Determination of nucleic acid backbone conformation by 1H NMR.

In DNA or RNA duplexes, the six-bond C3'-O3'-P-O5'-C5'-C4'-C3' backbone linkage connecting adjacent residues contains six torsion angles (epsilon, zeta, alpha, beta, gamma, delta) but only four protons. This seriously limits the ability to define the backbone conformation by NMR using purely 1H-1H distance geometry (DG) methods. The problem is further compounded by the inability to assign two of the four backbone protons, namely the poorly resolved H5' and H5' protons, and invariably leads to DG structures with poorly defined backbone conformations. We have developed and tested a reliable method to constrain the beta, gamma, and epsilon (and indirectly alpha and zeta) backbone torsion angles by lower-bound NOE distances to unassigned H5'/H5' resonances combined with either 1H line widths or the conservative use of sigma J measurements; the method relies only on 1H 2-D NMR data, does not involve any structural assumptions, and leads to much improved backbone convergence among DG structures. The C4'-C5' torsion angle gamma is constrained by lower-bound NOE distances from H2' and from H6/H8 to any H5'/H5', as well as by sigma JH4, coupling measurements in the 3.9-4.4 ppm region; delta is constrained by H1'-H4' NOE distances and by H3'-H4' and H3'-H2' J couplings in COSY data; epsilon is partially constrained by H3' line width and/or further constrained by subtracting the minimum possible sigma JH3'-H from the observed sigma JH3' (COSY) to arrive at the maximum possible JH3'-P, which is then converted to H3'-P distance bounds. The angle beta is partially constrained via H5'-P and H5'-P distance bounds consistent with the maximum H5'-P and H5'-P J couplings derived from the observed H5' and H5' line widths, while alpha and zeta are indirectly constrained by lower distance bounds on the observed (n)H1' to (n + 1)H5'/H5' NOEs combined with the prior partial constraints on beta, gamma, delta, and epsilon. The combined effects of these additional constraints in determining distance geometry structures have been demonstrated using a 12-base duplex, [d(GCCGTTAACGGC)]2. Coordinate RMSDs per atom between structures refined with these constraints from random-embedded DG structures, from ideal A-DNA, and from B-DNA starting structures were less than 0.4 A for the central 8 base pairs indicating good convergence. All backbone angles for the central 8 base pairs are very well constrained with less than 10 degrees variation in any of the 48 torsion angles.     

Effect of distortions in the deoxyribose phosphate backbone conformation of duplex oligodeoxyribonucleotide dodecamers containing GT, GG, GA, AC, and GU base-pair mismatches on 31P NMR spectra

We have previously suggested that variations in the 31P chemical shifts of individual phosphates in duplex oligonucleotides are attributable to torsional angle changes in the deoxyribose phosphate backbone. This hypothesis is not directly supported by analysis of the 1H/31P two-dimensional J-resolved spectra of a number of mismatch dodecamer oligonucleotide duplexes including the following sequences: d-(CGTGAATTCGCG), d(CGUGAATTCGCG), d(CGGGAATTCGCG), d(CGAGAATTCGCG), and d(CGCGAATTCACG). The 31P NMR signals of the dodecamer mismatch duplexes were assigned by 2D 1H/31P pure absorption phase constant time (PAC) heteronuclear correlation spectra. From the assigned H3' and H4' signals, the 31P signals of the base-pair mismatch dodecamers were identified. JH3'-P coupling constants for each of the phosphates of the dodecamers were obtained from 1H/31P J-resolved selective proton flip 2D spectra. By use of a modified Karplus relationship, the C4'-C3'-O3'-P torsional angles (epsilon) were obtained. JH3'-P coupling constants were measured for many of the oligonucleotides as a function of temperature. There exists a good linear correlation between 31P chemical shifts and the epsilon torsional angle. This correlation can be further extended to the C3'-O3'-P-O5' torsional angle (zeta) by using a linear relationship between epsilon and zeta obtained from crystal structure studies. The 31P chemical shifts follow the general observation that the more internally the phosphate is located within the oligonucleotide sequence, the more upfield the 31P resonance occurs. In addition, 31P chemical shifts show sequence- and site-specific variations. Analysis of the backbone torsional angle variations from the coupling constant analysis has provided additional information regarding the origin of these variations in 31P chemical shifts.     

