Conformational analysis of a modified ribotetranucleoside triphosphate: m6(2)A-U-m6(2)A-U studied in aqueous solution by nuclear magnetic resonance at 500 MHz

The complete and unequivocal assignment of the 24 ribose proton signals of m6(2)A(1)-U(2)-m6(2)(3)-U(4) by means of 500 MHz NMR spectroscopy at 17 degrees C is given. this assignment is based on scrupulous decoupling experiments carries out at various temperatures. Analysis of the observed chemical shifts and coupling constants of the tetramer shows that the two fragments -m6(2)A(3)-U(4) comprising the 3'-end occur mainly in the classical right-handed stack conformation, whereas the 5'-end the -U(2)- residue appears bulged out in favour of a less well-defined stacking interaction between the bases m6(2)A(1)-and -m6(2)A(3)-. Conformational populations about each of the torsional degrees of freedom along the backbone are discussed. A modernized version of pseudorotation analysis is used to delineate the conformational behaviour of the four ribose rings.     

Conformational analysis of the dinucleotides 5'-methylphospho-N6-dimethyladenylyl-uridine (mpm62A-U) and 5'methylphospho-uridylyl-N6-dimethyladenosine (mpU-m62A) and of the trinucleotide U-m62A-U. A nuclear magnetic resonance and circular dichroic study

NMR and CD studies were carried out on the dinucleotides 5'-methylphospho-N6-dimethyladenylyl-uridine (mpm62-U) and 5'-methylphospho-uridylyl-N6-dimethyladenosine (mpU-m62A) and on the trinucleotide U-m62A-U. A detailed comparison is given of the conformational features of mpm62A-U and mpU-m62A with the corresponding 5'-nonphosphorylated dinucleotides m62A-U and U-m62A, respectively. The behaviour of the trinucleotide U-m62A-U is compared with the properties of the constituent dinucleotides U-m62A and mpm62A-U. Chemical-shift and CD data were used to determine the amount of stacking interactions. For each compound NMR spectra were recorded at two or three sample concentrations in order to separate intermolecular and intramolecular base-base interactions. The coupling constants of the ribose ring are interpreted in terms of the N/S equilibrium, and population distributions along the backbone angles beta, gamma and epsilon are presented. The combined data indicate a strong similarity between mpm62A-U and m62A-U both in degree and in mode of stacking. In contrast, the existence of different types of stacking interactions in mpU-m62A and U-m62A is suggested in order to explain the NMR and CD data. It is concluded that dinucleoside bisphosphates serve better as a model for the behaviour of trinucleotides than dinucleoside monophosphates. The trinucleotide U-m62A-U adopts a regular single-stranded stacked RNA structure with preference for N-type ribose and gamma+ and beta t backbone torsion angles. The difference in behaviour between the U-m62A- part of U-m62A-U and the dimer U-m62A is seen as a typical example of conformational transmission.     

Conformational transitions of flanking purines in HIV-1 RNA dimerization initiation site kissing complexes studied by CHARMM explicit solvent molecular dynamics

Dimerization of HIV-1 genomic RNA is initiated by kissing loop interactions at the Dimerization Initiation Site (DIS). Dynamics of purines that flank the 5' ends of the loop-loop helix in HIV-1 DIS kissing complex were explored using explicit solvent molecular dynamics (MD) simulations with the CHARMM force field. Multiple MD simulations (200 ns in total) of X-ray structures for HIV-1 DIS Subtypes A, B, and F revealed conformational variability of flanking purines. In particular, the flanking purines, which in the starting X-ray structures are bulged-out and stack in pairs, formed a consecutive stack of four bulged-out adenines at the beginning of several simulations. This conformation is seen in the crystal structure of DIS Subtype F with no interference from crystal packing, and was frequently reported in our preceding MD studies performed with the AMBER force field. However, as CHARMM simulations progressed, the four continuously stacked adenines showed conformational transitions from the bulged-out into the bulged-in geometries. Although such an arrangement has not been seen in any X-ray structure, it has been suggested by a recent NMR investigation. In CHARMM simulations, in the longer time scale, the flanking purines display the tendency to move to bulged-in conformations. This is in contrast with the AMBER simulations, which indicate a modest prevalence for bulged-out flanking base positions in line with the X-ray data. The simulations also suggest that the intermolecular stacking between purines from the opposite hairpins can additionally stabilize the kissing complex.     

