential energy calculations have been made for dGpdC with C(3′)-endo and C(2′)-endo [or C(3′)-exo] sugar puckerings. These are compared with results for GpC. The global minima for dGpdC and GpC are almost identical. They are like A-form duplex DNA and RNA, respectively, with bases anti, the ω′, ω angle pair near 300°, 280°, and sugar pucker C(3′)-endo. For dGpdC, a B-form helical conformer, with sugar pucker C(2′)-endo and ω′ = 257°, ω = 298°, is found only 0.4 kcal/mol above the global minimum. A second low-energy conformation (2.3 kcal/mol) has ω′ = 263°, ω = 158° and ψ near 180°. This has dihedral angles like the original Watson–Crick model of the double helix. In contrast, for GpC, the C(2′)-endo B form is 6.9 kcal/mol above the global minimum. These theoretical results are consistent with experimental studies on DNA and RNA fibers. DNA fibers exist in both A and B forms, while RNA fibers generally assume only the A form. A low-energy conformation unlike the A or B forms was found for both dGpdC and GpC when the sugars were C(3′)-endo. This conformation—ω′,ω near 20°,80°—was not observed for C(2′)-endo dGpdC. Energy surface maps in the ω′,ω plane showed that C(2′)-endo dGpdC has one low-energy valley. It is in the B-form helical region (ω′ ～ 260°, ω ～ 300). When the sugar pucker is C(3′)-endo, dGpdC has two low-energy regions: the A-form helical region and the region with the minimum at ω′ = 16°, ω = 85°.     

Examination by the molecular orbital method of the intrinsic conformation preferences of nucleic acid sequence]

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, tRNA^Phe) 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⁺)

     

Conformational characteristics of the RNA subunit ApA from energy minimization studies

In an attempt to better our understanding of the conformational stabilities in RNAs, an intensive theoraticl study has been carried out on one of its dimeric subunits, ApA, using an improved set of atom-atom interaction energy parameters and an improved version of energy-minimization technique. The C(3′)0endo and the C(2′)-endo sugar ApA units were sperately considered and 38 probable conformations have been analyzed in each case. The total potential energy, comprising nonbonded, electrostatic, and torsional contributions, was minimized by varying all seven relevant dihedral angles simumtaneously. The result reveal that 17 conformations in the case of C(3′)-endo sugar ApA and 7 confomations in the case of C(2′)-endo sugar ApA unit, the lowest energy conformation corresponds to a nonhelical structure and the A-RNA and the Watson-Crick-yype conformations lie at energy levels of about 0.5 and 1.0 Kcal/mo., respectively, above the lowest energy found. For ApA with the lops of different types in the backbone and they all differ in energies by about 3.5 Kcal/mol with refrence to the lowest energy founs. It is noted that the order ofmprefrence of the base stacking is observed in the A-RNA and the Watson-Crick type conformers. The ApA unit with C(2′)-endo sugar is forced to assume phosphodiester conformations with large deviations fom the expected staggered conformations compared to the ApA unit with C(3′)-endo sugar. The result obtained for ApA are discussed with refrence to those previously obtained for the dApdA unit. Te theoretical predictions are compared with the experimental data on the tRNA^Phe crystal, as well as those on fibrous RNAs and RNa subunitlike crystal structures. This study brings out many important aspects of the conformational stability of ApA which have been missed by studies made by others on this system.     

Conformational studies on polynucleotide chains. V. A comparison between the quantum-mechanical and the consistent force field approach

Consistent force field (CFF) calculations were performed for the sugar–phosphate–sugar fragment, taken as a model of the polynucleotide backbone. The potential-energy-function is the sum of four contributions, accounting for bond and angle deformation, torsional motions, and nonbonded interactions. Both deoxyribose and ribose systems, with either C(2′)-endo or C(3′)-endo puckering in the starting geometry of ribose rings, were considered. A fair number of minima of the conformational-energy hypersurface were found. Although the numerical method employed in the CFF context cannot solve the problem of finding the global minimum in a definite way, one of the final conformations has a total energy much more attractive than the others, and may be regarded as the most stable conformation attainable with our potential-energy function. The energy-minimization affects the puckering of the first ribose ring differently from that of the second: in general, for the C(2′)-endo system the second ring retains its starting conformation (Ψ′ = 152°), while in the first the Ψ′ is modified by up to 70°; the opposite occurs for the C(3′)-endo system. This is explained by the different positions of the two rings relative to the phosphate group.     

