Biomedical subjects

B R Reid

Publications and source records attributed to B R Reid.

At least 37 records · Page 2Linked to original sources

PubMed1994

The unusual structure of the human centromere (GGA)2 motif. Unpaired guanosine residues stacked between sheared G.A pairs.

The centromere of human chromosomes contains multiple repeats of the DNA sequence d(TGGAA)n. This sequence has the interesting property of pairing with itself to form stable duplexes. We have determined the solution structure of the unusual DNA duplex 5'-TGGAATGGAA:TGGAATGGAA-3' at atomic resolution. The duplex contains unpaired staggered guanosine residues, which co-stack by intercalation between sheared G.A and A.G base-pairs to form an interesting new structural motif, the GA-bracketed G-stack. The TGGAA repeat unit contains six "steps", four of which are not Watson-Crick base-pairs.

Adenosine↗

PubMed1994

The solution structure of the r(gcg)d(TATACCC):d(GGGTATACGC) Okazaki fragment contains two distinct duplex morphologies connected by a junction.

Okazaki fragments are important intermediates in DNA replication. Chimeric duplexes that are structurally equivalent to Okazaki fragments also occur during reverse transcription of RNA retroviruses. Such duplexes consist of an RNA-DNA chimeric strand base-paired to a pure DNA strand; hence they have a hybrid duplex "left half" covalently linked to a "right half" that is pure DNA. We have determined the solution structure of the synthetic Okazaki fragment r(gcg)d(TATACCC):d(GGGTATACGC) by means of two-dimensional NMR, restrained molecular dynamics and full relaxation matrix simulation of the two-dimensional nuclear Overhauser effect spectra at various mixing times. The large negative x-displacement and large positive inclination in the hybrid section of the duplex are structural characteristics similar to those found in pure hybrid duplexes. However, the DNA sugar puckers and the width and depth of the minor groove in the pure DNA section are more like B-form DNA, especially beyond the junction. Thus, this Okazaki fragment duplex assumes a conformation in solution that is a chimeric mixture of hybrid-form (H-form) and B-form structures and the overall molecule cannot be classified as either an A-form or a B-form duplex. The co-existence of these two different conformations in a single duplex gives rise to a structural discontinuity with a bend of approximately 18.1 (+/- 0.4) degrees at the junction between the hybrid and DNA segments that may be important for reverse transcriptase binding and RNase H cleavage of such molecules. Despite the fact that the solution structure is quite different from the all A-form structure reported recently for the exact same molecule in the crystalline state, a surprising number of local helical parameters were found to be quite similar to those reported for the crystal structure.

Base Sequence↗

PubMed1994

DNA sequence GCGAATGAGC containing the human centromere core sequence GAAT forms a self-complementary duplex with sheared G.A pairs in solution.

The DNA sequence dGCGAATGAGC has a well-resolved, two-dimensional nuclear Overhauser (NOESY) spectrum that is suitable for high quality solution structure determination by NMR methods; in solution this sequence forms a stable self-complementary duplex containing sheared G.A base-pairs. A total of 220 distance constraints derived from time-dependent NOE measurements were collected and refined by repeated back-calculation of the NOESY spectra. Distance information from imino proton studies and from exclusive two-dimensional correlated spectroscopy (E. COSY) and/or linewidth analysis was included in the structure calculation using the program DSPACE 4.2, followed by restrained energy minimization with the program DISCOVER using the AMBER force field. The energies of the distance geometry (DG) structures decreased rapidly in the first few cycles and approached -510 +/- 3 kcal after 1000 cycles of conjugate gradient minimization (about 540 kcal lower than in the initial DG structures). All 15 final DG structures converged to a single family of closely related structures with pair-wise r.m.s.d. values of 0.96 +/- 0.34 A, which was further reduced by energy minimization to 0.70 +/- 0.35 A. Rather unusual structural features of the duplex are revealed in the final structures. The results indicate that, in addition to normal sequences with standard base-pairing, unusual nucleic acid structures can also be determined in solution with quite high precision by NMR/distance geometry methods.