Conformational studies of nucleic acids: III. Empirical multiple correlation functions for nucleic acid torsion angles

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, alpha (O3'-P-O5'-C5'), delta (C5'-C4'-C3'-O3') and epsilon (C4'-C3'-O3'-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, alpha, 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.     

DFT studies of the disaccharide, alpha-maltose: relaxed isopotential maps

The disaccharide, alpha-maltose, forms the molecular basis for the analysis of the structure of starch, and determining the conformational energy landscape as the molecule oscillates around the glycosidic bonds is of importance. Thus, it is of interest to determine, using density functionals and a medium size basis set, a relaxed isopotential contour map plotted as a function of the phi(H) and psi(H) dihedral angles. The technical aspects include the method of choosing the starting conformations, the choice of scanning step size, the method of constraining the specific dihedral angles, and the fitting of data to obtain well defined contour maps. Maps were calculated at the B3LYP/6-31+G( *) level of theory in 5 degrees intervals around the (phi(H),psi(H))=(0 degrees ,0 degrees ) position, out to approximately +/-30 degrees or greater, for gg-gg'-c, gg-gg'-r, gt-gt'-c, gt-gt'-r, tg-tg'-c, and tg-tg'-r conformers, as well as one-split gg(c)-gg'(r) conformer. The results show that the preferred conformation of alpha-maltose in vacuo depends strongly upon the hydroxyl group orientations ('c'/'r'), but the energy landscape moving away from the minimum-energy position is generally shallow and transitions between conformational positions can occur without the addition of significant energy. Mapped deviations of selected parameters such as the dipole moment; the C1-O1-C4', H1-C1-O1, and H4'-C4'-O1 bond angles; and deviations in hydroxymethyl rotamers, O5-C5-C6-O6, O5'-C5'-C6'-O6', C5-C6-O6-H, and C5'-C6'-O6'-H', are presented. These allow visualization of the structural and energetic changes that occur upon rotation about the glycosidic bonds. Interactions across the bridge are visualized by deviations in H(O2)...O3', H(O3')...O2, and H1...H4' distances and the H(O2)-O2-C2-C1 and H'(O3')-O3'-C3'-C4' hydroxyl dihedral angles.     

Conformational properties of adenylyl-3' leads to 5'-adenosine in aqueous solution.

A detailed 220-MHz NMR study has been made of the conformational properties for the homodinucleotide adenylyl-3' leads to 5'-adenosine, ApA, in D2O. Unambiguous signal assignments of all proton signals were made with the aid of selectively deuterated nucleotidyl units, ApA, ApA, and D-8ApA, and complete, accurate sets of NMR parameters were derived by simulation-iteration methods. Sets of limiting chemical shifts and coupling values were also obtained for ApA and constituent monomers 3'-AMP and 5'-AMP at infinite dilution and at identical ionization states for assessment of dimerization effects. Conformational properties were evaluated quantitatively for most of the conformational bonds of ApA and these are consistent with two compact folded dynamically averaged structures, a base-stacked right helical structure, I, characterized as anti, C3'-endo, g-, w,w' (320,330 degrees), g'g', gg, C3'-endo, anti, and a more loosely base-stacked loop structure, II, with anti, C3'-endo, g-, w,w' (80 degrees, 50 degrees), g'g', gg, C3'-endo, anti orientations. Dimerization produces a number of nucleotidyl conformational changes including a shift in ribose equilibrium C2'-endo (S) in equilibrium C3'-endo (N) in favor of C3'-endo in both Ap- and -pA (60:40 vs. 35:65 in monomers), a change in glycosidic torsion angle chiCN toward 0 degrees, and a greater locking-in of rotamers along bonds involved in the phosphodiester backbone. Moreover, there is clear evidence that the transitions from S leads to N forms and chiCN leads to 0 degrees are directly related to base stacking in ApA. Finally, ApA exists in solution as an equilibrium between I, II and an unstacked form(s) with as yet undetermined conformational features. Since C4'-C5', C5'-O5', and C3'-O3' bonds possess exceptional conformational stabilities, it is proposed that destacking occurs primarily by rotation about P-O5' and/or O3'-P. Predominant factors influencing the overall ApA conformation are thus base-base interaction and flexibility about P-O5' and O3'-P, with change of ribose conformation occurring in consequence of an alteration of chiCN, the latter in turn being governed by the need for maximum eta overlap of stacked adenine rings.     

