Conformation of a bulge-containing oligomer from a hot-spot sequence by NMR and energy minimization

Two-dimensional nmr data on a bulge-containing oligodeoxyribonucleotide, 5'dGATGGGCAG.dCTGACCCATC, and a regular oligomer of similar sequence, 5'dGATGGCAG.dCTGCCATC, are presented. The nonexchangeable protons are assigned from sequential nuclear Overhauser effect spectroscopy (NOESY) connectivities. The two-dimensional NOE (NOESY) and correlated (COSY) spectra of the bulge-containing oligomer are compared to those of the perfect 8-mer. Experimental proton-proton distances are determined from NOESY spectra acquired with mixing times of 100, 150, and 200 ms, using comparable distances in the B-DNA region of the molecule as a calibration. With this approach, measured distances do not depend systematically on mixing time. Energy minimization techniques are used to calculate a three-dimensional structure for the bulge-containing oligomer in agreement with the nmr data. The helix is of the B family, with the extra adenine stacked into the helix, and the helix axis is bent by 20 degrees.     

Solution structure of a trinucleotide A-T-A bulge loop within a DNA duplex.

We have synthesized an oligodeoxynucleotide duplex, d(G-C-A-T-C-G-A-T-A-G-C-T-A-C-G).d(C-G-T-A-G-C-C-G-A-T-C-G), with a three-base bulge loop (A-T-A) at a central site in the first strand. Nuclear Overhauser experiments (NOESY) in H2O indicate that the GC base pairs flanking the bulge loop are intact between 0 and 25 degrees C. Nuclear Overhauser effects in both H2O and D2O indicate that all bases within the bulge loop are stacked into the helix. These unpaired bases retain an anti conformation about their glycosidic bonds as they stack within the duplex. The absence of normal sequential connectivities between the two cytosine residues flanking the bulge site on the opposite strand indicates a disruption in the geometry of this base step upon insertion of the bulged bases into the helix. This conformational perturbation is more akin to a shearing apart of the bases, which laterally separates the two halves of the molecule, rather than the "wedge" model often invoked for single-base bulges. Using molecular dynamics calculations, with both NOE-derived proton-proton distances and relaxation matrix-calculated NOESY cross peak volumes as restraints, we have determined the solution structure of an A-T-A bulge loop within a DNA duplex. The bulged bases are stacked among themselves and with the guanine bases on either side of the loop. All three of the bulged bases are displaced by 2-3 A into the major groove, increasing the solvent accessibility of these residues. The ATA-bulge duplex is significantly kinked at the site of the lesion, in agreement with previously reported electron microscopy and gel retardation studies on bulge-containing duplexes [Hsieh, C.-H., & Griffith, J. D. (1989) Proc. Natl. Acad. Sci. U.S.A 86, 4833-4837; Bhattacharyya, A., & Lilley, D. M. J. (1989) Nucleic Acids Res. 17, 6821-6840]. Bending occurs in a direction away from the bulge-containing strand, and we find a significant twist difference of 84 degrees between the two base pairs flanking the bulge loop site. This value represents 58% of the twist difference for base pairs four steps apart in B-DNA. These results suggest a structural mechanism for the bending of DNA induced by unpaired bases, as well as accounting for the effect bulge loops may have on the secondary and tertiary structures of nucleic acids.     

2'-deoxyribonolactone lesion in DNA: refined solution structure determined by nuclear magnetic resonance and molecular modeling