Correlation between the backbone and side chain conformations in 5′-nucleotides. The concept of a ‘rigid’ nucleotide conformation

Conformational energies of the 5′-adenosine monophosphate have been computed as a function of χ and ψ, of the torsion angles about the side-chain glycosyl C(1′)–N(9) and of the main-chain exocyclic C(4′)–C(5′) bonds by considering nonbonded, torsion, and electrostatic interactions. The two primary modes of sugar puckering, namely, C(2′)-endo and C(3′)-endo have been considered. The results indicate that there is a striking correlation between the conformations about the side-chain glyocsyl bond and the backbone C(4′)–C(5′) bond of the nucleotide unit. It is found that the anti and the Gauche–Gauche (gg), conformations about the glycosyl and the C(4′)–C(5′) bonds, respectively, are energetically the most favored conformations for 5′-adenine nucleotide irrespective of whether the puckering of the ribose is C(2′)-endo or C(3′)-endo. Calculations have also shown that the other common 5′-pyrimidine nucleotides will show similar preferences for the glycosyl and C(4′)–C(5′) bond conformations. These results are in remarkable agreement with the concept of the “rigid” nucleotide unit that has been developed from available data on mononucleotides and dinucleoside monophosphates. It is found that the conformational ‘rigidity’ in 5′-nucleotides compared with that of nucleosides is a consequence of, predominantly, the coulombic interactions between the negatively charged phosphate group and the base. The above result permits one to consider polynucleotide conformations in terms of a “rigid” C(2′)-endo or C(3′)-endo nucleotide unit with the major conformational changes being brought about by rotations about the P–O bonds linking the internucleotide phosphorus atom. IT is predicted that the anti and the gg conformations about the glycosyl and the C(4′)–C(5′) bonds would be strongly preferred in the mononucleotide components of different purine and pyrimidine coenzymes and also in the nucleotide phosphates like adenodine di- and triphosphates.     

Conformational study of trinucleoside tetraphosphate d(pCpGpCp): Transition of right-handed form to left-handed form

Using the semiempirical potential functions, conformational energies of the model compounds DMP^?, d(pCp), d(pGp), and d(pCpGpCp) are calculated, and the B → Z transition is discussed along the pseudorotational path of the sugar ring. For dimethylmonophosphate anion, DMP^?, the energy contour map is presented and the stabilities of the phosphodiester conformations discussed. For the sugar ring without the base attached, the minimum energies for each sugar-puckering form are calculated along the pseudorotational path. The energy barrier of the interconversion between the C(3′)-endo form and the C(2′)-endo form is calculated to be about 2.0 kcal/mol. From the conformational energy calculations of the interconversions of mononucleoside diphosphates, d(pCp) and d(pGp), between the C(2′)-endo conformer and the C(3′)-endo conformer, the purine sugar segment is known to be more convertible than the pyrimidine sugar segment. The results also support the finding that the pseudorotational transition occurred with the O(1′)-endo form more easily than with the O(1′)-exo form. Based on the results of conformational studies of DMP^?, d(pCp), and d(pGp), a topological transition of the handedness of the model compound, d(pCpGpCp), is studied. The left-handed Z-form is found to be less stable by about 8.5 kcal/mol than is the right-handed B-form. The energy barrier of the Z → B transition is calculated to be about 17.4 kcal/mol. The contributions of the electrostatic and nonbonded energies to the energy barrier are discussed in connection with the conformation changes of the model compound, d(pCpGpCp).     