Base Composition↗

PubMed1994

1H NMR studies on an Asn-linked glycopeptide. GlcNAc-1 C2-N2 bond is rigid in H2O.

The conformation of an Asn-linked glycopeptide in H2O was studied by two-dimensional 1H NMR. Nonexchangeable proton and exchangeable amide (NH) proton resonances were assigned for the hen ovomucoid glycopeptide 1, Ser-Ile-Glu-Phe-Gly-Thr-Asn Ile-Ser-Lys, with pentasaccharide Man alpha 1-3 (Man alpha 1-6)Man beta 1-4GlcNAc beta 1-4GlcNAc beta 1-NH attached to the Asn7 gamma-carboxamide. The pentasaccharide increases the local correlation times of amino acid residues near the N-glycosylation site. Nuclear Overhauser effect (NOE) measurements on 1 and the corresponding Man3-GlcNAc2 pentasaccharide 3 show that the attached peptide does not perturb O-glycoside conformation. Sequential dNN (i, i + 1) NOEs in the Thr6-Ser9 region indicate populations of folded structure near the N-glycosylation site of both glycopeptide 1 and aglycosyl peptide 2. However, the Man3GlcNAc2 pentasaccharide does not dramatically affect the average conformation of either the peptide backbone or the Asn7 side chain. GlcNAc NH protons were studied at pH 3.0; and NOE and 3JNH data were used to constrain the glycopeptide's GlcNAc-1 side chain dihedral angle (tau) (C1-C2-N2-C7(Ac)). The glycopeptide's core GlcNAc-1 C2-N2 side chain bond is not flexible in H2O. A strong GlcNAc-1 NH2-H3 NOE, a medium strength NH2-H1 NOE, and a weak NH2-H2 interaction suggest that GlcNAc-1 has a rigid C2-N2 bond, with tau between 95 and 115 degrees. No evidence was found for intramolecular hydrogen bonds restricting this C2 side chain torsion. It may be that GlcNAc-1's rigid planar N-glycosidic linkage limits the conformational space available to the adjacent C2 acetamido side chain.

Acetylglucosamine↗

PubMed1994

Sequence dependence of DNA structure in solution.

Sequence-dependent structural variations in DNA can influence its binding by ligands and proteins. However, relatively little is known about sequence-structure relationship for arbitrary DNA sequences. The 1H two-dimensional NOESY data presented here for ten oligonucleotide duplexes show pronounced sequence-dependent changes in at least two types of internucleotide distances commonly used in sequential connectivity assignments, namely the H-6/H-8 to preceding (5') H-1' distance (S1) and the H-6/H-8 to preceding (5') H-2'' distance (S2). On the basis of these two measured distances, all dinucleotide steps can be divided into four different groups: Y-R, R-Y, R-R and Y-Y, where R is purine and Y is pyrimidine. These data suggest some rules for the variation in these distances along DNA duplexes. Correlations between these distances and helical parameters of DNA are discussed in comparison to well-resolved X-ray structures of B-type DNA.

Base Sequence↗

PubMed1994

The amplitude of local angular motion of purines in DNA in solution.