The solution conformation of the DNA duplex d(C1G2C3A4C5L6C7A8C9G10C11).d(G12C13G14T15G16T17G18T19G20C21G22 ) containing the 2'-deoxyribonolactone lesion (L6) in the middle of the sequence has been investigated by NMR spectroscopy and restrained molecular dynamics calculations. Interproton distances have been obtained by complete relaxation matrix analysis of the NOESY cross-peak intensities. These distances, along with torsion angles for sugar rings and additional data derived from canonical A- and B-DNA, have been used for structure refinement by restrained molecular dynamics (rMD). Six rMD simulations have been carried out starting from both regular A- and B-DNA forms. The pairwise rms deviations calculated for each refined structure are <1 A, indicating convergence to essentially the same geometry. The accuracy of the rMD structures has been assessed by complete relaxation matrix back-calculation. The average sixth-root residual index (Rx = 0.052 +/- 0.003) indicated that a good fit between experimental and calculated NOESY spectra has been achieved. Detailed analysis revealed a right-handed DNA conformation for the duplex in which both the T17 nucleotide opposite the abasic site and the lactone ring are located inside the helix. No kinking is observed for this molecule, even at the abasic site step. This structure is compared to that of the oligonucleotide with the identical sequence containing the stable tetrahydrofuran abasic site analogue that we reported previously [Coppel, Y., Berthet, N., Coulombeau, C., Coulombeau, Ce., Garcia, J., and Lhomme, J. (1997) Biochemistry 36, 4817-4830].     

Hybrid hexanucleotide duplex containing cyclonucleotides and deoxynucleotides: the d(TA) segment can adopt a high anti left-handed double-helical structure

It is known that oligonucleotides containing cyclonucleosides with a high anti (intermediate between anti and syn) glycosidic conformation adopt left-handed, single- and double-helical structures [Uesugi, S., Yano, J., Yano, E., & Ikehara, M. (1977) J. Am. Chem. Soc. 99, 2313-2323]. In order to see whether DNA can adopt the high anti left-handed double-helical structure or not, a self-complementary hexanucleotide containing 6,2'-O-cyclocytidine (C(o)), 8,2'-O-cycloguanosine (G(o)), thymidine, and deoxyadenosine, C(o)G(o)dTdAC(o)G(o), was synthesized. Imino proton NMR spectra and the results of nuclear Overhauser effect experiments strongly suggest that C(o)G(o)dTdAC(o)G(o) adopts a left-handed double-helical structure where the deoxynucleoside residues are involved in hydrogen bonding and take a high anti glycosidic conformation. A conformational model of the left-handed duplex was obtained by calculation with energy minimization. Thus it appears that DNA can form a high anti, left-handed double helix under some constrained conditions, which is quite different from that of Z-DNA.     

NMR studies of the exocyclic 1,N6-ethenodeoxyadenosine adduct (epsilon dA) opposite thymidine in a DNA duplex. Nonplanar alignment of epsilon dA(anti) and dT(anti) at the lesion site

Two-dimensional proton NMR studies are reported on the complementary d(C-A-T-G-T-G-T-A-C).d(G-T-A-C-epsilon A-C-A-T-G) nonanucleotide duplex (designated epsilon dA.dT 9-mer duplex) containing 1,N6-ethenodeoxyadenosine (epsilon dA), a carcinogen-DNA adduct, positioned opposite thymidine in the center of the helix. Our NMR studies have focused on the conformation of the epsilon dA.dT 9-mer duplex at neutral pH with emphasis on defining the alignment at the dT5.epsilon dA14 lesion site. The through-space NOE distance connectivities establish that both dT5 and epsilon dA14 adopt anti glycosidic torsion angles, are directed into the interior of the helix, and stack with flanking Watson-Crick dG4.dC15 and dG6.dC13 pairs. Furthermore, the d(G4-T5-G6).d(C13-epsilon A14-C15) trinucleotide segment centered about the dT5.epsilon dA14 lesion site adopts a right-handed helical conformation in solution. Energy minimization computations were undertaken starting from six different alignments of dT5(anti) and epsilon dA14(anti) at the lesion site and were guided by distance constraints defined by lower and upper bounds estimated from NOESY data sets on the epsilon dA.dT 9-mer duplex. Two families of energy-minimized structures were identified with the dT5 displaced toward either the flanking dG4.dC15 or the dG6.dC13 base pair. These structures can be differentiated on the basis of the observed NOEs from the imino proton of dT5 to the imino proton of dG4 but not dG6 and to the amino protons of dC15 but not dC13 that were not included in the constraints data set used in energy minimization. Our NMR data are consistent with a nonplanar alignment of epsilon dA14(anti) and dT5(anti) with dT5 displaced toward the flanking dG4.dC15 base pair within the d(G4-T5-G6).d(C13-epsilon A14-C15) segment of the epsilon dA.dT 9-mer duplex.     

