Two-dimensional Nuclear Overhauser Enhancement Spectroscopy Research Articles

Pyrimidine · pyrimidine base-pair mismatches in DNA: A nuclear magnetic resonance study of T · T pairing at neutral pH and C · C pairing at acidic pH in dodecanucleotide duplexes

Structural features of pyrimidine · pyrimidine mismatches in the interior of oligonucleotide duplexes have been investigated by high resolution two-dimensional proton nuclear magnetic resonance (n.m.r.) spectroscopy. These studies were conducted on the self-complementary d( C-G-C- T A-G-C-T- T -G-C-G ) duplex (designated T · T 12-mer) and the self-complementary d( C-G-C- C -A-G-C-T- C -G-C-G ) duplex (designated C · C 12-mer) containing T · T and C · C pairs located at identical positions four base-pairs from either end of the duplex. Proton n.m.r. studies on the T · T 12-mer duplex were undertaken in the neutral pH range, while studies on the C · C 12-mer duplex were recorded at acidic pH. The proton spectra narrowed considerably on lowering the pH below neutrality for the C · C 12-mer duplex. Two-dimensional nuclear Overhauser enhancement spectroscopy (NOESY) data sets have been recorded on the T · T 12-mer and C · C 12-mer duplexes in high salt H 2O and D 2O solution. The magnitude of the NOE crosspeaks and the directionality of the NOE connectivities demonstrate that both duplexes are right-handed with all bases, including those at the mismatch site, adopting an anti configuration about the glycosidic bond. The observed base and sugar proton chemical shifts suggest structural similarities for the trinucleotide segments centered about the T · T and C · C mismatches. A NOE is detected between the resolved imino protons of T4 and T9 at the mismatch site, consistent with formation of a stacked “wobble” T4( anti) · T9( anti) pair in the T · T 12-mer duplex. A comparison of the imino proton chemical shift and NOE data suggests that the imino-carbonyl hydrogen bonds in the wobble T · T mismatch are weaker than the corresponding imino-carbonyl hydrogen bonds in the wobble G · T mismatch. The 4-amino protons of C4 and C9 at the mismatch site in the C · C 12-mer duplex do not exhibit the pattern of hydrogen-bonded and exposed protons separated by approximately 1·5 parts per million characteristic of cytidine amino protons involved in Watson-Crick G · C pairing. The experimental data are insufficient to differentiate between wobble C( anti) · C + ( anti) and other pairing possibilities for the mismatch in the C · C 12-mer duplex at acidic pH.

Selective reversible deuteriation of oligodeoxynucleotides: simplification of two-dimensional nuclear Overhauser effect NMR spectral assignment of a non-self-complementary dodecamer duplex.

Oligodeoxynucleotides are reversibly deuteriated at the purine C8 and cytosine C5 positions with deuterioammonium bisulfite at pD 7.8. The exchange reaction is complete after 48 h at 65 degrees C. When an oligomer deuteriated under these conditions is analyzed by 1H nuclear magnetic resonance (NMR) spectroscopy, the purine H8 and cytosine H5 proton signals are selectively removed from the spectrum. A non-self-complementary oligodeoxynucleotide that has been deuteriated in this manner may be annealed with its complement and the resulting heteroduplex analyzed by two-dimensional nuclear Overhauser enhancement (NOESY) spectroscopy. NOE cross-peaks arising from pyrimidine H6-deoxyribose H1' dipolar interactions in both strands are observed, but purine H8-deoxyribose H1' and purine H8-deoxyribose H2',H2" dipolar interactions are only observed for the nondeuteriated strand. The intense cytosine H5-H6 cross-peaks are also removed from the spectrum of the deuteriated strand, which further simplifies interpretation since these strong cross-peaks often interfere with less intense NOE cross-peaks arising from dipolar coupling between purine H8 or pyrimidine H6 and deoxyribose anomeric protons. The resulting spectral simplification allows unambiguous assignments to be made on NOEs that otherwise may be difficult to distinguish. The deuteration procedure is demonstrated with the sequence d(CGTTATAATGCG).d(CGCATTATAACG), which has previously been assigned by traditional NOESY methods [Wemmer, D. E., Chou, S.-H., Hare, D. R., & Reid, B. R. (1984) Biochemistry 23, 2262-2268]. Although the assignment of this dodecadeoxynucleotide may be completed without deuteriation, several NOEs must be assigned indirectly because of degeneracies in the chemical shift of the purine H8 protons.(ABSTRACT TRUNCATED AT 250 WORDS)

Refinement of the solution structure of the DNA decamer 5'd(CTGGATCCAG)2: combined use of nuclear magnetic resonance and restrained molecular dynamics.