Influence of uracil on the conformational behaviour of RNA oligonucleotides in solution

NMR studies were carried out on some alternating pyrimidine-purine sequences: the single-stranded tetramers CACA and UGUG and the self-complementary octamer CACAUGUG. Assignments, based upon COSY, homonuclear Hartmann-Hahn, and NOESY experiments, are given for the resonances of all base protons and of several sugar protons. Chemical shift vs temperature profiles were used to obtain thermodynamic parameters for the single-stranded stack in equilibrium with random coil and the duplex in equilibrium with random coil equilibria. The populations of N-type conformer of the ribose rings were estimated from the observed J1'2'. Comparisons with another alternating pyrimidine-purine sequence Um2(6)AUm2(6)A and with the deoxyribose counterparts d(CACA), d(TGTG) and d(CACATGTG) are given. Previous 1H-NMR investigations of Um2(6)AUm2(6)A revealed that the population of bulge-out structure diminishes compared to m2(6)AUm2(6)A due to the U(1)-m2(6)A(2) stacking interaction. In CACA a strong stacking proclivity (Tm = 310 K) together with a clear preference for N-type ribose is observed. However, the stacking interactions in UGUG are relatively less stable (Tm = 288 K) and a bias towards S-type sugar is present. Besides a small amount of stack, a significant contribution of bulge out structure is proposed for UGUG. We conclude that the nature of the pyrimidine base mainly determines the formation of bulge-out structures. The poor stacking properties of uracil now appear to be mainly responsible for this phenomenon. Comparison with the deoxyribose counterparts shows a reasonable agreement between the Tm values of CACA and d(CACA), whereas the Tm of UGUG (288 K) is much lower than the Tm of d(TGTG) (315 K). It is suggested that the absence of bulge-out structures in DNA purine-pyrimidine-purine sequences is related to the relatively strong stacking proclivity of dT residues compared to that of U residues. The Tm values (average 341 K) for the duplex in equilibrium with random coil transition obtained for each residue of CACAUGUG appear very similar. All ribose rings, except the G(8), adopt a pure N conformer in the duplex. This is taken to mean that the differences in conformational behaviour of the constituent tetramers disappear upon duplex formation.     

A carbon-13 nuclear magnetic resonance study of the 3'-terminus of 16S ribosomal RNA of Escherichia coli specifically labeled with carbon-13 in the methylgroups of the m6(2)Am6(2)A sequence.

30S ribosomes were isolated from a kasugamycin resistant mutant of E. coli that lacks methylgroups on two adjacent adenines in 16S ribosomal RNA. These ribosomes were methylated in vitro with a purified methylating enzyme and 5-S-adenosyl-(13C-methyl)-L-methionine chloride ((13C-methyl)-SAM) as methyldonor. After in situ cleavage of the 16S ribosomal RNA by the bacteriocin cloacin DF13, the 49 nucleotide fragment from the 3'-end of the RNA was isolated. The carbon-13 nuclear magnetic resonance spectra of the fragment at various temperatures were compared with those of 6-N-dimethyladenosine (m6(2)A) and 6-N-dimethyladenylyl-(3' leads to 5')-6-N-dimethyladenosine (m6(2)Am6(2)A). The data show that the two methylated adenines, which are part of a four membered hairpin loop, show a strong tendency to be stacked in analogy to the dinucleotide m6(2)Am6(2).     

Comparative surface accessibility of a pore-lining threonine residue (T6') in the glycine and GABA(A) receptors

The substituted cysteine accessibility method was used to probe the surface exposure of a pore-lining threonine residue (T6') common to both the glycine receptor (GlyR) and gamma-aminobutyric acid, type A receptor (GABA(A)R) chloride channels. This residue lies close to the channel activation gate, the ionic selectivity filter, and the main pore blocker binding site. Despite their high amino acid sequence homologies and common role in conducting chloride ions, recent studies have suggested that the GlyRs and GABA(A)Rs have divergent open state pore structures at the 6' position. When both the human alpha1(T6'C) homomeric GlyR and the rat alpha1(T6'C)beta1(T6'C) heteromeric GABA(A)R were expressed in human embryonic kidney 293 cells, their 6' residue surface accessibilities differed significantly in the closed state. However, when a soluble cysteine-modifying compound was applied in the presence of saturating agonist concentrations, both receptors were locked into the open state. This action was not induced by oxidizing agents in either receptor. These results provide evidence for a conserved pore opening mechanism in anion-selective members of the ligand-gated ion channel family. The results also indicate that the GABA(A)R pore structure at the 6' level may vary between different expression systems.     