Conformational analysis of the trinucleoside diphosphate 3'd(A2'-5'A2'-5'A). An NMR and CD study.

A 500 MHz and 300 MHz NMR study of the trinucleoside diphosphate 3'd(A2'-5'A2'-5'A) is presented. In addition, circular dichroism is used to study base stacking in the title compound. The complete 1H-NMR spectral assignment of the sugar ring proton signals is given. Information about the sugar ring (N- or S-type conformation) and about the backbone geometry along C4'-C5' and C5'-O5' bonds is obtained from the NMR coupling constants. It is shown that the trimer mainly occurs in the N-N-N stacked state at low temperatures; the presence of a minor amount of N-N-S conformational sequence is indicated.     

Vibrational analysis of nucleic acids. V. Force field and conformation-dependent modes of the phosphodiester backbone modeled by diethyl phosphate.

A generalized valence force field is derived for the diethyl phosphate anion [(CH3CH2O)2PO2-] and its deuterium [(CH3CD2O)2PO2-, (CD3CH2O)2PO2- and (CD3CD2O)2PO2-] and carbon-13 [(CH3 13CH2O)2PO2-] derivatives in the stable trans-gauche-gauche-trans conformation. Normal coordinate analysis of the trans-gauche-gauche-trans conformer, which serves as a structural analog of the nucleic acid phosphodiester group, is based on comprehensive infrared and Raman spectroscopic data and vibrational assignments obtained for the diethyl phosphate anion. The generalized valence force field is in good agreement with the scaled ab initio force field of diethyl phosphate and represents significant improvement over earlier modeling of the phosphodiester moiety with dimethyl phosphate. The conformational dependence of skeletal C-C-O-P(O2-)-O-C-C stretching vibrations is also explored. Starting with the trans-gauche-gauche-trans conformation, the frequency dependence of skeletal stretching modes has been obtained by stepwise rotation of the torsion angles of the P-O and C-O bonds corresponding to nucleic acid torsions alpha (P-O5'), beta (O5'-C5'), epsilon (C3'-O3'), and zeta (O3'-P). Both symmetric and antisymmetric phosphoester stretching modes are highly sensitive to P-O and C-O torsions, whereas symmetric and antisymmetric phosphodioxy (PO2-) stretching modes are less sensitive. The present results provide an improved structural basis for understanding previously developed empirical correlations between vibrational marker bands and nucleic acid backbone conformation.     

Conformational studies of nucleic acids: IV. The conformational energetics of oligonucleotides: d(ApApApA) and ApApApA

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: delta (C5'-C4'-C3'-O3')-chi (O4'-C1'-N9-C4), where the energetic basis for an approximately linear delta-chi correlation can be seen: zeta (C3'-O3'-P-O5')-delta, in which the experimentally observed linear correlation between zeta and delta in DNA(220 degrees less than zeta less than 280 degrees) is clearly predicted; zeta-epsilon (C4'-C3'-O3'-P), which shows that epsilon increases with decreasing zeta less than 260 degrees; alpha (O3'-P-O5'-C5')-gamma (O5'-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 delta is predicted to be the most flexible, while for the RNA molecule, the greatest amount of flexibility is expected to reside in alpha and gamma. 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.     