The solution structure of the self-complementary DNA decamer 5'd(CTGGATCCAG)2 comprising the specific target site for the restriction endonuclease BamH1 is investigated by using nuclear magnetic resonance sectroscopy and restrained molecular dynamics. With the exception of the H5'/H5" sugar proton resonances, all the nonexchangeable proton resonances are assigned sequentially by using pure-phase absorption two-dimensional nuclear Overhauser enhancement spectroscopy. From the time dependence of the nuclear Overhauser effects a set of 160 approximate interproton distances is determined and used as the basis of a structure refinement employing restrained molecular dynamics in which the interproton distances are incorporated into the total energy function of the system in the form of an effective potential term. Two restrained dynamics simulations are carried out, starting from classical B- and A-DNA [atomic root mean square (rms) difference 5.7 A]. In both cases convergence is achieved to very similar B-type structures with an atomic rms difference of 0.9 A which is comparable to the rms fluctuations of the atoms about their average positions. In addition, the rms difference between the experimental and calculated values of the interproton distances for both average restrained dynamics structures is approximately 0.3 A. These results suggest that the converged restrained molecular dynamics structures represent reasonable approximations of the solution structure. The average restrained dynamics structures exhibit clear sequence-dependent variations of torsion angles and helical parameters. In addition, the structures exhibit a small bend of around 10-20 degrees at the second (TpG) and eighth (CpA) base pair steps. This can be attributed to the positive base roll angles and large base pair slide values at the two Pyr-Pur steps. The central core of the decamer comprising the six-base recognition site for BamH1 (GGATCC), however, is straight.

Method of Determining Protein Conformations by the Two-Dimensional Nuclear Overhauser Enhancement Spectroscopy Data

A method is suggested to determine the most probable values of the angles phi, psi of the protein backbone by the data on the availability and absence of d connectivities in the two-dimensional nuclear Overhauser enhancement spectra. In view of this, the dependences of the proton-proton distances in dipeptide units of L-amino acid residues on the dihedral angles phi, psi, chi1 are considered and the conformational states of amino acid residues of the proteins with the known spatial structure are analysed statistically. The potentialities of the method are assessed with the aid of model spectral nuclear magnetic resonance (NMR) parameters obtained from the X-ray data for the bovine pancreatic trypsin inhibitor and avian pancreatic polypeptide. It is shown that the developed procedure of structural interpretation of the NMR data allows one to correctly reproduce the local conformation of the protein backbone. The obtained backbone conformation may serve as a starting point to build and refine molecular three-dimensional structure.

Conformational changes in the oligonucleotide duples d(GCGTTGCG). d (CGCAACGC) induced by formation of a cis‐syn thymine dimer

In order to obtain insight into the repair mechanism of DNA containing thymine photo-dimer, the conformation of the duplex d(GCGTTGCG) x d(CGCAACGC) with a thymine dimer incorporated has been studied by proton NMR and the results are compared with NMR data of the parent octamer. Two-dimensional nuclear Overhauser enhancement (2D NOE) spectroscopy and two-dimensional homonuclear Hartmann-Hahn spectroscopy have been applied to assign all the non-exchangeable base protons and most of the deoxyribose protons of both duplexes. From these experiments it is clear that indeed a cis-syn cyclobutane-type thymine photodimer is formed by the irradiation of this oligonucleotide with ultraviolet light. Comparison of 2D NOE spectra and the 1H chemical shifts of the damaged and the intact DNA duplexes reveals that formation of a thymine dimer induces small distortions of the B-DNA structure, the main conformational change occurring at the site of the thymine dimer.

Conversions of poly(2-aminodeoxyadenylate-5-halodeoxyuridylate) from B to A forms in high salt. An NMR and circular dichroism study.

Proton one- and two-dimensional nuclear Overhauser enhancement (1D and 2D NOE) spectroscopy has been used to demonstrate that poly(d2NH2A-d5IU) and poly(d2NH2A-d5BrU) are converted from the B to the A conformation in high salt, as found previously for poly(d2NH2A-dT) [Borah, B., Cohen, J. S., Howard, F. B., & Miles, H. T. (1985) Biochemistry 24, 7456-7462]. The 2D NOE and 1D NOE spectra exhibit strong base proton (H8,H6)-H3' cross relaxation, suggesting short interproton distances. These results are indicative of a C3'-endo sugar pucker for both purine and pyrimidine residues in an A or closely related structure. The circular dichroism and UV spectra are consistent with the interpretation of an A conformation in high salt.