Molecular recognition in purine-rich internal loops: thermodynamic,structural, and dynamic consequences of purine for adenine substitutions in 5'(rGGCAAGCCU)2

The contribution of amino groups to the thermodynamics, structure, and dynamics of tandem A.A mismatches is investigated by substitution of purine (P) for adenine (A) within the RNA duplex, 5'(rGGCAAGCCU)(2), to give 5'(rGGCPAGCCU)(2), 5'(rGGCAPGCCU)(2), and 5'(rGGCPPGCCU)(2). The 5'(rGGCAAGCCU)(2) duplex has sheared A(anti).A(anti) (A.A trans Hoogsteen/Sugar-edge) pairs in which the A5 amino group is involved in hydrogen bonds but the A4 amino group is not [Znosko, B. M., Burkard, M. E., Schroeder, S. J., Krugh, T. R., and Turner, D. H. (2002) Biochemistry 41, 14969-14977]. In comparison to 5'(rGGCAAGCCU)(2), replacing the amino group of A4 with a hydrogen stabilizes the duplex by 1.3 kcal/mol, replacement of the A5 amino group destabilizes the duplex by 0.6 kcal/mol, and replacement of both A4 and A5 amino groups destabilizes the duplex by 0.8 kcal/mol. In NMR structures, the P.A noncanonical pairs of the 5'(rGGCPAGCCU)(2) duplex have a sheared anti-anti structure (P.A trans Hoogsteen/Sugar-edge) with P4.A5 interstrand hydrogen bonding and A5 bases that interstrand stack, similar to the structure of 5'(rGGCAAGCCU)(2). In contrast, the A.P pairs of the 5'(rGGCAPGCCU)(2) duplex have a face-to-face conformation (A.P trans Watson-Crick/Watson-Crick) with intrastrand stacking resembling typical A-form geometry. Although the P5 bases in 5'(rGGCPPGCCU)(2) are involved in an interstrand stack, the loop region is largely undefined. The results illustrate that both hydrogen-bonded and non-hydrogen-bonded amino groups play important roles in determining the thermodynamic, structural, and dynamic characteristics of purine rich internal loops.     

Influence of N6-methylation of residue A(5) on the conformational behaviour of d(C-C-G-A-A-T-T-C-G-G) in solution studied by 1H-NMR spectroscopy. 1. The duplex form

One- and two-dimensional NMR studies at 300 MHz and 500 MHz were carried out on the two oligonucleotides d(C-C-G-A-A-T-T-C-G-G) and d(C-C-G-A-m6A-T-T-C-G-G) in aqueous solution. NMR spectra were observed at 10 mM sample concentration over the temperature range 273-368 K. Assignments are given of the base, H1', H2', H2", H3' and of some H4' resonances, based upon a combination of two-dimensional correlation spectra (COSY) and two-dimensional nuclear Overhauser effect spectra (NOESY); imino-proton resonances were assigned with the aid of a two-dimensional NOE experiment. Chemical shift vs temperature profiles were constructed in order to gain insight into the influence of N6-methylation of residue A(5) on the temperature-dependent conformational behaviour of the decamer and to determine thermodynamic parameters for the duplex-to-coil transition. The NOESY spectra, the imino-proton spectra and the shift profiles of the two compounds, under conditions where each forms a B-DNA-type duplex, are very similar. This is taken to indicate that the influence of N6-methylation of residue A(5) on the local structure of the duplex must be small. However, the temperature dependence of the (non-)exchangeable proton resonances of the two compounds reveals that methylation slows down the duplex-single-strand exchange. Furthermore, a thermodynamic analysis of the two compounds indicates that N6-methylation slightly decreases the stability of the duplex relative to the monomeric forms (Tm is reduced from 332 K down to 325 K at 10 mM sample concentration). Proton-proton couplings were obtained by means of one-dimensional and two-dimensional NMR experiments and were used in a conformational analysis of the sugar ring of each residue of the two compounds in the duplex form. The analysis indicated that all sugar rings display conformational flexibility in the intact duplex: population S-type sugar conformation ranges from 70% to 100%. A more refined analysis of the sugar rings of the parent compound revealed a sequence-dependent variation of the sugar geometry. This variation does not follow well the trend predicted by the Calladine/Dickerson sigma 3-sum rule [Dickerson, R. E. (1983) J. Mol. Biol. 166, 419-441; Calladine, C. R. (1982) J. Mol. Biol. 161, 343-352]; moreover the actual variations appear to be smaller in solution than those expected on the basis of known X-ray structures.     