Conformational characteristics of the trinucleoside diphosphate d(ApApA) from energy-minimization studies

Energy-minimization studies were carried out on the trinucleoside diphosphate d(ApApA). The potential energy contributions from nonbonded, electrostatic, hydrogen-bonding, and torsional interactions were minimized by treating the 13 relevant dihedral angles as simultaneous variables. For the C(3′)-endo trimer, 14 low-energy conformations are within 10 kcal/mol above the lowest energy found, compared to only 3 in the case of the C(2′)-endo trimer. This result shows the flexible character of the C(3′)-endo unit. The hairpin-type, loop-promoting conformer with (ω′,ω) = (101°, 59°) was found to be the most favored structure at the 3′-terminus of d(ApApA). The predicted U- and L-type bend conformers were found to lie within 5 kcal/mol, compared to the lowest energy B-DNA structure. The A-DNA and Watson-Crick DNA types of helical conformers also lie within very small energy barriers. The phosphate group at the 5′-end of the nucleotide residue has a definite influence on the base of the corresponding nucleotide, keeping it in the normal anti-region, and hence on the base-stacking property. The results are compared with the presently available experimental data, mainly with the tRNA^Phe crystal.     

Conformational characteristics of dApdA,dApdT, dTpdA,and dTpdT from energy minimization studies

The conformational characteristics of the deoxydinucleoside monophosphates with adenine and thymine bases in all possible sequences, namely, dApdA, dApdT, dTpdA, and dTpdT have been studied using an improved set of energy parameters to calculate the total potential energy and an improved set of energy parameters to calculate the total potential energy and an improved version of the minimization technique to minimize the total energy by allowing all seven dihedral angles of the molecular fragment to vary simultaneously. The results reveal that the most preferred conformation in all these units usually corresponds to one of the four helical conformations, namely, the A-DNA, B-DNA, C-DNA, and Watson-Crick DNA models. These helical conformations differ in energies by about 3 kcal/mol with respect to one another. The conformations which could promote a loop or bend in the backbone are, in general, less stable by about 3.5 kcal/mol with respect to the respective lowest-energy helical conformation. The results indicate that there is a definite influence of bases and their actual sequences on the preferred conformations of the deoxydinucleoside monophosphates. The lowest-energy structure, although corresponding to one of the four helical conformations, differ with the type of the deoxydinucleoside monophosphate. Good or reasonable base stacking is noted in dApdA and dTpdA with both C(3′)-endo and C(2′)-endo sugars and in dApdT and dTpdT with only C(3′)-endo sugar. The inversion of the base sequence in deoxydinucleoside monophosphates alters the order of preference of low-energy conformations as well as the base-stacking property of the unit. The paths linking the starting and final states in the (ω′, ω) plane show interesting features with regard to the energy spread, thus providing insight into the path of conformational movement ofthe molecule under slight perturbation. The stabilities of the A and B forms, including the internal energies of the C(3′)-endo ans C(2′)-endo sugar systems, indicate that for dTpdT the B → A transition is less probable. For dApdA, dApdT, and dTpdA this transition is probable in the same order of preference. We propose that the T-A sequence in the polynucleotide chain might serve as the site accessible for B ? A transitions. The theoretical predictions are in good agreement with the experimental observations.     

Conformational studies on polynucleotide chains. I. Hartree-fock energies and description of nonbonded interactions with Lennard-Jones potentials

The sugar–phosphate–sugar complex C₁₀H₁₈O₈P, a unit of the polynucleotide chains, was analyzed, making use of 100 conformational energies computed in the Hartree-Fock approximation with a small basis set of Gaussian type orbitals. The geometry of the conformations [which corresponds to the C(2′)-endo deoxy system], the basis set, and the computed total energies are reported in this work. In addition, a number of attempts are presented where we searched for a computationally very simple analytical expression apt to fit, with reasonable accuracy, the computed energies. Lennard-Jones type potential seems to offer an appropriate form capable of reproducing the positions of the maxima and the minima resulting from ab initio computations, but neither the 6-12 nor other similar forms seem to be able to correctly reproduce the intensity of the barriers. Form a details analysis of the barriers to rotation about the bonds O(5′)—C(5′) and C(5′)—C(4′) in terms of nonboned interactions, we found that a substantial improvement in the fit of analytical to ab initio energies may be obtained by distinguishing between atoms characterized by the same atomic number but having different chemical characteristics, like the oxygen atoms of the phosphate group, on one hand, and the oxygen atoms of the sugar rings and the hydroxyl groups, on the other.     