Nuclear magnetic resonance and optical experiments are combined to determine the rms amplitude of local angular motion of purines in DNA in solution. A 12 base-pair duplex DNA with the sequence d(CGCGAATTCGCG)2 is deuterated at the H8 positions of adenine and guanine by exchange with solvent at 55 degrees C. The deuterium nmr spectrum of this DNA is measured at 30 mg/mL at 30 degrees C in an 11.76 Tesla magnet (76.75 MHz). The time-resolved fluorescence polarization anisotropies (FPA) of this same sample and also a greatly diluted sample (0.215 mg/mL) were measured after addition of ethidium. FPA measurements of the dilute sample yield the hydrodynamic radius, RH = 9.94 +/- 0.2 A, while those at the nmr concentration are employed to characterize the collective motions in terms of either an enhanced viscosity or dimer formation. The rms amplitude of local angular motion was determined by analyzing the 2H-nmr spectrum, in particular the line width, using recently developed theory for the transverse relaxation rate (RQ2) together with essential information about the collective motions from these and other optical studies. When the principal-axis frame of the electric field gradient tensor is assumed to undergo overdamped libration around each of its three body-fixed axes in an isotropic deflection potential, then the rms amplitude of local angular motion around any single axis is found to lie in the range 10 degrees-11 degrees, provided the high DNA concentration acts to enhance the viscosity, and is about 9 degrees-11 degrees, if it acts to produce end-to-end dimers. The proton nmr relaxation data of Eimer et al. are reanalyzed and shown to yield an rms amplitude of angular motion of the cytosine H5-H6 internuclear vector of 9 degrees-10 degrees, depending upon its orientation with respect to the helix axis. In all of these analyses, full account is taken of the collective twisting and bending deformations, which have a small but significant effect on the results. It is shown that the rms amplitudes of local angular motion do not depend strongly on the model (potential), provided that isotropic rotation around the same number of axes is allowed and that one compares rms angles of the same dimensionality. The rms amplitudes of local angular motion in solution are comparable to those observed for the same sequence at low levels of hydration in the solid state.

Base Sequence↗

PubMed1994

A solid-state 2H NMR investigation of purine motion in a 12 base pair RNA duplex.

Solid-state 2H NMR spectroscopy has been used to investigate the base dynamics of a RNA oligonucleotide with a defined sequence, [r(CGCGAAUUCGCG)]2, which contains the RNA analogue of the EcoRI binding site. The C8 protons of all purines in the self-complementary dodecamer were exchanged for deuterons. The quadrupole-echo lineshapes and spin-lattice relaxation times as a function of hydration for the sample in the form of the Na salt have previously been reported. In that study the 2H NMR lineshapes and T1 values of [r(CG*CG*A*A*UUCG*CG*)]2 were compared with those of the analogously labeled DNA sequence, [(CG*CG*A*A*TTCG*CG*)]2 (Wang et al., J. Am. Chem. Soc. 114, 6583, 1992). It was concluded that the amplitudes of purine motion for DNA and RNA are similar at all hydration levels; however, the rate difference observed at low-hydration levels may or may not persist at high hydration. Here the internal motions of the purine bases in the RNA oligomer have been thoroughly investigated. Three models were used to simulate the motion: (1) two-site jump, (2) diffusion in a cone, and (3) restricted diffusion on the surface of a cone. The purine motion is best simulated by the restricted-diffusion on a cone model with an amplitude of +/- 9.5 degrees and a rate between 8.0 x 10(6) rad/s at 90% RH and 8.4 x 10(8) rad/s at 0% RH. This small amplitude and fast rate of purine motion for RNA are similar to previous results obtained for DNA purines.

Base Sequence↗

PubMed1993

Structure of a DNA:RNA hybrid duplex. Why RNase H does not cleave pure RNA.

The solution structure of the DNA:RNA hybrid duplex d(GTCACATG):r(caugugac) has been determined by means of two-dimensional nuclear Overhauser effect (2D-NOE) spectra, restrained molecular dynamics and full-relaxation matrix stimulation of the 2D-NOE spectra. The DNA:RNA hybrid duplex assumes neither an A-form nor a B-form structure in solution, but an intermediate heteromerous duplex structure. The sugars of the RNA strand have a normal N-type C3'-endo conformation, but the DNA strand sugars have neither N-type nor S-type conformations; instead, they have an unexpected intermediate O4'-endo conformation. The negative x-displacement, as well as the small rise and positive inclination of the base-pairs, resembles A-form morphology but the minor groove width is intermediate between that of A-form and B-form duplexes. Both the DNA and RNA strands show prominent sequence-dependent variations in their helical parameters. Combined analysis of NOE and J-coupling data indicates that the DNA sugars are not in a dynamical two-state equilibrium. The detailed three-dimensional structure of this DNA:RNA hybrid molecule leads to a proposed model for its interaction with RNase H. Several specific structural features of the enzyme complexed with the hybrid duplex appear to explain the mechanism whereby RNase H discriminates between DNA:RNA hybrid duplexes and pure RNA:RNA duplexes.