Circular dichroism studies suggest that TAR RNA changes conformation upon specific binding of arginine or guanidine.

Short basic peptides from the HIV Tat protein bind specifically to a bulge region in TAR RNA, with a single arginine residue providing the only sequence-specific contact. The free amino acid arginine also binds specifically to TAR. Previous circular dichroism (CD) experiments suggested that peptide binding induces a conformational change in TAR. Here we confirm this observation using single arginine-containing peptides and show that arginine or guanidine binding also induces a conformational change in TAR. A peptide containing a single arginine within a stretch of histidines (CYHHHRHHHHHA) shows pH-dependent binding and a corresponding change in TAR conformation, as detected by a decrease in the CD signal at 265 nm. Arginine and guanidine, which bind to TAR with apparent Kd's of approximately 1.5 mM, induce similar CD changes. In contrast, lysine, which does not bind specifically to TAR, has no effect. Mutants of TAR that abolish specific binding (a U-->C substitution in the three-nucleotide bulge, a deletion of the bulge, or an A-U to U-A base pair change above the bulge) show no change in the CD signal upon binding of peptides, arginine, or guanidine. The results suggest that binding of a single guanidinium group to a specific site in TAR induces a change in RNA conformation.     

Comparative NMR study of A(n)-bulge loops in DNA duplexes: intrahelical stacking of A, A-A, and A-A-A bulge loops.

We have prepared a series of deoxyoligonucleotide duplexes of the sequence d(G-C-A-T-C-G-X-G-C-T-A-C-G).d(C-G-T-A-G-C-C-G-A-T-G-C), in which X represents either one (A), two (A-A), or three (A-A-A) unpaired adenine basis. Using two-dimensional proton and phosphorus NMR spectroscopy, we have characterized conformational features of these bulge-loop duplexes in solution. We find that Watson-Crick hydrogen bonding is intact for all 12 base pairs, including the GC bases that flank the bulge loop. Observation of NOE connectivities in both H2O and D2O allows us to unambiguously localize all of the bulged adenine residues to intrahelical positions within the duplex. This is in contrast to an earlier model for multiple-base bulge loops in DNA [Bhattacharyya, A., & Lilley, D. M. J. (1989) Nucleic Acids Res. 17, 6821-6840], in which all but the most 5' bulged base are looped out into solution. We find that insertion of two or three bases into the duplex results in the disruption of specific sequential NOEs for the base step across from the bulge loop site on the opposite strand. This disruption is characterized by a partial shearing apart of these bases, such that certain sequential NOEs for this base step are preserved. We observe a downfield-shifted phosphorus resonance, which we assign in the A-A-A bulge duplex to the 3' side of the last bulged adenine residue. Proton and phosphorus chemical shift trends within the An-bulge duplex series indicate that there is an additive effect on the structural perturbations caused by additional unpaired bases within the bulge loop. This finding parallels previous observations [Bhattacharyya, A., & Lilley, D. M. J. (1989) Nucleic Acids Res. 17, 6821-6840; Hsieh, C.-H., & Griffith, J. D. (1989) Proc. Natl. Acad. Sci. U.S.A. 86, 4833-4837] on the magnitude of the induced bending of DNA duplexes by multiple-base bulge loops.     

Solution structure of the SL1 RNA of the M1 double-stranded RNA virus of Saccharomyces cerevisiae

The 20-nucleotide SL1 VBS RNA, 5'-GGAGACGC[GAUUC]GCGCUCC (bulged A underlined and loop bases in brackets), plays a crucial role in viral particle binding to the plus strand and packaging of the RNA. Its structure was determined by NMR spectroscopy. Structure calculations gave a precisely defined structure, with an average pairwise root mean square deviation (RMSD) of 1.28 A for the entire molecule, 0.57 A for the loop region (C8-G14), and 0.46 A for the bulge region (G4-G7, C15-C17). Base stacking continues for three nucleotides on the 5' side of the loop. The final structure contains a single hydrogen bond involving the guanine imino proton and the carbonyl O(2) of the cytosine between the nucleotides on the 5' and 3' ends of the loop, although they do not form a Watson-Crick base pair. All three pyrimidine bases in the loop point toward the major groove, which implies that Cap-Pol protein may recognize the major groove of the SL1 loop region. The bulged A5 residue is stacked in the stem, but nuclear Overhauser enhancements (NOEs) suggest that A5 spends part of the time in the bulged-out conformation. The rigid conformation of the upper stem and loop regions may allow the SL1 VBS RNA to interact with Cap-Pol protein without drastically changing its own conformation.     