Conformations of cyclic 2,3-nucleotides and 2,3-Cyclic-5-diphosphates. Interrelation between the phase angle of pseudorotation of the sugar and the torsions about the glycosyl C(1)-N and the backbone C(4)-C(5) bonds

Semiempirical potential energy calculations have been carried out for cyclic 2′,3′-nucleotides and their 5′-phosphorylated derivatives, which are the intermediates in the hydrolysis of RNA. Calculations have been performed for both purine and pyrimidine bases for the observed O(1′)-endo, O(1′)-exo and the unpuckered planar sugar ring conformations. It is found that the mode of sugar pucker largely determines the preferred conformations of these molecules. For cyclic 2′,3′-nucleotides themselves, the O(1′)-endo sugars show a preference for the syn glycosyl conformation while the O(1′)-exo sugars exclusively favor the anti conformation regardless of whether the base is a purine or pyrimidine. For the unpuckered planar sugar, the syn conformation is favored for purines and anti for pyrimidines. Both the gauche (+) (60°) and trans (180°) conformations about the C(4′)? C(5′) bond are favored for O(1′)-endo sugars, while the gauche (?) (300°) and trans (180°) are favored for O(1′)-exo sugars. On the contrary, the 5′-phosphorylated cyclic 2′,3′-nucleotides of both purines and pyrimidines show a preference for the anti-gauche (+) conformational combination about the glycosyl and C(4′)? C(5′) bonds for the O(1′)-endo sugars and the anti-trans combination for the O(1′)-exo sugars. The correlation between the phase angle of the sugar ring and the favored torsions about the glycosyl and the backbone C(4′)? C(5′) bonds as one traverses along the pseudorotational pathway of the sugar ring is examined.     

Interaction of molecules with nucleic acids. II. Two pairs of families of intercalation sites, unwinding angles, and the neighbor-exclusion principle

Intercalation-site geometries are generated for a tetramer duplex extracted from B-DNA. Glycosidic angles and puckers of the deoxyribose sugar groups bonded to base pairs BP₁ and BP₄, namely, those at either end of the tetramer duplex, are assumed to be those of B-DNA to insure continuity. All possible geometrical conformations for combinations of C(2′)-endo, C(3′)-endo, C(2′)-exo, and C(3′)-exo sugar puckers are determined for the tetranucleotide backbone. Those with minimum energy are selected as candidates for intercalation sites. Calculations reveal two pairs of physically meaningful families of intercalation sites which occur in two distinct regions, I and II, of helical angles which orient BP₂ relative to BP₃ and with the helical axis disjointed between these base pairs. For each site I and II within BP₂ and BP₃, there are two distinct backbone conformations, A and B, connecting BP₃ to BP₄ or BP₁ to BP₂ which do not disrupt backbone conformations connecting BP₂ to BP₃. Hence two pairs, IA and IB, and IIA and IIB, of intercalation sites exist in which the sugar puckers along the backbone of the tetramer alternate from C(2′)-endo to C(3′)-endo on the backbone (5′p3′) connecting BP₂ to BP₃. The glycosidic angles of the C(3′)-endo sugar χ₃^γ are, coincidentally, 80° ± 2° for both conformations γ = A and B connecting BP₃ to BP₄ along the phosphate backbone (5′p3′). Consistent with the theoretical results, the experimental unwinding angles can be grouped into two categories with absolute values of 18° and 26°. The theoretical unwinding angles for sites IA and IB of 16° and for sites IIA and IIB of 20° occur for a displacement of -0.8 Å in the helical axes of BP₂ and BP₃ and for a 100% G·C composition, with a decrease depending on the amount of A·T base pairs present. Ratios of theoretical unwinding angles of sites I and II, which range from 0.75 to 0.84 for the two principal sites, compare well with the experimental value of 0.71. The theoretical results, in agreement with experimental observation, provide a new interpretation of the nature and conformation of the possible binding sites. Conformations obtained from these studies of intercalation sites in a tetramer duplex are used to rationalize the well-known neighbor-exclusion principle. The possibility of violation of this principle is demonstrated by the existence of two families of physically meaningful conformations. Conformations of unconstrained dimer duplexes are also obtained, one of which corresponds to the experimental crystal structure of ethidium–dinucleoside complexes, but these cannot be joined to the B-DNA structure. Backbone conformations of the tetramer duplex can be constructed until the base-pair separation reaches 8.25 Å, which may limit the molecules that can intercalate.     

