Conformational transitions in thymidine bulge-containing deoxytridecanucleotide duplexes. Role of flanking sequence and temperature in modulating the equilibrium between looped out and stacked thymidine bulge states

Structural features at extra thymidine bulge sites in DNA duplexes have been elucidated from a two-dimensional NMR analysis of through-bond and through-space connectivities in the otherwise self-complementary d(C-C-G-T-G-A-A-T-T-C-C-G-G) (GTG 13-mer) and d(C-C-G-G-A-A-T-T-C-T-C-G-G) (CTC 13-mer) duplexes in aqueous solution. These studies establish that the extra thymidine flanked by guanosines in the GTG 13-mer duplex is in a conformational equilibrium between looped out and stacked states. The looped-out state is favored at low temperature (0 degrees C), whereas the equilibrium shifts in favor of the stacked state at elevated temperatures (35 degrees C) prior to the onset of the duplex-strand transition. By contrast, the extra thymidine flanked by cytidines in the CTC 13-mer duplex is looped out independent of temperature in the duplex state. Our results demonstrate that temperature and flanking sequence modulate the equilibrium between looped-out and stacked conformations of single base thymidine bulges in DNA oligomer duplexes.     

Conformation of adenosine bulge-containing deoxytridecanucleotide duplexes in solution. Extra adenosine stacks into duplex independent of flanking sequence and temperature

Structural features at the extra adenosine bulge sites in DNA duplexes have been elucidated from an NMR analysis of two-dimensional through space and through bond connectivities in the self-complementary d(C-C-G-G-A-A-T-T-C-A-C-G-G) (CAC 13-mer) and d(C-C-G-A-G-A-A-T-T-C-C-G-G) (GAG 13-mer) duplexes in aqueous solution. These studies establish that the extra adenosine stacks into the helix at all temperatures below the onset of the melting transition in solution, and the results are independent of whether the extra adenosine is flanked by cytidines (CAC 13-mer) or guanosines (GAG 13-mer). The NMR parameters establish that the extra adenosine can be accommodated into the helix with the flanking base pairs adopting a wedge-shaped orientation. The resulting perturbation extends out to the C10-G11 phosphodiester backbone adjacent to the bulge segment in both the CAC 13-mer and GAG 13-mer duplexes.     

Sequence-dependent conformations of DNA duplexes: the TATA segment of the d(G-G-T-A-T-A-C-C) duplex in aqueous solution

The base and sugar protons of the d(G-G-T-A-T-A-C-C) duplex have been assigned from two-dimensional correlated (COSY) and nuclear Overhauser effect (NOESY) measurements in D₂O solution at 25°C. The nucleic acid protons have been assigned from NOEs between protons on adjacent bases on the same and partner strands, as well as from NOEs between the base protons and their own and 5′-flanking H1′, H2′, H2″, H3′, and H4′ sugar protons. These assignments are confirmed from coupling constant and NOE connectivities within the sugar protons of a given residue. Several of these NOEs exhibit directionality and demonstrate that the d(G-G-T-A-T-A-C-C) duplex is a right-handed helix. The relative magnitude of the NOEs between the base protons and the sugar H2′ protons of its own and 5′-flanking sugar demonstrate that the TATA segment of the d(G-G-T-A-T-A-C-C) duplex adopts a B-DNA type helix geometry in solution, in contrast to the previous observation of a A-type helix for the same octanucleotide duplex in the crystalline state.     

Conformational transitions of poly(dA-bromo5dU) and poly(dA-iodo5dU) in solution.

Extensive circular dichroism studies have been conducted with the title polynucleotides under various solution conditions. The studies provided the following information: (i) The halogen atoms in place of thymine methyl hinder the isomerization into X-DNA. (ii) The brominated but not iodinated polynucleotide isomerizes into Z-DNA in concentrated NaCl+NiCl2. The transition takes place at lower NiCl2 concentrations than with poly(dA-dT). (iii) The iodinated polynucleotide forms an unusual conformation in aqueous solution in which it is very stable. It isomerizes from this conformer into the usual B-type double helix in concentrated ethanol solutions. The isomerization is a two-state cooperative process. (iv) Both title polynucleotides undergo still another two-state cooperative transition in trifluorethanol solutions presumably into A-DNA showing a rather unusual circular dichroism spectrum.     