The B and Z forms of the d(m5C-G)3 and d(br5C-G)3 hexamers in solution. A 300-MHz and 500-MHz two-dimensional NMR study.

The non-exchangeable proton resonances of the hexadeoxynucleoside pentakisphosphates d(m5C-G)3 and d(br5C-G)3 in the B form as well as in the Z form were assigned by means of two-dimensional correlated spectroscopy and two-dimensional nuclear Overhauser enhancement spectroscopy. The complete proton NMR spectrum of the B form of the methylated compound was assigned in a pure 2H2O solution as well as in a 2H2O/C2H3O2H mixed solvent, containing 5 mM MgCl2. In the latter solvent the B form occurs in slow equilibrium (on the NMR time scale) with the Z form, the resonances of which also were fully assigned. The proton resonances of the B and Z forms of the brominated fragment were assigned in a 2H2O/C2H3O2H solution containing 5 mM MgCl2. A new and general method is described for the sequential assignment of the non-exchangeable proton resonances of oligonucleotides in the Z form.

Amide proton exchange in proteins by EX1 kinetics: studies of the basic pancreatic trypsin inhibitor at variable p2H and temperature

With the use of one-dimensional 1H nuclear magnetic resonance, two-dimensional correlated spectroscopy, and two-dimensional nuclear Overhauser enhancement spectroscopy, the exchange mechanisms for numerous individual amide protons in the basic pancreatic trypsin inhibitor (BPTI) were investigated over a wide range of p2H and temperature. Correlated exchange under an EX1 regime was observed only for the most slowly exchanging protons in the central hydrogen bonds of the antiparallel beta-sheet and only over a narrow range of temperature and p2H, i.e., above ca. 55 degrees C and between p2H 7 and 9, where the opening rates of the structure fluctuations which promote the exchange of these protons are of the order 0.1 min-1. At p2H below 7, the exchange of this most stable group of protons is uncorrelated and is governed by an EX2 mechanism. At p2H above 9, the exchange is also uncorrelated and occurs via either EX2 or EX1 processes promoted by strictly local structure fluctuations. For all other backbone amide protons in BPTI, the exchange was found to be uncorrelated and by an EX2 mechanism under all conditions of p2H and temperature where quantitative measurements could be obtained with the methods used, i.e., for kex approximately less than 5 min-1. From these observations with BPTI it can be concluded that the amide proton exchange in globular proteins is quite generally via EX2 processes, with rare exceptions for measurements with extremely stable protons at high temperature and basic p2H. This emphasizes the need for further development of suitable concepts for the structural interpretation of EX2 amide proton exchange [Wagner, G. (1983) Q. Rev. Biophys. 16, 1-57; Wagner, G., Stassinopoulou, C. I., & Wüthrich, K. (1984) Eur. J. Biochem. 145, 431-436] and for more detailed investigations of the intrinsic exchange rates for solvent-exposed amide protons in the "open" states of a protein [Roder, H., Wagner, G., & Wüthrich, K. (1985) Biochemistry (following paper in this issue)].

Investigation of the solution structure of a DNA octamer [d(GGAATTCC)]2 using two-dimensional nuclear Overhauser enhancement spectroscopy.

Proton two-dimensional nuclear Overhauser enhancement (2D NOE) spectra in the pure absorption phase were obtained at 500 MHz for [d(GGAATTCC)]2 in aqueous solution at a series of mixing times. The experimental data were analyzed by comparison with theoretical spectra calculated using the complete 70 X 70 relaxation matrix including all proton dipole-dipole interactions and spin diffusion [Keepers, J. W. & James, T. L. (1984) J. Magn. Reson. 57, 404-426]. The theoretical spectra at each mixing time were calculated using two structures: a standard B-form DNA structure and an energy-minimized structure based on the similarity of the six internal residues of the title octamer with those of the dodecamer [d(CGCGAATTCGCG)]2, for which the crystal structure has been determined. Neither the standard B-form nor the energy-minimized structure will yield theoretical 2D NOE spectra which accurately reproduce all peak intensities in the experimental spectra. However, many features of the experimental spectra can be represented by both the B-form and the energy-minimized structure. Sequence-dependent structural characteristics are manifest in the 2D NOE spectra, in particular at the purine-pyrimidine junction as noted previously in the crystal structure. On the whole, the energy-minimized structure appears to yield theoretical 2D NOE spectra which mimic many, if not all, aspects of the experimental spectra. All 2D NOE data were consistent with nanosecond correction times as implied by proton spin-lattice relaxation time measurements. But better fits of some of the 2D NOE data using small variations in an effective isotropic correlation time suggest that there may be some local variations in mobility within the octamer duplex structure in solution.