Determination of the molecular conformation of beta-D-O2,2'-cyclouridine in aqueous solution by proton magnetic resonance spectroscopy

The solution conformation of β-D -O²,2′-cyclouridine has been determined at 27 and 88°C in D₂O by proton magnetic resonance spectroscopy. The conformation is described in terms of a fixed syn-like sugar-base torsional angle, a type S furanose ring conformation (similar to 2′-endo), and a temperature-dependent exocyclic C(4)′–C(5′) rotamer population containing approximately 50% of the gauche-gauche form at 27°C. β-D -O²,2′-Cyclouridine 5′-phosphate likewise possesses a type S furanose ring conformation.     

The conformational analysis of adenosine triphosphate by classical potential energy calculations

The conformational analysis of adenosine triphosphate was conducted by using classical potential energy calculations. All rotatable bonds were examined, i.e., no dihedral angles were fixed at predetermined conformations except for the ribofuranose ring, which was held in the C(3′)-endo conformation—the conformation observed for adenosine in the crystal state. The energy terms included in the total energy expression consist of nonbonded pairwise interaction, electrostatic pairwise interaction, free energy of solvation, and torsional bond potentials. Two separate approaches were used in the conformational analyses. The first consisted of a sequential fragment approach were four bonds were rotated simultaneously at 30° increments. Each fragment overlapped the preceding one by at least one bond. All rotors were then simultaneously examined at their minima and at ±15°. The second approach consisted of a coarse grid search where all rotors were examined simultaneously, but only at staggered positions. The low-energy conformations thus obtained were then used as starting conformations for a minimization routine based on the method of conjugate directions. The first approach required about 40 hr of central processing unit (CPU) computer time, while the coarse grid/minimization approach required about 4 hr of CPU time. Both the sequential fragment approach and the minimization approach yielded lowest-energy conformations which are remarkably similar to the solid-state conformation of C(3′)-endo ATP.     

Minimum energy conformations of DNA dimeric subunits: Potential energy calculations for dGpdC,dApdA, dCpdC,dGpdG, and dTpdT

Minimum energy conformations have been calculated for the deoxydinucleoside phosphates dGpdC, dApdA, dCpdC, dGpdG, and dTpdT. In these potential energy calculations the eight diheldral angles and the sugar pucker were flexible parameters. A substantial survey of conformation space was made in which all staggred combination ofthe dihedral angles ω′,ω, and ψ, in conjuction with C(2′)-endo puker, were used as starting conformers for the energy minimization. The most important conformations in the C(3′)-endo-puckering domain have ψ = g⁺; ω′,ω = g^?,g^?(A-form),g⁺, g⁺, and g^?,t. With C(2′)-endo-type puker the most important conformations have ψ = g⁺; ω′,ω =g^_,g^_(B-form) and g⁺,t; and ψ =t; ω′,ω =g^_,t(Watson-Crick from) and t,g⁺ (skewed). Stacked bases are a persistent feature of the low-energy conformations, the g⁺ conformer being an exception. Freeing the suger puker allowed this conformation to become low energy, with C(3′)-exo puker. It also caused other low-energy forms, such and the Waston-Crick conformation, to become more favourable. Conformation flexibility in the sugar puker and in ψ, as well as the ω′,ω angle pair, is indicated for the dimeric subunits of DNA.     