Antiamoebin I in methanol solution: rapid exchange between right-handed and left-handed 3(10)-helical conformations

Antiamoebin I (Aam-I) is a membrane-active peptaibol antibiotic isolated from fungal species belonging to the genera Cephalosporium, Emericellopsis, Gliocladium, and Stilbella. Antiamoebin I has the amino acid sequence: Ac-Phe(1)-Aib-Aib-Aib-Iva-Gly-Leu-Aib(8)-Aib-Hyp-Gln-Iva-Hyp-Aib-Pro-Phl(16). By using the uniformly (13)C,(15)N-labeled sample of Aam-I, the set of conformationally dependent J couplings and (3h)J(NC) couplings through H-bonds were measured. Analysis of these data along with the data on magnetic nonequivalence of the (13)C(beta) nuclei (Deltadelta((13)C(beta))) in Aib and Iva residues allowed us to draw the univocal conclusion that the N-terminal part (Phe(1)-Gly(6)) of Aam-I in MeOH solution is in fast exchange between the right-handed and left-handed 3(10)-helical conformations, with an approximately equal population of both states. An additional conformational exchange process was found at the Aib(8) residue. The (15)N-NMR-relaxation and CD-spectroscopy measurements confirmed these findings. Molecular modeling and Monte Carlo simulations revealed that both exchange processes are correlated and coupled with significant hinge-bending motions around the Aib(8) residue. Our results explain relatively low activity of Aam-I with respect to other 15-amino acid residue peptaibols (for example, zervamicin) in functional and biological tests. The high dynamic 'propensity' possibly prevents both initial binding of the antiamoebin to the membrane and subsequent formation of stable ionic channels according to the barrel-stave mechanism.     

Conformational transitions of poly(dA-dC).poly(dG-dT) induced by high salt or in ethanolic solution.

Poly(dA-dC).poly(dG-dT) was studied by circular dichroism in the presence of high CsCl concentrations and in ethanolic solutions. This alternating purine-pyrimidine duplex may undergo two conformational transitions from a B-type to a novel structure and subsequently into an A-form. Cs+ ions or increasing ethanol concentrations induced a change of the B-type CD spectrum and an inversion of the long wavelength CD band. Lowering the temperature below 0 C or addition of small amounts of Ca++ ions were particularly potent in producing a large negative CD band. A modified B-type structure or a conversion into a left-handed Z-form is considered for this conformational transition.     

Conformational changes in serpins: I. The native and cleaved conformations of alpha(1)-antitrypsin

The serpins (SERine Proteinase INhibitors) are a family of proteins with important physiological roles, including but not limited to the inhibition of chymotrypsin-like serine proteinases. The inhibitory mechan- ism involves a large conformational change known as the S-->R (stressed-->relaxed) transition. The largest structural differences occur in a region around the scissile bond called the reactive centre loop: In the native (S) state, the reactive centre is exposed, and is free to interact with proteinases. In inhibitory serpins, in the cleaved (R) state the reactive centre loop forms an additional strand within the beta-sheet. The latent state is an uncleaved state in which the intact reactive centre loop is integrated into the A sheet as in the cleaved form, to give an alternative R state.The serpin structures illustrate detailed control of conformation within a single protein. Serpins are also an unusual family of proteins in which homologues have native states with different folding topologies. Determination of the structures of inhibitory serpins in multiple conformational states permits a detailed analysis of the mechanism of the S-->R transition, and of the way in which a single sequence can form two stabilised states of different topology.Here we compare the conformations of alpha(1)-antitrypsin in native and cleaved states. Many protein conformational changes involve relative motions of large rigid subunits. We determine the rigid subunits of alpha(1)-antitrypsin and analyse the changes in their relative position and orientation. Knowing that the conformational change is initiated by cleavage at the reactive centre, we describe a mechanism of the S-->R transition as a logical sequence of mechanical effects, even though the transition likely proceeds in a concerted manner.     