Base Sequence↗

PubMed1993

Mobility at the TpA cleavage site in the T3A3-containing AhaIII and PmeI restriction sequences.

Lefevre et al. originally observed conformational transitions at the TpA step in the TTAA Pribnow box sequence of the trp promoter [Lefevre, J.-F., Lane, A. N., & Jardetzky, O. (1985) FEBS Lett. 190, 37-40]. In 500-MHz 1H NMR studies on the TnA(n)-containing DNA oligonucleotides [d(CGAGGTTTAAACCTCG)]2, [d(GCTCCTTTAAAGGAGC)]2, and [d(GCCGTTAACGGC)]2, we observe that, in addition to the H2 proton (which resides in the minor groove of DNA), the H8 proton of the first adenine (which resides in the major groove) is also broadened due to motion at the TpA junction. In analogous 16-mers where the T3A3 segment has been replaced by an A3T3 sequence, and therefore contains CA, GA, and AT steps (but no TA steps), all adenine proton resonances are narrow, indicating that the broadening occurs only at TpA steps. Assuming chemical exchange in the form of conformational dynamics, e.g., oscillation of the purine base about the glycosidic torsion angle, the experimental 500-MHz 1H T1 rho and 2D-NOESY data were used to constrain the correlation time of the internal motion to a range between the T1 and T1 rho minima. Calculated line shapes using a two-site exchange model indicate that the motion has an amplitude of 20-50 degrees with an associated tau c of ca. 1.6 x 10(-4) to 1.0 x 10(-5) s rad-1, respectively. The mobility appears to be a consequence of the structure at the TpA junction which is characterized by (1) a wide minor groove between two regions of narrow minor groove, (2) an unusual average orientation of the adenine heterocycle probably resulting from a poor base-stacking interaction of the adenine with the preceding thymine, and (3) a sharp discontinuity in the sugar conformation at the TpA step.

Base Sequence↗

PubMed1993

The DNA strand in DNA.RNA hybrid duplexes is neither B-form nor A-form in solution.

The structure of the DNA.RNA hybrid (GTCACATG).(caugugac), where lowercase letters designate RNA residues, has been determined on the basis of J-coupling analysis and 2D-NOE studies. The central hexamer in this sequence has been previously studied [Reid, D. G., Salisbury, S. A., Brown, T., Williams, D. H., Vasseur, J.-J., Rayner, B., & Imabach, J.-L. (1983) Eur. J. Biochem. 135, 307-314] via one-dimensional NOE methods and circular dichroism studies. Contrary to their results, we find that this duplex does not assume a B-form conformation in solution. Instead, the RNA residues retain their C3'-endo (A-form) conformation, as indicated by the absence of H1'-H2' couplings and by strong H6/H8 to (n-1) H2'NOEs. The sugars of the DNA residues, on the other hand, do not assume an A-form (or a B-form) conformation but an intermediate conformation in the O4'-endo range (P approximately 72-110 degrees), as indicated by the presence of strong H1'-H4' NOEs, medium-strength H2"-H3' COSY cross peaks, strong H3'-H4' DQF-COSY cross peaks, and H1'-H2' coupling constants that are of approximately the same magnitude as the H1'-H2" coupling constants. These results suggest that the RNA strand not only retains its N-type structure but also exerts an influence on the conformation of the DNA strand. Our results provide strong evidence that DNA.RNA hybrid duplexes do not assume an all-C2'-endo B-type conformation; neither do they assume an all-C3'-endo A-type conformation in solution. Furthermore, although not the main focus of this study, a comparison of the longitudinal relaxation times of the DNA and RNA residues indicates the need for extended relaxation delays in two-dimensional NMR spectra of hybrid duplexes, as has been previously observed for DNA.RNA chimeric duplexes (Wang, A. C., Kim, S.-G., Chou, S.-H., Orban, J., Flynn, P., & Reid, B. R. (1992) Biochemistry 31, 3940-3946).