Molecular Conformation of 2′-Deoxy-2′-methylidene-cytidine: A Potent Antineoplastic Nucleoside

Abstract

2′-Deoxy-2′-methylidenecytidine (DMDC), a potent inhibitor of the growth of tumor cells, was crystallized with two different forms. One is dihydrated (DMDC·2H₂O) and the other is its hydrochloride salt (DMDC·HCLl). Both crystal and molecular structures have been determined by the X-ray diffraction method. In both forms the glycosidic and sugar conformations are anti and C(4′)-exo, respectively, whereas the conformation about the exocyclic bond is trans for DMDC·2H₂O and gauche ⁺ for DMDC·HCl. Proton nuclear magnetic resonance data of DMDC indicate a preference for the anti C(4′)-exo conformation found in the solid state. These molecular conformations were compared with the related pyrimidine nucleosides. When the cytosine bases are brought into coincidence, DMDC displays the exocyclic C(4′)-C(5′) bond located on the very close position to those of pyrimidine nucleosides with typical overall conformations. On the other hand, the hydroxyl O(3′)-H groups are separated by ca. 3 Å in the cases of DMDC and other pyrimidine nucleosides which have the C(2′)-endo sugar conformation. This result may be useful for the implication about the mechanism of the biological activity of DMDC.     

6-Azauridine, a nucleoside with unusual ribose conformation. The molecular and crystal structure

The cytostatic analogue ribo-6-azauridine crystallizes in the orthorhombic space group P2₁2₁2₁ with eight molecules per unit cell of dimensions $\text{a = 20.230, b = 7.709, c = 12.863}\text{A}\text{?}$. A trial structure was obtained by direct methods. Least-squares refinement of co-ordinates and anisotropic thermal parameters based on 1998 reflections measured on a four-circle diffractometer led to a discrepancy index R = 4.0%. Like uridine, 6-azauridine has the anti conformation about the glycosidic bond and a C(3′)-endo sugar pucker. Unlike uridine, it exhibits a close approach of N(6) to C(2′) at only 2.814 and 2.844 Å in the two independent molecules, and a C(5′)(5′) bond that is gauche to C(4′)O(1′) but trans to C(4′)C(3′); this conformation about a C(4′)C(5′) bond has never been observed before for C(3′)-endo puckered riboses in the crystalline state. The crystal structure displays a pseudo-A face centering and very similar conformational parameters for the two independent molecules. Every OH and NH group in the structure serves as a proton donor in a hydrogen bond, including an unusual N(3)—H(3) … O(1′) link. Molecular orbital calculations by the extended Hückel method indicate that from uridine to 6-azauridine the net charge changes sign at ring positions 5 and 6 and disappears at 1.     

Interactions of molecules with nucleic acids. I. An algorithm to generate nucleic acid structures with an application to the B-DNA structure and a counterclockwise helix.

An algorithm is developed that enables the routine determination of backbone conformations of nucleic acids. All atomic positions including hydrogen are specified in accord with experimental bond lengths and angles but with theoretically determined conformational angles. For two Watson-Crick base pairs at a separation of 3.38 Å, and perpendicular to a common helical axis, minimum energy configurations are found for all 10 combinations at helical angles of α ～ 36°–38°, corresponding to the B-DNA structure with C(2′)-endo sugar puckers. Backbone configurations exist only within the range 35.5° ? α ? 42°, which suggests the origin of the 10-fold helix. Calculated stacking energies for the B-DNA structure increases for each of the clustered groups of base pairs: G·C with G·C, G·C with A·T, and A·T with A·T, and they are in approximate agreement with experimental observations. The counter-clockwise helix is examined, and physically meaningful structures are found only when the helical axes of successive base pairs are disjointed.     