The effect of (2''-5'') and (3''-5'') phosphodiester linkages on conformational and stacking properties of cytidylyl-cytidine in aqueous solution.

Conformational properties of (2'-5') and (3'-5') CpC have been determined by proton magnetic resonance spectroscopy at 220 MHz. The ribose ring structures are predominantly 3E with the exception of the ring from the 2'-phosphate fragment of C(2'-5')pC which exhibits an 2E pucker. Bases are oriented anti with respect to the ribose and the conformations about C4'-C5', C5'-O5', C3'-O3' (C2'-O2') are gg, g'g', and g+ in equilibrium g-, respectively. The dimers exist as mixtures of stacked (g+g+ and g-g- about the P-O(C) bonds) and unstacked species at 20 degrees C. Stacking is estimated to be 35% in both dimers.     

Conformational properties of branched RNA fragments in aqueous solution

The conformational properties of branched trinucleoside diphosphates ACC, ACG, AGC, AGG, AUU, AGU, AUG, ATT, GUU, and aAUU [XYZ = X(2'p5'Y)3'p5'Z] have been studied in aqueous solution by nuclear magnetic resonance (1H, 13C), ultraviolet absorption, and circular dichroism. It is concluded from these studies that the purine ring of the central residue (X; e.g., adenosine) forms a base-base stack exclusively with the purine or pyrimidine ring of the 2'-nucleotidyl unit (Y; 2'-residue). The residue attached to the central nucleoside via the 3'-5'-linkage (Z; 3'-residue) is "free" from the influence of the other two heterocyclic rings. The ribose rings of the central nucleoside and the 2'- and 3'-residues exist as equilibrium mixtures of C2'-endo (2E)-C3'-endo (3E) conformers. The furanose ring of the central nucleoside (e.g., A) when linked to a pyrimidine nucleoside via the 2'-5'-linkage shows a higher preference for the 2E pucker conformation (e.g., AUG, AUU, ACG, ca. 80%) than those linked to a guanosine nucleoside through the same type of bond (AGU, AGG, AGC, ca. 70%). This indicates some correlation between nucleotide sequence and ribose conformational equilibrium. The 2E-3E equilibrium of 2'-pyrimidines (Y) shows significant, sometimes exclusive, preference (70-100%) for the 3E conformation; 3'-pyrimidines and 2'-guanosines have nearly equal 2E and 3E rotamer populations; and the ribose conformational equilibrium of 3'-guanosines shows a preference (60-65%) for the 2E pucker. Conformational properties were quantitatively evaluated for most of the bonds (C4'-C5', C5'-O5', C2'-O2', and C3'-O3') in the branched "trinucleotides" AUU and AGG by analysis of 1H-1H, 1H-31P, and 13C-31P coupling constants. The C4'-C5' bond of the adenosine units shows a significant preference for the gamma + conformation. The dominant conformation about C4'-C5' and C5'-O5' for the 2'-and 3'-nucleotidyl units is gamma + and beta t, respectively, with larger gamma + and beta t rotamer populations for the 2'-unit. The increased conformational purity in the 2'-residue, compared to the 3'-residue, is ascribed to the presence of an ordered (adenine----2'-residue) stacked state. The favored rotamers about C3'-O3' and C2'-O2' are epsilon- and epsilon'-, respectively. The conformational features of AUU and AGG were compared to those of their constitutive dimers A3'p5'G, A2'p5'G, A3'p5'U, and A2'p5'U and monomers 5'pG and 5'pU.     