Base Sequence↗

PubMed1993

Sugar conformations at hybrid duplex junctions in HIV-1 and Okazaki fragments.

We have carried out a solution study of the local conformation in a hybrid-chimeric duplex of the [sequence: see text] type (where r and D represent RNA and DNA). The object of this study was to investigate the sugar conformations at the internal junction in the hybrid-DNA octamer duplex (gccaCTGC). (GCAGTGGC)--where the lower-case letters represent RNA residues. Such duplexes represent good models for Okazaki fragments in which RNA primers are covalently extended into DNA strands during DNA replication of the lagging strand. Furthermore, this particular sequence occurs during HIV-1 retrovirus reverse transcription. The chimeric RNA-DNA strand and the complementary pure DNA strand chosen for this study result from the priming of (-)-strand DNA synthesis by tRNA(Lys) and subsequent (+)-strand DNA synthesis by reverse transcriptase prior to HIV-1 retrovirus integration. Despite the unusual specificity of the RNase H activity of reverse transcriptase, which cleaves the RNA c-a phosphodiester rather than the junction a-C linkage, we found no major structural differences among the RNA c-a phosphodiester rather than the junction a-C linkage, we found no major structural differences among the RNA sugar conformations--all RNA sugars were found in the normal C3'-endo A-form conformation. Instead, we find that the first DNA residue of the chimeric strand (5C) assumes a sugar conformation in the C4'-exo to O4'-endo range (P = 54-90 degrees). Furthermore, the hybrid segment of this duplex is more heteronomous than previously assumed for duplexes of the [sequence: see text] type.(ABSTRACT TRUNCATED AT 250 WORDS)

Base Sequence↗

PubMed1993

Sequence-selective metal ion binding to DNA oligonucleotides.

Metal ion titrations of several DNA oligonucleotides, 10 dodecamers and one decamer have been monitored by 1H NMR spectroscopy in order to elucidate metal ion binding patterns. Also, the effects of paramagnetic impurities on resonance linewidths and NOESY cross-peak intensities have been reversed by EDTA back-titration experiments. 1H 1D NMR spectra were recorded after successive additions of aliquots of different metal salts to oligonucleotide samples. Paramagnetic manganese(II) salts were used in most cases, but a few samples were also titrated with diamagnetic zinc(II). From this study, we conclude that there exists a sequence-selective metal ion binding pattern. The metal ions bind predominantly to 5'-G in the contexts 5'-GC and 5'-GA. The order of preference seems to be GG > or = GA > GT > > GC. No evidence of metal ion binding to 5'-G in 5'-GC steps or to non-G residues was found. The H6 or H8 resonances on preceding (5'-) bases were affected by the adjacent bound paramagnetic metal ion, but no effect was observed on the protons of the succeeding (3'-) base. The metal binding site in the duplexes is most likely at G-N7, as manifested by the pronounced paramagnetic line broadening or diamagnetic shift of the G-H8 signal. This sequence selectivity may be qualitatively explained by a sequence-dependent variation in the molecular electrostatic potentials of guanine residues (MEPs) along the oligonucleotide chain.

Base Sequence↗

PubMed1992

Base pairing geometry in GA mismatches depends entirely on the neighboring sequence.