The 2 A structure of helix 6 of the human signal recognition particle RNA

BACKGROUND: The mammalian signal recognition particle (SRP) is an essential cytoplasmic ribonucleoprotein complex involved in targeting signal-peptide-containing proteins to the endoplasmic reticulum. Assembly of the SRP requires protein SRP19 to bind first to helix 6 of the SRP RNA before the signal-peptide-recognizing protein, SRP54, can bind to helix 8 of the RNA. Helix 6 is closed by a GGAG tetraloop, which has been shown to form part of the SRP19-binding site. RESULTS: The high-resolution (2.0 A) structure of a fragment of human SRP RNA comprising 29 nucleotides of helix 6 has been determined using the multiple anomalous dispersion (MAD) method and bromine-labelled RNA. In the crystal the molecule forms 28-mer duplexes rather than the native monomeric hairpin structure, although two chemically equivalent 11 base pair stretches of the duplex represent the presumed native structure. The duplex has highly distorted A-RNA geometry caused by the occurrence of several non-Watson-Crick base pairs. These include a 5'-GGAG-3'/3'-GAGG-5' purine bulge (which replaces the tetraloop) and a 5'-AC-3'/3'-CA-5' tandem mismatch that, depending on the protonation state of the adenine bases, adopts a different conformation in the two native-like parts of the structure. The structure also shows the 2'3'-cyclic phosphate reaction product of the hammerhead ribozyme cleavage reaction. CONCLUSIONS: The 29-mer RNA is the first RNA structure of the human SRP and provides some insight into the binding mode of SRP19. The observed strong irregularities of the RNA helix make the major groove wide enough and flat enough to possibly accommodate an alpha helix of SRP19. The variety of non-canonical base pairs observed enlarges the limited repertoire of irregular RNA folds known to date and the observed conformation of the 2'3'-cyclic phosphate containing Ade29 is consistent with the current understanding of the hammerhead ribozyme reaction mechanism.     

Bulged adenosine influence on the RNA duplex conformation in solution

The RNA single bulge motif is an unpaired residue within a strand of several complementary base pairs. To gain insight into structural changes induced by the presence of the adenosine bulge on RNA duplex, the solution structures of RNA duplex containing a single adenine bulge (5'-GCAGAAGAGCG-3'/5'-CGCUCUCUGC-3') and a reference duplex with all Watson-Crick base pairs (5'-GCAGAGAGCG-3'/5'-CGCUCUCUGC-3') have been determined by NMR spectroscopy. The reference duplex structure is a regular right-handed helix with all of the attributes of an A-type helix. In the bulged duplex, single adenine bulge stacks into the helix, and the bulge region forms a well-defined structure. Both structures were analyzed by the use of calculated helical parameters. Distortions induced by the accommodation of unpaired residue into the helical structure propagate over the entire structure and are manifested as the reduced base pairs inclination and x-displacement. Intrahelical position of bulged adenine A5 is stabilized by efficient stacking with 5'-neighboring residues G4.     

Evidence for the tetraplex structure of the d(GT)n repetitive sequences in solution.

The ability of oligonucleotides 3'-d(GT)5pO(CH2)6Opd(GT)5-5' (anti[d(GT)]) and 3'-d(GT)5pO(CH2)6Opd(GT)5-3' (par[par[d(GT)]) to form tertiary structures has been studied. Circular dichroism (CD) as well as the fluorescence of the ethidium bromide (EtBr) complexes with oligonucleotides and hydrodynamic volume measurements in solutions containing 0.01 M phosphate buffer, pH 7 and NaCl in concentrations from 0.1 M to 1 M, have been used. The data obtained in the temperature interval from 3 degrees C to 10 degrees C are in good agreement with the structure suggested earlier where the par[d(GT)] and anti[d(GT)] form structures with four parallel strands in which layers of four G-residues alternate with unpaired bulged-out T-residues. Ethidium bromide interacts with the structure in a cooperative manner. Two ethidium bromide molecules intercalate between two layers of four G-residues.     

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.     