A comparative conformational study of thymidylyl(3'----5')-thymidine, thymidylyl(3'----5')-5'-thio-5'- deoxythymidine and thymidinylacetamido-[3'(O)----5'(C)]-5'-deoxythymidine

A comparative 270 MHz NMR spectroscopic study on the solution structure of the dimer d(TpT) 1, and its two analogues, namely, d(TpST) 2, and NH2d(TcmT) 4 has been reported. Analysis of chemical shifts and coupling constants indicate that: (i) The sugar moieties of the constituent nucleotides are not affected by modification of the internucleotide linkages and adopt preferentially an S-type conformation. (ii) The C4'-C5' bond in the pT part of the modified dimers 2 and 4 shows a large conformational freedom (gamma+ = 32% and 35%, respectively) compared to 1 (gamma+ = 75%). (iii) The population of the trans conformer about C5'-O5' is less important in d(TpST) 2 compared to d(TpT) 1. (iv) The C3'-O3' bond in 2 adopts a trans conformation as in 1. (v) The glycosidic bonds in the modified dimers 2 and 4 showed preferential syn conformation. UV and CD data show that the modified dimers 2 and 4 have poor tendency to stack intramolecularly, they also base pair less efficiently with d(ApA) as compared to d(TpT) 1.     

Sequence-dependent variations in the 31P NMR spectra and backbone torsional angles of wild-type and mutant Lac operator fragments

Assignment of the 31P resonances of a series of six sequenced-related tetradecamer DNA duplexes, d(TGTGAGCGCTCACA)2, d(TATGAGCGCTCATA)2, d(TCTGAGCGCTCAGA)2, d(TGTGTGCGCACACA)2, d(TGTGACGCGTCACA)2 and d(CACAGTATACTGTG)2, related to the lac operator DNA sequence was determined either by site-specific 17O labeling of the phosphoryl groups or by two-dimensional 1H-31P pure absorption phase constant time (PAC) heteronuclear correlation spectroscopy. J(H3'-P) coupling constants for each of the phosphates of the tetradecamers were obtained from 1H-31P J-resolved selective proton flip 2D spectra. By use of a modified Karplus relationship the C4'-C3'-O3'-P torsional angles (epsilon) were obtained. Comparison of the 31P chemical shifts and J(H3'-P) coupling constants of these sequences has allowed greater insight into those various factors responsible for 31P chemical shift variations in oligonucleotides and provided an important probe of the sequence-dependent structural variation of the deoxyribose phosphate backbone of DNA in solution. These sequence-specific variations in the conformation of the DNA sugar phosphate backbone of various lac operator DNA sequences can possibly explain the sequence-specific recognition of DNA by DNA binding proteins, as mediated through direct contacts between the phosphates and the protein.     

Molecular and crystalline structure of 3'-methylamino-2',3'-dideoxyribosylthymine--a potential inhibitor of HIV]

The structure of 3'-methylamino-2',3'-dideoxyribosylthymine [ddT(3'NHMe)] was determined by X-ray analysis. The space group is P2(1)2(1)2(1). Cell dimensions are: a 5.132(1), b 13.718(1), c 16.947(2) A, V 1193.2 A3, Z 4. The structure was solved by directed methods and refined by the full-matrix least square method to R 4.8%. The molecule of ddT(3'NHMe) has anti-conformation with respect to the glycosidic bond (chi (O4'-C1'-N1-C2) = -106.7 degrees), C3'-endo-C4'-exo puckering of the sugar moiety (P -28.8 degrees, psi m -31.5 degrees) and gauche-gauche conformation about exocyclic C4'-C5' bond (psi(C3'-C4'-C5'-O5') 45.8 degrees). The structure of ddT(3'NHMe) was compared with those of 3'-amino-3'-deoxythymidine, 3'-azido-3'-deoxythymidine and natural thymidine.     