We have synthesized nine self-complementary DNA oligomers containing different flanking sequences adjacent to a pair of contiguous GA mismatches, and have used high resolution nuclear magnetic resonance (n.m.r.) to investigate the GpA phosphodiester backbone conformation and mismatch pairing schemes in these duplexes. We found dramatic effects of the flanking base pair on the hydrogen bonding and backbone conformation, which appear to be coupled. Thus the Ganti-Aanti base pairing scheme in a NAGATN sequence switches to a more stable sheared GA base pairing scheme in a NCGAGN or NTGAAN context, while no duplex is formed (or only GA bulges occur) when NAGATN is changed to NGGACN. Furthermore, the more stable sheared GA pairing in NPyGAPuN sequences is associated with a BII rather than BI backbone conformation for the phosphodiester between the adjacent mismatched GA pairs. The overall stability of these adjacent GA mismatches as measured by imino proton n.m.r. studies is Py-GA-Pu > A-GA-T > G-GA-C.

Base Composition↗

PubMed1992

Solution structure of the TnAn DNA duplex GCCGTTAACGCG containing the HpaI restriction site.

The solution structure of the self-complementary DNA duplex [d(GCCGTTAACGGC)]2, which contains the HpaI restriction site GTTAAC, has been elucidated by two-dimensional NMR, distance geometry (DG), and NOE back-calculation methods. Initial distance constraints were determined by polynomial fitting the two-spin initial NOE rates; backbone constraints from NOE and J-coupling observations (Kim et al., 1992) were included. RMSDs between initial-distance-refined structures derived from random-embedded DG, A-DNA, and B-DNA starting structures were all in the range 0.5-1.0 A, indicating good convergence properties of the algorithm, regardless of the starting structure. A semiautomatic back-calculation refinement procedure was developed and used to generate more refined structures for which the BKCALC-simulated NOE volumes matched the experimental data. The six final structures refined from various starting structures exhibit very good agreement with the experimental data (R values = 0.18) and converge well to within 0.8-A RMSD differences for the central 8 base pairs. The torsion and pseudorotation phase angles were found to be well determined by the data, and the local helical parameters for each base step converged quite well. The final structures show that the central T6-A7 step is somewhat underwound (twist angle ca. 29 degrees), with a large negative cup and a normal (wide) minor groove width, while the T5-T6 and A7-A8 steps have a partially narrowed minor groove.

Base Sequence↗

PubMed1992

Solution structure of [d(GCGTATACGC)]2.

The solution structure of the alternating pyrimidine-purine DNA duplex [d(GCGTATACGC)]2 has been determined using two-dimensional nuclear magnetic resonance techniques and distance geometry methods. Backbone distance constraints derived from experimental nuclear Overhauser enhancement and J-coupling torsion angle constraints were required to adequately define the conformation of the inter-residue backbone linkages and to avoid underwinding of the duplex. The distance geometry structures were further refined by back-calculation of the two-dimensional nuclear Overhauser enhancement spectra to correct spin-diffusion distance errors. Fifteen final structures for [d(GCGTATACGC)]2 were generated from the refined experimental distance bounds. These structures all exhibit fully wound B-form geometry with small penalty values (< 1.5 A) against the distance bounds and small pair-wise root-mean-square deviation values (typically 0.6 A to 1.5 A). The final structures exhibit positive base-pair inclination with respect to the helix axis, a marked alternation in rise and twist, and are shorter and wider than classical fiber B-form DNA. The purines were found to adopt a sugar pucker close to the C-2'-endo conformation while pyrimidine sugars exhibited significantly lower pseudorotation phase angles in the C-1'-exo to C-2'-endo range. The minor groove cross-strand steric clashes at pyrimidine-purine steps that would exist in pure B-DNA are attenuated by an increased rise at these steps (and an increased roll angle at TpA steps). Concomitantly the backbone torsion angles of the pyrimidine moieties have larger gamma values, larger epsilon values, and smaller zeta values than the purines. The structures generated by distance geometry methods were also compared with those obtained from restrained molecular dynamics with empirical force-field potentials. The results indicate that the nuclear magnetic resonance/distance geometry approach alone is capable of elucidating most of the salient structural features of double-stranded helical nucleic acids in solution without resorting to empirical energy potentials and without using any structural assumptions from crystallographic data.