Conformational changes in serpins: I. The native and cleaved conformations of alpha(1)-antitrypsin

The serpins (SERine Proteinase INhibitors) are a family of proteins with important physiological roles, including but not limited to the inhibition of chymotrypsin-like serine proteinases. The inhibitory mechan- ism involves a large conformational change known as the S-->R (stressed-->relaxed) transition. The largest structural differences occur in a region around the scissile bond called the reactive centre loop: In the native (S) state, the reactive centre is exposed, and is free to interact with proteinases. In inhibitory serpins, in the cleaved (R) state the reactive centre loop forms an additional strand within the beta-sheet. The latent state is an uncleaved state in which the intact reactive centre loop is integrated into the A sheet as in the cleaved form, to give an alternative R state.The serpin structures illustrate detailed control of conformation within a single protein. Serpins are also an unusual family of proteins in which homologues have native states with different folding topologies. Determination of the structures of inhibitory serpins in multiple conformational states permits a detailed analysis of the mechanism of the S-->R transition, and of the way in which a single sequence can form two stabilised states of different topology.Here we compare the conformations of alpha(1)-antitrypsin in native and cleaved states. Many protein conformational changes involve relative motions of large rigid subunits. We determine the rigid subunits of alpha(1)-antitrypsin and analyse the changes in their relative position and orientation. Knowing that the conformational change is initiated by cleavage at the reactive centre, we describe a mechanism of the S-->R transition as a logical sequence of mechanical effects, even though the transition likely proceeds in a concerted manner.     

Conformation, dynamics, and structural transitions of the TATA box region of self-complementary d[(C-G)n-T-A-T-A-(C-G)n] duplexes in solution

Structural and kinetic features of the TATA box located in the center of the alternating self-complementary d(C-G-C-G-T-A-T-A-C-G-C-G) duplex (TATA 12-mer) and d(C-G-C-G-C-G-T-A-T-A-C-G-C-G-C-G) duplex (TATA 16-mer) have been probed by high-resolution proton and phosphorus NMR spectroscopy in aqueous solution. The imino exchangeable Watson-Crick protons and the nonexchangeable base protons in the TATA box of the TATA 12-mer and TATA 16-mer duplexes have been assigned from intra and inter base pair nuclear Overhauser effect (NOE) measurements. Imino proton line-width and hydrogen exchange saturation recovery measurements demonstrate that the dA X dT base pairs in the TATA box located in the center of the TATA 12-mer and TATA 16-mer duplexes are kinetically more labile than flanking dG X dC base pairs. The proton and phosphorus NMR parameters of the TATA 12-mer monitor a cooperative premelting transition in the TATA box prior to the onset of the melting transition to unstacked strands. Phosphorus NMR studies have been unable to detect any indication of a right-handed B DNA to a left-handed Z DNA transition for the TATA 12-mer duplex in saturated NaCl solution. By contrast, we do detect the onset of the B to Z transition for the TATA 16-mer in saturated NaCl solution. Proton and phosphorus NMR studies demonstrate formation of a loop conformation with chain reversal at the TATA segment for the TATA 12-mer and TATA 16-mer duplexes on lowering the DNA and counterion concentration. The imino protons (10-11 ppm) and phosphorus resonances (3.5-4.0 ppm; 4.5-5.0 ppm) of the loop segment fall in spectral windows well resolved from the corresponding markers in fully paired segments so tha it should be possible to identify loops in longer DNA helixes. The equilibrium between the loop and fully paired duplex conformations of the TATA 12-mer and TATA 16-mer is shifted toward the latter on addition of moderate salt.     

Conformational transitions in the nootropic peptide semax (MEHFPGP) and its N-terminal modifications

We use molecular dynamics simulation to examine the conformational possibilities in solution for the peptide MEHFPGP (Semax) representing the minimal nootropic fragment of MSH, and its versions with N-terminal substitutions of K, G, or R for M. We discuss the possible relationship between molecule structure and physiological activity, considering the influence of Coulomb interactions on the dynamics and the putative stabilization of a certain peptide conformation at pH < 6.     