Binding of 9-aminoacridine to bulged-base DNA oligomers from a frame-shift hot spot

Complexes of 9-aminoacridine and two derivatives with oligomers based on the sequence of a hot spot for frame-shift mutations, 5'dGATGGGGCAG, are investigated by proton NMR and equilibrium dialysis. Competition dialysis experiments show that the drug binds bulge-containing oligomers more strongly than regular duplexes of similar sequence and length, with one apparent strong site. A duplex containing an extra cytidine in a run of C's has the highest affinity for 9-aminoacridine among the sequences tested. An oligomer containing five consecutive G.C pairs shows cooperative drug binding, indicating that G tracts of this length may have an altered helical structure. Complexes of a regular 8-mer and a 9-mer containing a bulged guanosine are examined in detail by two-dimensional NMR techniques. 9-Aminoacridine preferentially binds at TpG sites in the 8-mer but binds primarily at the bulged guanosine in the G-bulge 9-mer. Drug-DNA NOE's in the 8-mer complex are compared with the crystal structure of 9-aminoacridine and 5-iodo-CpG [Sakore et al. (1979) J. Mol. Biol. 135, 763-785]. The NMR data suggest that the drug intercalates across the base pairs of both strands with the amino group projecting into the minor groove.     

NMR studies of abasic sites in DNA duplexes: deoxyadenosine stacks into the helix opposite acyclic lesions

Proton and phosphorus NMR studies are reported for two complementary nonanucleotide duplexes containing acyclic abasic sites. The first duplex, d(C-A-T-G-A-G-T-A-C).d(G-T-A-C-P-C-A-T-G), contains an acyclic propanyl moiety, P, located opposite a deoxyadenosine at the center of the helix (designated APP 9-mer duplex). The second duplex, d(C-A-T-G-A-G-T-A-C).d(G-T-A-C-E-C-A-T-G), contains a similarly located acyclic ethanyl moiety, E (designated APE 9-mer duplex). The ethanyl moiety is one carbon shorter than the natural carbon-phosphodiester backbone of a single nucleotide unit of DNA. The majority of the exchangeable and nonexchangeable base and sugar protons in both the APP 9-mer and APE 9-mer duplexes, including those at the abasic site, have been assigned by recording and analyzing two-dimensional phase-sensitive NOESY data sets in H2O and D2O solution between -5 and 5 degrees C. These spectroscopic observations establish that A5 inserts into the helix opposite the abasic site (P14 and E14) and stacks between the flanking G4.C15 and G6.C13 Watson-Crick base pairs in both the APP 9-mer and APE 9-mer duplexes. The helix is right-handed at and adjacent to the abasic site, and all glycosidic torsion angles are anti in both 9-mer duplexes. Proton NMR parameters for the APP 9-mer and APE 9-mer duplexes are similar to those reported previously for the APF 9-mer duplex (F = furan) in which a cyclic analogue of deoxyribose was embedded in an otherwise identical DNA sequence [Kalnik, M. W., Chang, C. N., Grollman, A. P., & Patel, D. J. (1988) Biochemistry 27, 924-931]. These proton NMR experiments demonstrate that the structures at abasic sites are very similar whether the five-membered ring is open or closed or whether the phosphodiester backbone is shortened by one carbon atom. Phosphorus spectra of the APP 9-mer and APE 9-mer duplexes (5 degrees C) indicate that the backbone conformation is similarly perturbed at three phosphodiester backbone torsion angles. These same torsion angles are also distorted in the APF 9-mer but assume a different conformation than those in the APP 9-mer and APE 9-mer duplexes.     