2',3'-cyclic nucleotide 2'-phosphodiesterase from Fusarium culmorum

We describe the properties of a 2',3'-cyclic nucleotide 2'-phosphodiesterase (EC 3.1.4.16), found in Fusarium culmorum, which hydrolyzes nucleoside 2',3'-cyclic monophosphates to nucleoside 3'-phosphates. In contrast with a similar enzyme found in bacteria, the Fusarium enzyme does not exhibit nucleotidase activity and does not show a requirement for metal ions, but is inhibited by micromolar concentrations of Cu++ and Zn++, and is very stable to heat. This cyclic phosphodiesterase hydrolyzes the four major nucleoside 2',3'-cyclic monophosphates and has greater affinity for purine (Kms for Ado-2',3'-P = 0.3 mM and for Guo-2',3'-P = 0.1 mM) than for pyrimidine nucleotides (Kms for Cyd-2',3'-P = 0.6 mM and for Urd-2',3'-P = 2 mM). The respective Vmax for Urd-2',3'-P; Cyd-2',3'-P; Ado-2',3'-P; and Guo-2',3' are 100:45:16:5. The efficacy of the phosphodiesterase to hydrolyze the four major 2',3' cyclic nucleotides (based on the relative values of Vmax/Km) is not significantly different. The Fusarium enzyme differs from a previously described 2',3' cyclic phosphodiesterase from Neurospora, in that it is inactive on 3',5'-nucleoside monophosphates and nucleoside 2' or 3' phosphates.     

Two-dimensional 1H and 31P NMR spectra and restrained molecular dynamics structure of a mismatched GA decamer oligodeoxyribonucleotide duplex

Assignment of the 1H and 31P NMR spectra of a tandem G.A mismatched base pair decamer oligodeoxyribonucleotide duplex, d(CCAAGATTGG)2, has been made by two-dimensional 1H-1H and heteronuclear 31P-1H correlated spectroscopy. Unusual downfield 31P resonances have been assigned by a pure absorption phase constant-time heteronuclear 31P-1H correlated spectrum to be associated with the phosphates on the 5'- and 3'-sides of the mismatched guanosine residue. JH3'-P coupling constants for each of the phosphates of the decamer were obtained from the 1H-31P J-resolved selective proton-flip 2D spectrum. The two most downfield-shifted 31P resonances each appear to consist of two overlapping signals that can be resolved into two distinct doublets with different coupling constants in the J-resolved spectrum. This as well as the temperature dependence of the 31P spectra demonstrates that two distinct conformations exist at lower temperatures. By use of a modified Karplus relationship, the C4'-C3'-O3'-P torsional angles (epsilon) were obtained. A linear correlation between 31P chemical shifts and the measured coupling constants is quite good (only when the larger set of coupling constants of the two most downfield 31P signals is included). The 31P chemical shifts as well as the measured coupling constants tend to follow the positional variation seen in other duplexes of interior phosphates resonating more upfield than terminal residues and of interior phosphates exhibiting smaller coupling constants; however, this pattern is disrupted at the site of the mismatch. Modeling and initial NOESY distance restrained molecular mechanics energy minimization and restrained molecular dynamics support previous observations that the mismatched guanine and adenine bases are both in anti conformations. Most significantly, the epsilon backbone torsional angle variaions calculated from the NOESY distance restrained structures are in agreement with both the crystal structure values and the measured JH3'-P coupling constants.     

Carbon-13 NMR in conformational analysis of nucleic acid fragments. 4. The torsion angle distribution about the C3''-O3'' bond in DNA constituents.

Carbon-13 and proton NMR spectra of a series of oligodeoxynucleotides (d(CT), d(CC), d(TA), d(AT), d(CG), d(GC), d(AG), d(AAA), d(TATA) and d(GGTAAT] were measured at various temperatures. The three coupling constants that are related to the magnitude of backbone angle epsilon (J(C4'-P), J(C2'-P) and J(H3'-P] are analyzed in terms of a three-state equilibrium about this bond. Two epsilon (trans) angles occur, which differ in magnitude depending on the conformation (N or S) of the adjoining deoxyribose ring. The S-type deoxyribose ring is associated with a smaller epsilon (trans) angle: epsilon (t,S) = 192 degrees. The N-type deoxyribose ring is associated with a larger epsilon (trans) angle epsilon (t,N) = 212 degrees. The third rotamer participating in the conformational equilibrium, is a gauche(-) (epsilon (-] conformer and occurs exclusively in combination with the S-type sugar ring (epsilon (-,S) = 266 degrees). Within the limits of experimental error, the magnitude of these three angles appears to be independent of the particular base sequence, except in the case of d(CG) where a slightly larger epsilon (t,S) angle (197 degrees) is indicated. A simple equation is proposed which may be used to calculate the population of epsilon (t,S) conformer in cases where only J(H3'-P) is known.     