Base Sequence↗

PubMed1992

Solution structure of [d(ATGAGCGAATA)]2. Adjacent G:A mismatches stabilized by cross-strand base-stacking and BII phosphate groups.

The solution structure of a rather unusual B-form duplex [d(ATGAGCGAATA)]2 has been determined using two-dimensional nuclear magnetic resonance (2D-NMR) and distance geometry methods. This sequence forms a stable ten base-pair B-form duplex with 3' overhangs and two pairs of adjacent G:A mismatches paired via a sheared hydrogen-bonding scheme. All non-exchangeable protons, including the stereo-specific H-5'S/H-5'R of the 3G and 7G residues, were assigned by 2D-NMR. The phosphorus spectrum was assigned using heteronuclear correlation with H-3' and H-4' reasonances. The complete assignments reveal several unusual nuclear Overhauser enhancements (NOEs) and unusual chemical shifts for the neighboring G:A mismatch pairs and their adjacent nucleotides. Inter-proton distances were derived from time-dependent NOEs and used to generate initial structures, which were further refined by iterative back-calculation of the two-dimensional nuclear Overhauser enhancement spectra; 22 final structures were calculated from the refined distance bounds. All these final structures exhibit fully wound helical structures with small penalty values against the refined distance bounds and small pair-wise root-mean-square deviation values (typically 0.5 A to 0.9 A). The two helical strands exchange base stacking at both of the two G:A mismatch sites, resulting in base stacking down each side rather than down each strand of the twisted duplex. Very large twist angles (77 degrees) were found at the G:A mismatch steps. All the final structures were found to have BII phosphate conformations at the adjacent G:A mismatch sites, consistent with observed downfield 31P chemical shifts and Monte-Carlo conformational search results. Our results support the hypothesis that 31P chemical shifts are related to backbone torsion angles. These BII phosphate conformations in the adjacent G:A mismatch step suggest that hydrogen bonding of the G:A pair G-NH2 to a nearby phosphate oxygen atom is unlikely. The unusual structure of the duplex may be stabilized by strong interstrand base stacking as well as intrastrand stacking, as indicated by excellent base overlap within the mismatch stacks.

Base Composition↗

PubMed1992

Errors in RNA NOESY distance measurements in chimeric and hybrid duplexes: differences in RNA and DNA proton relaxation.

Nuclear magnetic resonance experiments reveal that the base H8/H6 protons of oligoribonucleotides (RNA) have T1 relaxation times that are distinctly longer than those of oligodeoxyribonucleotides (DNA). Similarly, the T1 values for the RNA H1' protons are approximately twice those of the corresponding DNA H1' protons. These relaxation differences persist in single duplexes containing covalently linked RNA and DNA segments and cause serious overestimation of distances involving RNA protons in typical NOESY spectra collected with a duty cycle of 2-3 s. NMR and circular dichroism experiments indicate that the segments of RNA maintain their A-form geometry even in the interior of DNA-RNA-DNA chimeric duplexes, suggesting that the relaxation times are correlated with the type of helix topology. The difference in local proton density is the major cause of the longer nonselective T1s of RNA compared to DNA, although small differences in internal motion cannot be completely ruled out. Fortunately, any internal motion differences that might exist are shown to be too small to affect cross-relaxation rates, and therefore reliable distance data can be obtained from time-dependent NOESY data sets provided an adequately long relaxation delay is used. In hybrid or chimeric RNA-DNA duplexes, if the longer RNA relaxation times are not taken into account in the recycle delay of NOESY pulse sequences, serious errors in measuring RNA proton distances are introduced.

Base Sequence↗

PubMed1992

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.

Base Sequence↗