Molecular conformations and 8-CH exchange rates of purine ribo- and deoxyribonucleotides: investigation by Raman spectroscopy

The rate of deuterium exchange of the 8-CH group in a purine deoxyribonucleotide, is the same as the 8-CH exchange rate in the corresponding purine ribonucleotide, with the exception of 5′-nucleotides of guanine. The observed 20% slower rate of 8-CH exchange in 5′-dGMP versus 5′-rGMP, over the temperature range 50–80°C, are attributable to differences in molecular conformation, including differences in ring puckering of the furanose substituents. Minor differences in 8-CH exhange rates are observed between 5′-and cyclic (3′:5′)-deoxyribonucleotides of a given purine, which are similar to those observed previously between corresponding 5′- and cyclic ribonucleotides that have been attributed to the charge difference of their respective phosphate groups [Ferreira, S. A. & Thomas, G. J., Jr. (1981) J. Raman Spectrosc. 11 , 508–514]. The coupling of guanine and furanose ring structures in the 5′-nucleotides is also evident from the vibrational frequencies of the guanine ring, which are strongly dependent on the pucker of the attached furanose moiety. Raman difference spectroscopy clearly reveals the dependence of purine nucleotide spectra on sugar-ring pucker. In the case of GMP, the guanine characteristic ring breathing mode near 600–700 cm^?1 depends for its exact position and intensity on the proportion of C3′-endo (668 cm^?1) and C2′-endo (682 cm^?1) conformers in equilibrium with one another. The Raman intensity ratio I(668)/I(682) is proposed as a measure of the conformer ratio C3′-endo/C2′-endo in 5′-dGMP with possible application also to nucleic acids. Among cyclic nucleotides, differences in spectra of deoxyribo- and ribo- forms also appear to be related to differences of molecular conformation.     

A vibrational spectroscopic study of the self-association of polyinosinic acid and polyguanylic acid in aqueous solution

We have studied by Raman and ir spectroscopy the structure of self-associated polyinosinic acid and polyguanylic acid in aqueous solution. The results are consistent with the formation of a four-stranded complex, which melts cooperatively near 60°C in the case of poly (I) in the presence of K⁺ ions. The conformation of the ribose in both systems is mixed C2′-endo/C3′-endo, giving a structure that is intermediate between the extremes proposed previously from x-ray diffraction studies. Characteristic Raman bands for the C2′-endo ribose conformation in polyribonucleotides are identified. The four-stranded structure of poly (I) appears to be very flexible, with ≈15% of the tetrameric segments being disrupted and ≈30% of the ribose units adopting a disordered conformation prior to melting. This disordering process increases to ≈75% above the melting transition, with the remaining ≈25% of the ribose units keeping an ordered C2′-endo or C3′-endo conformation. © 1994 John Wiley & Sons, Inc.     

Conformational analysis of the 2'-deoxyribofuranose ring from proton-proton coupling constants: analysis of a nucleoside-carcinogen adduct formed from 2-acetylaminofluorene utilizing a three-state model

The conformation of the sugar moiety of 8-(N-fluoren-2-ylamino)-2′-deoxyguanosine in solution has been examined as a function of temperature by ¹H-nmr spectroscopy. Analysis of coupling constants shows that lowering the temperature to ?50°C in methanol shifts the conformational equilibrium of the sugar ring resulting in a C2′-endo conformation at a mole fraction of 0.97. The computed phase angle of pseudorotation and amplitude of pucker are 154° and 36°, respectively, with very little discrepancy between the five calculated coupling constants and coupling constants extrapolated from the temperature profiles. A computer program has been written enabling a three-state best-fit analysis. The three-state analysis indicates an equilibrium between C2′-endo, C3′-endo, and 04′-endo conformations. In aqueous solution, the computed mole fraction of the 04′-endo form is 0.18 at 30°C. The conformation associated with the sugar ring and the C4′? C5′ bond is compared to that of 2′-deoxyguanosine.