The structure and antiviral activity of ribavirin analogs. I. Molecular and crystal structure of 1-(2-hydroxyethoxymethyl)-1,2,4-triazole-5-carboxamide

The crystal and molecular structures of the antiviral compound 1-(2-hydroxyethoxymethyl)-1,2,4-triazole-5-carboxamide has been determined by the X-ray diffraction method. The space group is P2i/c, unit cell parameters a = 4,381, b = 18,679, c = 10,776 A, beta = 107,40 degrees, Z = 4. The structure was solved by the direct method and refined by a full-matrix least-squares procedure to R = 4.9%. Two planar groups of atoms can be distinguished in the molecule. The first group involves the atoms of triazole ring, C6, and C1', the second one contains C5, C6, O6 and N6 atoms. The angle between these planes is 5.6 degrees. The carboxyamide group is rotated by 180 degrees in comparison with this group in ribavirin. That is why the intramolecular hydrogen bond C1'-H1'. 1...O6 can form. Torsion angle O5'-C5'-C4'-O4' is 73.9 degrees and it corresponds to gauche-rotamer. The conformation about O4'-C4' bond is trans. The C1'-C4' bond is approximately perpendicular to the aglycone.     

The structure and antiviral activity of ribavirin analogs. III. Molecular and crystal structure of 1-(2-hydroxyethoxymethyl)-1,2,4-triazole-carboxamide

The crystal and molecular structure of a ribavirin acyclic analogue, 1-(2-hydroxyethoxymethyl)-1,2,4-triazole-3-carboxamide, has been determined by X-ray diffraction method. The space group is P1, unit cell parameters: a = 5,237, b = 6,960, c = 11,483 A, alpha = 93,89, beta = 97,43, gamma = 94,26 degrees; Z = 2. The structure was solved by the direct method and refined by least-squares procedure to R = 3.7%. Two molecular conformers statistically coexist in the unit cell, differing in the hydroxyethoxymethyl group conformation. Trans-conformation about O4'-C4' bond and gauche about C4'-C5' bond are observed in both molecules. C1'-O4' bond is approximately perpendicular to the aglicon.     

Advanced nuclear magnetic resonance lanthanide probe analyses of short-range conformational interrelations controlling ribonucleic acid structures

An advanced method was developed for lanthanide-probe analyses of the conformations of flexible biomolecules such as nucleotides. The new method is to determine structure parameters (such as internal-rotation angles) and population parameters for local conformational equilibria of flexible sites, together with standard deviations of these parameters. As the prominent advantage of this method, the interrelations among local conformations of flexible sites may be quantitatively elucidated from the experimental data of lanthanide-induced shifts and relaxations and vicinal coupling constants. As a structural unit of ribonucleic acids, the molecular conformations and conformational equilibria of uridine 3'-monophosphate in aqueous solution were analyzed. The stable local conformers about the C3'-O3' bond are the G+ (phi' = 281 +/- 11 degrees) and G- (phi' = 211 +/- 8 degrees) forms. The internal rotation about the C3'-O3' bond and the ribose-ring puckering are interrelated; 97 +/- 5% of the C3'-endo ribose ring is associated with the G- form while 70 +/- 22% o the C2'-endo ribose ring is associated with the G+ form. An interdependency also exists between the internal rotation about the C4'-C5' bond and the ribose-ring puckering. These short-range conformational interrelations are probably important in controlling the dynamic aspects of ribonucleic acid structures.