Imino-proton resonances of yeast tRNAPhe studied by two-dimensional nuclear Overhauser enhancement spectroscopy.

Application of two-dimensional nuclear Overhauser enhancement (NOE) spectroscopy to yeast tRNAPhe in H2O solution demonstrates that all imino-proton resonances, related to the secondary structure, and nearly all imino proton resonances, originating from the tertiary structure, can be assigned efficiently by this method. The results corroborate the assignments of the imino-proton resonances of this tRNA as established previously by one-dimensional NOE experiments (only the assignment of base pairs G1 X C72 and C2 X G71 should be reversed). The advantages of two-dimensional NOE spectroscopy over one-dimensional NOE spectroscopy for the assignments of imino-proton resonances and the structure elucidation of tRNA are illustrated and discussed. Furthermore, the use of non-exchangeable proton resonances as probes of the molecular structure is explored.

Solution conformation of proteinase inhibitor IIA from bull seminal plasma by 1H nuclear magnetic resonance and distance geometry

A determination of the solution conformation of the proteinase inhibitor IIA from bull seminal plasma (BUSI IIA) is described. Two-dimensional nuclear Overhauser enhancement spectroscopy (NOESY) was used to obtain a list of 202 distance constraints between individually assigned hydrogen atoms of the polypeptide chain, to identify the positions of the three disulfide bridges, and to locate the single cis peptide bond. Supplementary geometric constraints were derived from the vicinal spin-spin couplings and the locations of certain hydrogen bonds, as determined by nuclear magnetic resonance (n.m.r.). Using a new distance geometry program (DISGEO) which is capable of computing all-atom structures for proteins the size of BUSI IIA, five conformers were computed from the NOE distance constraints alone, and another five were computed with the supplementary constraints included. Comparison of the different structures computed from the n.m.r. data among themselves and with the crystal structures of two homologous proteins shows that the global features of the conformation of BUSI IIA (i.e. the overall dimensions of the molecule and the threading of the polypeptide chain) were well-defined by the available n.m.r. data. In the Appendix, we describe a preliminary energy refinement of the structure, which showed that the constraints derived from the n.m.r. data are compatible with a low energy spatial structure.

A two-dimensional NMR study of the solution structure of a DNA dodecamer comprising the concensus sequence for the specific DNA-binding sites of the glucocorticoid receptor protein.

A two-dimensional 500-MHz 1H-NMR study on the non-self-complementary double-stranded DNA dodecamer 5'd(C-C-A-G-A-A-C-A-G-T-G-G)5'd(C-C-A-C-T-G-T-T-C-T-G-G), is presented. This oligonucleotide contains the consensus octanucleotide sequence 5'd(A-G-A-A-C-A-G-T) for the specific DNA-binding sites of the glucocorticoid receptor protein [Payvar, F. et al. (1984) Cell 35, 381-392]. Using a combination of two-dimensional pure phase absorption nuclear Overhauser enhancement (NOESY) and homonuclear J-correlated (COSY) spectroscopy all non-exchangeable base (with the exception fo the adenine H2 protons), methyl and deoxyribose H1', H2', H2", H3' and H4' resonances are assigned unambiguously using a sequential resonance assignment strategy. From the relative intensities of the cross peaks in the pure phase absorption NOESY spectra at two mixing times it is shown that the dodecamer adopts a B-type conformation in solution.

A distance geometry program for determining the structures of small proteins and other macromolecules from nuclear magnetic resonance measurements of intramolecular 1H- 1H proximities in solution

DISGEO is a new implementation of a distance geometry algorithm which has been specialized for the calculation of macromolecular conformation from distance measurements obtained by two-dimensional nuclear Overhauser enhancement spectroscopy. The improvements include (1) a decomposition of the complete embedding process into two successive, more tractable calculations by the use of “substructures”, (2) a compact data structure for storing incomplete distance information on a structure, (3) a more efficient shortest-path algorithm for computing the triangle inequality limits on all distances from this information, (4) a new algorithm for selecting random metric spaces from within these limits, (5) the use of chirality constraints to obtain good covalent geometry without the use of ad hoc weights or excessive optimization. The utility of the resultant program with nuclear magnetic resonance data is demonstrated by embedding complete spatial structures for the protein basic pancreatic trypsin inhibitor vs all 508 intramolecular, interresidue proton-proton contacts shorter than 4.0 A that were present in its crystal structure. The crystal structure could be reproduced from this data set to within 1.3 A minimum root mean square coordinate difference between the backbone atoms. We conclude that the information potentially available from nuclear magnetic resonance experiments in solution is sufficient to define the spatial structure of small proteins.