Conformational transitions and hydration of poly d (A-T) · poly d (A-T) in fibers

Conformational transitions of poly d(A-T) · poly d (A-T) have been studied by fiber X-ray diffraction and measurement of fiber dimensions. Results obtained for the D-A-B and D-B transitions are presented and analyzed. For all these form transitions, cooperativity effects are observed for the variation of the rise per nucleotide versus the relative humidity. Detailed information about hydration of the polynucleotide during form transitions and the numbers of water molecules per nucleotide necessary to stabilize the different helical conformations are presented. Offprint requests to: S. Premilat     

Conformational transitions and specific heat anomaly in poly(dG-dC) and its methylated analogue.

The Zimm and Bragg theory of the helix<-->coil transition has been modified to explain order<-->order transitions in polynucleotides, in particular B<-->Z<-->psi(-)<-->coil transitions in poly(dG-dC) and poly(dG-me5dC). Lambda anomalies in specific heat measurements around the transition point have also been explained by a further modification of the same theory. Theoretical results are found to be in good agreement with the experimental data. The nucleation parameter is consistent with the stabilization/destabilization of the ordered states (Z helix) under various environmental conditions, e.g. methylation of cytosine residue at C5 position or change in the cationic concentration of the solvent.     

X-ray solution scattering (SAXS) combined with crystallography and computation: defining accurate macromolecular structures, conformations and assemblies in solution

Crystallography supplies unparalleled detail on structural information critical for mechanistic analyses; however, it is restricted to describing low energy conformations of macromolecules within crystal lattices. Small angle X-ray scattering (SAXS) offers complementary information about macromolecular folding, unfolding, aggregation, extended conformations, flexibly linked domains, shape, conformation, and assembly state in solution, albeit at the lower resolution range of about 50 A to 10 A resolution, but without the size limitations inherent in NMR and electron microscopy studies. Together these techniques can allow multi-scale modeling to create complete and accurate images of macromolecules for modeling allosteric mechanisms, supramolecular complexes, and dynamic molecular machines acting in diverse processes ranging from eukaryotic DNA replication, recombination and repair to microbial membrane secretion and assembly systems. This review addresses both theoretical and practical concepts, concerns and considerations for using these techniques in conjunction with computational methods to productively combine solution scattering data with high-resolution structures. Detailed aspects of SAXS experimental results are considered with a focus on data interpretation tools suitable to model protein and nucleic acid macromolecular structures, including membrane protein, RNA, DNA, and protein-nucleic acid complexes. The methods discussed provide the basis to examine molecular interactions in solution and to study macromolecular flexibility and conformational changes that have become increasingly relevant for accurate understanding, simulation, and prediction of mechanisms in structural cell biology and nanotechnology.     

Determination of sugar conformations by NMR in larger DNA duplexes using both dipolar and scalar data: Application to d(CATGTGACGTCACATG)2

Summary Different methods for determining sugar conformations in large oligonucleotides have been evaluated using both J-coupling and NOE data. In order to simulate COSY spectra, reliable estimates of line widths are required. We have measured T_1p (=T₂) values for a large number of protons of the hexadecamer d(CATGTGACGTCACATG)₂ using a new two-dimensional NMR experiment (T1RHOSY) to provide baseline information for the simulations. Both DQF-COSY and P.E.COSY cross-peaks have been systematically simulated as a function of line width, digitisation and signal-to-noise ratio. We find that for longer correlation times (5 ns), where line widths are comparable to or larger than active couplings, only {ie190-1} is reasonably accurately determined (within ±1 Hz). Under these conditions, additional information is needed to determine the sugar conformation. We have used apparent distances H1-2-H4 and H2-H4, which provide a range of P_s over an interval of ca. 20°. Complete analysis of time courses for intraresidue NOEs, with and without coupling constants, has also been evaluated for determining nucleotide conformations. Whereas P_s is poorly determined in the absence of both intrasugar NOEs and coupling constants, the range of solutions is decreased when intrasugar NOEs and {ie190-2} are also available. DQF-COSY, P.E.COSY and NOESY spectra at different mixing times of the hexadecamer d(CATGTGACGTCACATG)₂ were recorded at three temperatures. A detailed analysis of the NOEs and coupling constants provided estimates of the sugar conformations in the hexadecamer. At 50 °C, the sugar conformations are well determined by the scalar and dipolar data, with pseudorotation phase angles of 126–162° and mole fractions of the S conformation (f_s) of 0.86±0.05. There was no statistically significant difference between f_s for the purines and the pyrimidines, although there was a small tendency for P_s of the purines to be larger than those of the pyrimidines. At 25 °C, the sugar conformations were much less well determined, although the estimates of f_s were the same within experimental error as at 50 °C. The experimental and theoretical results provide guidelines for the limits of conformational analysis of nucleic acids based on homonuclear NMR methods.     