NMR studies of the interaction of chromomycin A3 with small DNA duplexes. Binding to GC-containing sequences

The interaction of chromomycin A3 with the oligodeoxyribonucleotides 1, d(ATGCAT), 2, d(ATCGAT), 3, d(TATGCATA), and 4, d(ATAGCTAT), has been investigated by 1H and 31P NMR. In the presence of Mg2+, chromomycin binds strongly to the three GC-containing oligomers 1, 3, and 4 but not to the CG-containing oligomer 2. The proton chemical shift changes for 1 and 3 are similar, and these DNA duplexes appear to bind with a stoichiometry of 2 drugs:1 Mg2+:1 duplex. The same stoichiometry of 2 drugs:1 duplex is confirmed with 4; however, proton chemical shift changes differ. An overall C2 symmetry is exhibited by the drug complex with 1, 3, and 4. At a molar ratio of 2.0 (drugs:duplex), no free DNA proton NMR signals remain. Two-dimensional nuclear Overhauser exchange spectroscopy (NOESY) of the saturated chromomycin complex with 1 and 3 positions both chromomycinone hydroxyls and the E carbohydrates in the minor groove and provides evidence suggesting that the B carbohydrates lie on the major-groove side. This is supported by several dipolar coupling cross-peaks between the drug and the DNA duplex. Drug-induced conformational changes in duplex 1 are evaluated over a range of NOESY mixing times and found to possess some characteristics of both B-DNA and A-DNA, where the minor groove is wider and shallower. A widening of the minor groove is essential for the DNA duplex to accommodate two drug molecules. This current minor-groove model is a substantial revision of our earlier major-groove model [Keniry, M.A., Brown, S.C., Berman, E., & Shafer, R.H. (1987) Biochemistry 26, 1058-1067] and is in agreement with the model recently proposed by Gao and Patel [Gao, X., & Patel, D. J. (1989a) Biochemistry 28, 751-762].     

An abasic site in DNA. Solution conformation determined by proton NMR and molecular mechanics calculations

We have determined the three-dimensional structure of a non-selfcomplementary nonanucleotide duplex which contains an abasic (apyrimidinic) site in the centre, i.e. a deoxyribose residue opposite an adenosine. The majority of the base and sugar proton resonances were assigned by NOESY, COSY and 2DQF spectra in D2O and H2O. We have measured the initial slope of buildup of NOEs in NOESY spectra at very short mixing times (25 to 50 ms), and from these were able to establish interproton distances for the central part of the duplex. We propose a different strategy for proton-proton distance determinations which takes into account the observed variations in correlation times for particular proton-proton vectors. A set of 31 measured interproton distances was incorporated into the refinement of the oligonucleotide structure by molecular mechanics calculations. Two structures were obtained which retain all aspects of a classical B DNA in which the unpaired adenine and the abasic deoxyribose lie inside the helix. We observe that the non-hydrogen bonded adenine is held well in the helix, the Tm of this base being the same as that of the A.T base pairs in the same duplex.     

NMR studies of abasic sites in DNA duplexes: deoxyadenosine stacks into the helix opposite the cyclic analogue of 2-deoxyribose

Proton and phosphorus NMR studies are reported for the complementary d(C-A-T-G-A-G-T-A-C).d(G-T-A-C-F-C-A-T-G) nonanucleotide duplex (designated APF 9-mer duplex) which contains a stable abasic site analogue, F, in the center of the helix. This oligodeoxynucleotide contains a modified tetrahydrofuran moiety, isosteric with 2-deoxyribofuranose, which serves as a structural analogue of a natural apurinic/apyrimidinic site [Takeshita, M., Chang, C.N., Johnson, F., Will, S., & Grollman, A.P. (1987) J. Biol. Chem. 262, 10171-10179]. Exchangeable and nonexchangeable base and sugar protons, including those located at the abasic site, have been assigned in the complementary APF 9-mer duplex by recording and analyzing two-dimensional phase-sensitive NOESY data sets in H2O and D2O solution at low temperature (0 degrees C). These studies indicate that A5 inserts into the helix opposite the abasic site F14 and stacks with flanking G4.C15 and G6.C13 Watson-Crick base pairs. Base-sugar proton NOE connectivities were measured through G4-A5-G6 on the unmodified strand and between the base protons of C15 and the sugar protons of the 5'-flanking residue F14 on the modified strand. These studies establish that all glycosidic torsion angles are anti and that the helix is right-handed at and adjacent to the abasic site in the APF 9-mer duplex. Two of the 16 phosphodiester groups exhibit phosphorus resonances outside the normal spectral dispersion indicative of altered torsion angles at two of the phosphate groups in the backbone of the APF 9-mer duplex.     