Conformation of glucagon in a lipid-water interphase by 1H nuclear magnetic resonance

A determination of the spatial structure of the polypeptide hormone glucagon bound to perdeuterated dodecylphosphocholine micelles is described. A map of distance constraints between individually assigned hydrogen atoms of the polypeptide chain was obtained from two-dimensional nuclear Overhauser enhancement spectroscopy. These data were used as the input for a distance geometry algorithm for computing conformations that would be compatible with the experiments. In the region from residues 5 to 29 the mobility of the polypeptide backbone and most of the amino acid side-chains was found to be essentially restricted to the overall rotational tumbling of the micelles. The secondary structure in this region includes three turns of irregular alpha-helix in the segment of residues 17 to 29 near the C terminus, a stretch of extended polypeptide chain from residues 14 to 17, an alpha-helix-like turn formed by the residues 10 to 14 and another extended region from residues 5 to 10. In the N-terminal tetrapeptide H-His-Ser-Gln-Gly- the two terminal residues are highly mobile, indicating that they extend into the aqueous phase, and the mobility of the residues Gln3 and Gly4 appears to be only partially restricted by the binding to the micelle. The absence of long range nuclear Overhauser effects between the peptide segments 5-9 and 11-29, and between 5-16 and 19-29 shows that the polypeptide chain does not fold back on itself and hence that micelle-bound glucagon does not adopt a globular tertiary structure. Previously it was shown that the polypeptide backbone of glucagon is located close to and runs roughly parallel to the micelle surface. Combination of these observations suggests that the overall spatial arrangement of the glucagon polypeptide chain in a lipid-water interphase is largely determined by the topology of the lipid support, in the present case the curvature of the dodecylphosphocholine micelles. The tertiary structure is further characterized by the formation of two hydrophobic patches by the side-chains of Phe6, Tyr10 and Leu14, and the side-chains of Ala19, Phe22, Val23, Trp25 and Leu26, respectively.

Buildup rates of the nuclear Overhauser effect measured by two-dimensional proton magnetic resonance spectroscopy: implications for studies of protein conformation

It is demonstrated, by means of experiments with the basic pancreatic trypsin inhibitor, that the buildup rates of the nuclear Overhauser effect can be measured by two-dimensional NMR spectroscopy. Qualitative correlations between the buildup rates of first-order Overhauser effects, which arise from direct dipole-dipole coupling between closely spaced protons, and the proton-proton distances in the protein conformation are established. Second-order Overhauser effects due to spin diffusion by cross-relaxation between more distant protons are also identified. On the basis of these observations, potentialities and limitations of two-dimensional nuclear Overhauser enhancement spectroscopy for studies of the conformation of biological macromolecules are discussed and suggestions made for improved experimental procedures. For quantitative measurements of Overhauser effects, the use of phase-sensitive spectra and of techniques for selective suppression of J cross-peaks in data sets recorded with very short mixing times appears particularly important.

Systematic application of two-dimensional 1H nuclear-magnetic-resonance techniques for studies of proteins. 2. Combined use of correlated spectroscopy and nuclear Overhauser spectroscopy for sequential assignments of backbone resonances and elucidation of polypeptide secondary structures.

This paper describes a new nuclear magnetic resonance approach for the determination of secondary structure in globular proteins. To illustrate the practical application of the new procedure, two-dimensional correlated spectroscopy and two-dimensional nuclear Overhauser enhancement spectroscopy were used to obtain individual assignments for all the backbone protons of the beta-sheet secondary structures in the basic pancreatic trypsin inhibitor. First, combined connectivity diagrams of these two methods recorded in both 2H2O solution and H2O solution of the inhibitor were employed to obtain sequential, individual resonance assignments for the separate strands in the beta sheet. Second, a 2D nuclear Overhauser enhancement spectrum recorded with a long mixing time was used to determine how the separate, extended polypeptide strands are linked by hydrogen bonds in the sheet structures. By combination of these results with the identifications of the amino acid side-chain resonances described in the preceding paper, the beta-sheet structures can, without reference to data on the spatial structure obtained with other techniques, be localized in the amino acid sequence. This investigation confirms results on limited regions of the beta sheet in the inhibitor obtained previously with one-dimensional nuclear magnetic resonance experiments and demonstrates that the entire beta-sheet structure seen in single crystals of the inhibitor is preserved in aqueous solution.