NMR studies of an exocyclic 1,N2-propanodeoxyguanosine adduct (X) located opposite deoxyadenosine (A) in DNA duplexes at basic pH: simultaneous partial intercalation of X and A between stacked bases

The NMR parameters for the 1,N2-propanodeoxyguanosine (X) opposite deoxyadenosine positioned in the center of the complementary d(C1-A2-T3-G4-X5-G6-T7-A8-C9).d(G10-T11-A12-C13-A14-C15-A 16-T17-G18) X.A 9-mer duplex are pH dependent. A previous paper established protonated X5(syn).A14(anti) pairing in the X.A 9-mer duplex at pH 5.8 [Kouchakdjian, M., Marinelli, E., Gao, X., Johnson, F., Grollman, A., & Patel, D. J. (1989) Biochemistry 28, 5647-5657]; this paper focuses on the pairing alignment at the lesion site at pH 8.9. The observed NOEs between specific exocyclic CH2 protons and both the imino proton of G6 and the sugar H1' protons of C13 and A14 establish that X5 is positioned toward the G6.C13 base pair with the exocyclic ring directed between C13 and A14 on the partner strand. The observed NOE between the H2 proton of A14 and the imino proton of G4, but not G6, establishes that A14 at the lesion site is directed toward the G4.C15 base pair. NOEs are detected between all exocyclic CH2 protons of X5 and the H2 proton of A14, confirming that both X5 and A14 are directed toward the interior of the helix. The X5(anti).A14(anti) alignment at pH 8.9 is accommodated within the helix with retention of Watson-Crick pairing at flanking G4.C15 and G6.C13 base pairs. The energy-minimized conformation of the (G4-X5-G6).(C13-A14-C15) segment at pH 8.9 establishes that X5 and A14 are directed into the helix, partially stack on each other, and are not stabilized by intermolecular hydrogen bonds. The X5 base is partially intercalated between C13 and A14 on the unmodified strand, while A14 is partially intercalated between G4 and X5 on the modified strand. This results in a larger separation between the G4.C15 and G6.C13 base pairs flanking the lesion site in the basic pH conformation of the X.A 9-mer duplex. The midpoint of the transition between the protonated X5(syn).A14(anti) and X5(anti).A14(anti) conformations occurs at pH 7.6, establishing an unusually high pKa for protonation of the A14 ring opposite the X5 exocyclic adduct site. Thus, the interplay between hydrophobic and hydrogen-bonding contributions modulated by pH defines the alignment of 1,N2-propanodeoxyguanosine opposite deoxyadenosine in the interior of DNA helices.     

Conformational isomerizations of the poly(dA-dT) and poly(amino2dA-dT) duplexes involving the unusual X-DNA double helix: a fourth derivative spectrophotometric study

Fourth derivative spectrophotometry has been applied to monitor conformational isomerizations of polynucleotides for the first time. The transitions studied have been the B-A and A-X isomerizations of poly(dA-dT) and the B-X one of poly(amino2dA-dT). Parameters obtained from the fourth derivative spectra have been used to follow these conformational changes. The A form of poly(dA-dT) has been characterized by a new fourth derivative peak at 293.0 nm which can be associated to interstrand adenine-adenine interactions. Furthermore, some of the fourth derivative peaks in the long wavelength region (270-310 nm) can be related to stacking interactions present in the polynucleotide double helices. The tentative assignment of these peaks, particularly that at 299.0 nm in the derivative spectra of poly(amino2dA-dT), to n----pi electronic transitions is discussed.     