Experimental and theoretical studies of the conformational perturbations induced by an abasic site

The three-dimensional structure of the natural undecamer duplex d(CGCACACACGC). d(GCGTGTGTGCG) has been determined by the combined use of NMR spectroscopy and restrained molecular dynamics (rMD) and also by molecular mechanics calculations using the JUMNA program without experimental distance constraints. Both procedures have also been used to model the abasic structure d(CGCACOCACGC).d(GCGTGTGTGCG), where 'O' indicates a modified abasic site: 3-hydroxy-2-(hydroxymethyl) tetrahydrofuran. For the natural duplex, 134 interproton distances have been obtained by complete relaxation matrix analysis of the NOESY cross-peaks intensities, using MARDIGRAS software. These distances along with 100 torsion angles for sugar ring and additional data derived from canonical A and B-DNA, have been used for structures refinement by restrained molecular dynamics. Comparison of the natural oligomer with the abasic structure obtained earlier by NMR/rMD (Y. Coppel, N. Berthet, C. Coulombeau, Ce. Coulombeau, J. Garcia and J. Lhomme, Biochemistry 36, 4817-4830, 1997) confirms that the creation of an abasic site, in this sequence context, leads to marked helix kinking. It is also shown that the JUMNA procedure is capable of reproducing the overall structural features of the natural and damaged DNA conformations without the use of experimental constraints.     

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)     

Solution structures of a duplex containing an adenine opposite a gap (absence of one nucleotide). An NMR study and molecular dynamic simulations with explicit water molecules.

We investigated the behaviour of a 15mer DNA duplex, [5'd(CAGAGTCACTGGCTC)3']. [5'd(GAGCCAG)3' + 5'd(GACTCTG)3'] which contained an adenine opposite the gap. Analysis of the NMR data showed the existence of one major species, which was in equilibrium with two minor species. Their relative concentrations varied as a function of pH with a pKa of approximately 4.5. For the major species, the duplex was globally in B conformation with the central adenine stacked in the helix. The two G.C base pairs adjacent to the central adenine were well formed and a gap was present in front of this adenine. For the minor species, major structural perturbations occurred in the centre of the duplex. At neutral pH, the central adenine was involved in a G.A mismatch with G23 adjacent to the gap. Cytosine C7 was then extrahelical and no gap was observed. Under these conditions, the major neutral species corresponded to 70% of the total and the minor species to 30%. At acidic pH, the central adenine of the minor species was protonated and was involved in a G(syn).A+(anti) mismatch. The difference is that C9 is now extrahelical and G22 is implicated in the mispair. Three-dimensional models were built to initiate molecular dynamic simulations, which were in good agreement with the NMR data. Their structural stability in terms of hydrogen bonding and their flexibility are discussed and the biological significance for the interaction with DNA polymerase is evoked.     

The structure of ColE1 rop in solution

Summary The structure of the ColE1 repressor of primer (rop) protein in solution was determined from the proton nuclear magnetic resonance data by a combined use of distance geometry and restrained molecular dynamics calculations. A set of structures was determined with low internal energy and virtually no violations of the experimental distance restraints. Rop forms homodimers: Two helical hairpins are arranged as an antiparallel four helix bundle with a left-handed rope-like twist of the helix axes and with left-handed bundle topology. The very compact packing of the side chains in the helix interfaces of the rop coiled-coil structure may well account for its high stability. Overall, the solution structure is highly similar to the recently determined X-ray structure (Banner, D.W., Kokkinidis, M. and Tsernoglou, D. (1987)J. Mol. Biol.,196, 657–675), although there are minor differences in regions where packing forces appear to influence the crystal structure.Abbreviations rop repressor of primer - NMR nuclear magnetic resonance - NOE nuclear Overhauser enhancement - NOESY NOE spectroscopy - RAN Set Structures generated from random choice of the dihedrai angles - HEL Set Structures generated from random choice of the dihedral angles restricted to ranges allowed for helices - MD molecular dynamics - EM energy minimization - RMSD root-mean-square deviation of atomic positions     

The nature of stabilization of the tandem DNA duplex pTGGAGCTG (pCAGC + (Phn-NH-(CH2)3-NH)pTCCA) based on the UV-, CD-, and two-dimensional NMR spectroscopy data