Two-dimensional proton nuclear magnetic resonance investigation of the synthetic deoxyribonucleic acid decamer d(ATATCGATAT)2

In this study two-dimensional NMR techniques (COSY and NOESY) have been used in conjunction with one-dimensional NMR results to complete the assignment of the proton NMR spectrum of the double-stranded DNA decamer, d(ATATCGATAT)2, and to obtain qualitative information about numerous interproton distances in this molecule and some limited information about conformational dynamics. COSY and NOESY measurements have been combined to systematically assign many of the resonances from the H1' and H2',2" sugar protons to specific nucleotides in the double helix. This method relies on the fact that sugar protons within a specific nucleotide are scalar coupled and that base protons (AH8, GH8, TH6, and CH6) in right-handed helices can interact simultaneously with their own H2',2" sugar protons and those of the adjacent (5'-3') nucleotide attached to its 5' side (i.e., XpA not ApX). A COSY experiment is used to identify sugar resonances within a residue whereas the NOESY experiment allows the neighboring sugar to be connected (linked). The CH5 and CH6 resonances in the spectrum can immediately be identified by the COSY experiment. The methyl protons of thymine residues exhibit strong through-space interbase interactions both with their own TH6 proton and with AH8 proton on the adjacent (5'-3') adenine residue. These interactions are used both to make assignments of the spectra and to establish that the thymine methyl groups are in close proximity to the AH8 protons of adjacent adenine residues [Feigon, J., Wright, J. M., Leupin, W., Denny, W. A., & Kearns, D. R. (1982) J. Am. Chem. Soc. 104, 5540].(ABSTRACT TRUNCATED AT 250 WORDS)     

Conformational preferences of modified nucleic acid bases N6-methyl-N6-(N-threonylcarbonyl) adenine and 2-methylthio-N6-(N-threonylcarbonyl) adenine by the quantum chemical PCILO calculations

Conformational preferences of the hypermodified nucleic acid bases N6-methyl-N6-(N-threonylcarbonyl) Adenine, m6tc6 Ade, and 2-methylthio-N6-(N-threonylcarbonyl) Adenine, mS2 tc6 Ade, have been studied theoretically using the quantum chemical PCILO (Perturbative Configuration Interaction using Localized Orbitals) method. The multidimensional conformational space has been searched using selected grid points formed by combining the various torsion angles which take the favoured values obtained from energy variation with respect to each torsion angle individually. In m6 tc6 Ade and mS 2tc6 Ade alike the threonylcarbonyl substituent preferably orients away (distal) from the imidazole moiety of the adenine ring. And as in the simpler N6-(N-threonylcarbonyl) Adenine, tc6 Ade, the atoms in the ureido group as well as the amino acid carbon atoms C(12) and C(13) remain coplanar with the purine base. As in tc6 Ade, this conformation is stabilized by the intramolecular hydrogen bond between N(11)H of the amino acid and N(1) of the adenine base. The N6-methyl protons, in m6 tc6 Ade, take trans-staggered orientation with respect to the C(6)-N(6) bond. The preferred orientation of the 2-methylthio group is cis to the C(2)-N(3) bond in mS 2tc6 Ade. This is in marked contrast to the modified nucleic acid base 2-methylthio-N6-(delta 2-isopentenyl) Adenine, mS 2i6 Ade, where the 2-methylthio group orients trans to the C(2)-N(3) bond, causing a change in the preferred orientation of the isopentenyl component on methylthiolation. The present results thus indicate that unlike in the isopentenyl adenine the role of further chemical substitutions in threonylcarbonyl adenine may be indirect and less pronounced.     

Conformational analysis of m4(2)C-m4(2)C-m6(2)A: a chemically modified 3'-acceptor end of tRNA, studied by NMR and CD methods.

A study on the conformation of the title compound, C-C-A, and on its constituent dinucleotides is presented. 1H-NMR spectra at 360 and 500 MHz were completely assigned by decoupling experiments. Computer simulation of the spectra yielded precise proton-proton and proton-phosphorus coupling constant values. The coupling constants are analyzed in terms of torsion angles and of N- and S-type sugar pucker. 31P-NMR spectra gave some information about P-O backbone torsion angles alpha and zeta. CD spectroscopy was used to obtain insight in the base-base interaction. The C(1) and C(2) unit in C-C-A show normal preference for N-type conformation of the sugar ring, whereas the A(3) residue appears rather biased towards the S-conformation. The zeta and alpha backbone torsion angles in the C-C phosphodiester linkage in C-C-A appear to assume normal g-, g- conformation, the zeta, alpha combination in the C-A linkage is proposed to have a g+, t conformation. In the C-C fragment in C-C-A a regular stack is indicated; it is suggested that the C-A part adopts an unusual antiparallel base stack.