Protein conformations explored by difference high-angle solution X-ray scattering: oxidation state and temperature dependent changes in cytochrome C

We demonstrate the use of high-angle X-ray scattering to explore protein conformational states in solution by resolving oxidation state- and temperature-dependent changes in the conformation of horse heart cytochrome c. Several detailed models exist for oxidation-dependent changes in mitochondrial class I c cytochromes determined by X-ray crystallography and solution NMR techniques. These models differ in the magnitude and locations of structural change. Our scattering measurements show that high-angle X-ray scattering can discriminate between these models, and that the experimental scattering data for horse cytochrome c can be best reconciled with selected NMR models for the same protein. These results demonstrate the ability to use high-angle X-ray scattering to resolve conformational states of proteins in solution, and to relate these measurements to detailed structural models. Furthermore, temperature-dependent changes are found in the high angle scattering patterns for horse cytochrome c, illustrating the sensitivity of these measurements to dynamic aspects of protein structure. These results demonstrate the ability to use difference high angle scattering as a quantitative monitor of reaction-linked changes in protein conformation and structural dynamics. Synchrotron-based high-angle scattering holds promise as a widely applicable, high throughput technique for exploring conformational states linked to physiological protein function, for resolving configurational differences between protein structures in solution and crystalline states, and for bridging the gap between solution NMR and crystallographic structure techniques.     

Conformational studies of the copolymer poly(L-lysine,L-tyrosine) 1:1 in aqueous solution

The absorption and circular dichroism spectra of the 1:1 copolymer (L -Lys, L -Tyr)_n have been investigated in aqueous solutions at pH ranging from 3 to 13. The spectral patterns indicate that the fully charged polympholyte assumes a nonperiodic conformation on the acid and basic sides of the isoelectric point. At pH ranging from 9.2 to 11.6, the polymer is largely ordered and takes mostly an antiparallel β-structure as is shown by the infrared spectra in D₂O solutions. Moreover, the rotational strength of the L_a transition of tyrosyl is independent of the polymer conformation, whereas that of the L_b transition is strongly sensitive to it.     

Conformational transitions and aggregation in poly(dA)-poly(dT) system induced by Na+ and Mg2+ ions

Effects of Mg²⁺ ions on thermally induced conformational transitions in the synthetic poly(dA)·poly(dT) and poly(dA)·2poly(dT) were studied in the buffered solutions (pH 6.9), containing 0.1 or 1 M NaCl at polynucleotide concentration of 0.1–0.3 mM (in nucleic bases). The experiments consist of measurements of the UV absorption and intensity of conventional visible static light scattering. The diagram of conformational transitions in the poly(dA)–poly(dT)–Mg²⁺ system was constructed on a basis of experimental data obtained. Anomalously strong light scattering, like critical opalescence, has been revealed at 0.1 M NaCl and [Mg²⁺]≥20 mM in the melting range of both polynucleotides, which eventually disappeared after the completion of polymer strands separation. The effect presumably is caused by a fluctuation process of polymer strands complexing which arises at a certain concentration of Mg²⁺ ions.     

Internal mobility of the ologonucleotide duplexes d(TCGCG)2 and d(CGCGCG)2 in aqueous solution from molecular dynamics simulations

Summary In this paper we present longitudinal relaxation times, order parameters and effective correlation times for the base and sugar carbons in both strands of the oligonucleotide duplexes d(TCGCG)₂ and d(CGCGCG)₂, as calculated from 400 ps molecular dynamics trajectories in aqueous solution. The model-free approach (Lipari and Szabo, 1982) was used to determine the amplitudes and time scales of the internal motion. Comparisons were made with NMR relaxation measurements (Borer et al., 1994). The order parameters could acceptably be reproduced, and the effective correlation times were found to be lower than the experimental estimates. Reasonable T₁ relaxation times were obtained in comparison with experiment for the nonterminal nucleosides. The T₁ relaxation times were found to depend mainly on the order parameters and overall rotational correlation time.Abbreviations MD molecular dynamics - CSA chemical shift anisotropy To whom correspondence should be addressed.