Properties and three-dimensional structure of the tandem DNA duplex pTGGAGCTG.(pCAGC+(PhnL)pTCCA) in aqueous solution, where L is an amino linker and Phn is an N-(2-hydroxyethyl)phenazinium residue, were studied spectrophotometrically and by two-dimensional 1H NMR spectroscopy (COSY and NOESY). When a tandem complex involving a Phn residue-bearing oligonucleotide is formed, the dye aromatic system intercalates into the double helix at the nick site and takes part in two stacking interactions: a strong one (3.5-4 A) with the T5-A12 base pair of its own duplex moiety and a weak one (4-5 A) with the C4-G13 pair of the adjoining duplex (mainly with the C4 base). This arrangement of the dye residue, providing a cross-interaction of the phenazinium moiety with the base pairs of the adjacent duplex structures, results in the stabilization of the whole tandem complex.     

Structural Characterization of Neurokinin-3 Receptor Selective Peptide Agonist Scyliorhinin II Bound to DPC Micelles

Abstract

Scyliorhinin II, a cyclic Tachykinin peptide, is a potent NK3 receptor agonist. The pharmacology of NK3 receptor is least characterized out of the three tachykinin receptor subtypes cloned and characterized for Tachykinins. To understand the structural basis of peptide-receptor interaction, the three-dimensional structure of the Scyliorhinin II in aqueous and micellar environments has been studied by two-dimensional proton nuclear magnetic resonance (2D ¹H-NMR spectroscopy) and distance geometry calculations. Proton NMR assignments have been carried out with the aid of correlation spectroscopy (gradient-COSY and TOCSY) and nuclear Overhauser effect spectroscopy (NOESY and ROESY) experiments. The inter proton distances and dihedral angle constraints obtained from the NMR data have been used in torsion angle dynamics algorithm for NMR applications (DYANA) to generate a family of structures, which have been refined using restrained energy minimization and dynamics. The results show that in an aqueous environment, Scyliorhinin II lacks a definite secondary structure. The structure is well-defined in presence of dodecyl phosphocholine micelles. The global fold of Scyliorhinin II bound to DPC micelles consists of a well-defined helix in the C-terminal region from residue 12–18 and a series of turns towards N-terminus. The structure is further stabilized by disulfide bond between Cys7 and Cys13. The conformational range of the peptide revealed by NMR and CD studies has been analyzed in terms of characteristic secondary features. Observed conformational features have been compared with those of Substance P, Neurokinin A and Neurokinin B, potent NK1, NK2, and NK3 agonists, respectively.     

Structural characterization of neurokinin-3 receptor selective peptide agonist scyliorhinin II bound to DPC micelles

Scyliorhinin II, a cyclic Tachykinin peptide, is a potent NK3 receptor agonist. The pharmacology of NK3 receptor is least characterized out of the three tachykinin receptor subtypes cloned and characterized for Tachykinins. To understand the structural basis of peptide-receptor interaction, the three-dimensional structure of the Scyliorhinin II in aqueous and micellar environments has been studied by two-dimensional proton nuclear magnetic resonance (2D 1H-NMR spectroscopy) and distance geometry calculations. Proton NMR assignments have been carried out with the aid of correlation spectroscopy (gradient-COSY and TOCSY) and nuclear Overhauser effect spectroscopy (NOESY and ROESY) experiments. The inter proton distances and dihedral angle constraints obtained from the NMR data have been used in torsion angle dynamics algorithm for NMR applications (DYANA) to generate a family of structures, which have been refined using restrained energy minimization and dynamics. The results show that in an aqueous environment, Scyliorhinin II lacks a definite secondary structure. The structure is well-defined in presence of dodecyl phosphocholine micelles. The global fold of Scyliorhinin II bound to DPC micelles consists of a well-defined helix in the C-terminal region from residue 12-18 and a series of turns towards N-terminus. The structure is further stabilized by disulfide bond between Cys7 and Cys13. The conformational range of the peptide revealed by NMR and CD studies has been analyzed in terms of characteristic secondary features. Observed conformational features have been compared with those of Substance P, Neurokinin A and Neurokinin B, potent NK1, NK2, and NK3 agonists, respectively.     

The solution structure of a locked nucleic acid (LNA) hybridized to DNA

LNA (Locked Nucleic Acids) is a novel oligonucleotide analogue containing a conformationally restricted nucleotide with a 2'-O, 4'-C-methylene bridge that induces unprecedented thermal affinities when mixed with complementary single stranded DNA and RNA. We have used two-dimensional 1H NMR spectroscopy obtained at 750 and 500 MHz to determine a high resolution solution structure of an LNA oligonucleotide hybridized to the complementary DNA strand. The determination of the structure was based on a complete relaxation matrix analysis of the NOESY cross peaks followed by restrained molecular dynamics calculations. Forty final structures were generated for the duplex from A-type and B-type dsDNA starting structures. The root-mean-square deviation (RMSD) of the coordinates for the forty structures of the complex was 0.32A. The structures were analysed by use of calculated helix parameters. This showed that the values for rise and buckle in the LNA duplex is markedly different from canonical B-DNA at the modification site. A value of twist similar to A-DNA is also observed at the modification site. The overall length of the helix which is 27.3 A. The average twist over the sequence are 35.9 degrees +/- 0.3 degrees. Consequently, the modification does not cause the helix to unwind. The bis-intercalation of the thiazole orange dye TOTO to the LNA duplex was also investigated by 1H NMR spectroscopy to sense the structural change from the unmodified oligonucleotide. We observed that the bis-intercalation of TOTO is much less favourable in the 5'-CT(L)AG-3' site than in the unmodified 5'-CTAG-3' site. This was related to the change in the base stacking of the LNA duplex compared to the unmodified duplex.     

Structural studies of alpha-bungarotoxin. 1. Sequence-specific 1H NMR resonance assignments

We report the complete sequence-specific assignment of the backbone resonances and most of the side-chain resonances in the 1H NMR spectrum of alpha-bungarotoxin by two-dimensional NMR. Problems with resonance overlap were resolved with the assistance of the HRNOESY experiment described in an accompanying paper [Basus, V.J., & Scheek, R.M. (1988) Biochemistry (second paper of three in this issue)]. Significant differences exist between the solution structure described here and the crystal structure of alpha-bungarotoxin, on the basis of the proton to proton distances obtained by nuclear Overhauser enhancement spectroscopy (NOESY) and the corresponding distances from the X-ray crystal structure [Love, R.A., & Stroud, R.M. (1986) Protein Eng. 1, 37]. These differences include a larger beta-sheet in solution and a different orientation of the invariant tryptophan, Trp-28, making the solution structure more consistent with the crystal structure of the homologous neurotoxin alpha-cobratoxin. Four errors in the order of the amino acids in the primary sequence were indicated by the NMR data. These errors were confirmed by chemical means, as described in an accompanying paper [Kosen, P.A., Finer-Moore, J., McCarthy, M.P., & Basus, V.J. (1988) Biochemistry (third paper of three in this issue)].     

1H NMR study of the base-pairing reactions of d(GGAATTCC): salt effects on the equilibria and kinetics of strand association

Previously, we examined the imino proton relaxation of d(GGAATTCC) in order to characterize salt and polyamine effects on the base-pair opening kinetics of this oligonucleotide [Braunlin, W. H., & Bloomfield, V. A. (1988) Biochemistry 27, 1184-1191]. Here, we report salt-dependent measurements of the NMR behavior of the nonexchangeable base proton resonances of d(GGAATTCC). From chemical shift measurements, we find an unexpectedly large salt dependence of Ka, the equilibrium constant for helix association. A total of 1.8 +/- 0.3 sodium ions are thermodynamically released upon dissociation of the octamer duplex. Most of the salt dependence of the equilibrium constant can be traced to a large salt dependence of the association rate. Thus, 1.4 +/- 0.2 sodium ions associate during the rate-limiting step of helix association. In agreement with our previous imino proton results, we also find a significant salt dependence of the duplex dissociation rate. Activation energies for helix association are very small, and possibly negative; most of the temperature dependence of the association equilibrium can be traced to a large activation energy (approximately 50 kcal/mol) for duplex dissociation.