The crystal structure of d(CCCCGGGG): a new A-form variant with an extended backbone conformation

The crystal structure of d(CCCCGGGG) has been determined at a resolution of 2.25 A. The oligomers crystallize as A-DNA duplexes occupying crystallographic two-fold axes. The backbone conformation is, in general, similar to that observed in previously reported crystal structures of A-DNA fragments, except for the central linkage, where it adopts an extended structure resulting from all trans conformation at the P-O5'-C5'-C4' bonds. This type of conformation facilitates interstrand stacking between the guanines at the C-G site. The local helix twist at this step is very small (25 degrees) compared to an overall average of 33.5 degrees. The unique structure of the C-G base-pair step, namely the extended backbone and the distinct stacking geometry, may be an important feature in the recognition mechanism between double-stranded DNA molecules and restriction endonucleases such as Msp I, which cuts the sequence CCGG very specifically with a rate unaffected by neighboring base pairs.     

The Crystal Structure of d(CCCCGGGG): A New A-Form Variant with an Extended Backbone Conformation

Abstract

The crystal structure of d(CCCCGGGG) has been determined at a resolution of 2.25Å. The oligomers crystallize as A-DNA duplexes occupying crystallographic two-fold axes. The backbone conformation is, in general, similar to that observed in previously reported crystal structures of A-DNA fragments, except for the central linkage, where it adopts an extended structure resulting from all trans conformation at the P-05′-C5′-C4′ bonds. This type of conformation facilitates interstrand stacking between the guanines at the C-G site. The local helix twist at this step is very small (25°) compared to an overall average of 33.5°. The unique structure of the C-G base-pair step, namely the extended backbone and the distinct stacking geometry, may be an important feature in the recognition mechanism between double- stranded DNA molecules and restriction endonucleases such as Msp I, which cuts the sequence CCGG very specifically with a rate unaffected by neighboring base pairs.     

Thermodynamics of unpaired terminal nucleotides on short RNA helixes correlates with stacking at helix termini in larger RNAs.

Free energies for stacking of unpaired nucleotides (dangling ends) at the termini of oligoribonucleotide Watson-Crick helixes (DeltaG(0)37,stack) depend on sequence for 3' ends but are always small for 5' ends. Here, these free energies are correlated with stacking at helix termini in a database of 34 RNA structures determined by X-ray crystallography and NMR spectroscopy. Stacking involving GA pairs is considered separately. A base is categorized as stacked by its distance from (相似文献   

Inosine.adenine base pairs in a B-DNA duplex.

The structure of the synthetic deoxydodecamer d(C-G-C-I-A-A-T-T-A-G-C-G) has been determined by single crystal X-ray diffraction techniques at 2.5A resolution. The refinement converged with a crystallographic residual, R = 0.19 and the location of 64 solvent molecules. The sequence crystallises as a B-DNA helix with 10 Watson-Crick base-pairs (4 A.T. and 6 G.C) and 2 inosine.adenine (I.A) pairs. The present work shows that in the purine.purine base-pairs the adenine adopts syn orientation with respect to the furanose moiety while the inosine is in the trans (anti) orientation. Two hydrogen bonds link the I.A. base-pair, one between N-1(I) and N-7(A), the other between O-6(I) and N-6(A). This bulky purine.purine base-pair is incorporated in the double helix at two positions with little distortion of either local or global conformation. The pairing observed in this study is presented as a model for I.A base-pairs in RNA codon-anticodon interactions and may help explain the thermodynamic stability of inosine containing base-pairs. Conformational parameters and base stacking interactions are presented and where appropriate compared with those of the native compound, d(C-G-C-G-A-A-T-T-C-G-C-G) and with other studies of oligonucleotides containing purine.purine base-pairs.     

Structural features and hydration of a dodecamer duplex containing two C.A mispairs.

X-ray diffraction techniques have been used to characterise the crystal and molecular structure of the deoxyoligomer d(C-G-C-A-A-A-T-T-C-G-C-G) at 2.5A resolution. The final R factor is 0.19 with the location of 78 solvent molecules. The oligomer crystallises in a B-DNA type conformation with two strands coiled about each other to produce a duplex. This double helix consists of four A.T and six G.C Watson-Crick base pairs and two C.A mispairs. The mismatched base pairs adopt a "wobble" type structure with the cytosine displaced laterally into the major groove, the adenine into the minor groove. We have proposed that the two close contacts observed in the C.A pairing represent two hydrogen bonds one of which results from protonation of adenine. The mispairs are accommodated in the double helix with small adjustments in the conformation of the sugar-phosphate backbone. Details of the backbone conformation, base stacking interactions, thermal parameters and the hydration are now presented and compared with those of the native oligomer d(C-G-C-G-A-A-T-T-C-G-C-G) and with variations of this sequence containing G.T and G.A mispairs.     

The crystal structure of d(GTACGTAC) at 2.25 A resolution: are the A-DNA's always unwound approximately 10 degrees at the C-G steps?

The structure of the self-complementary octamer d(GTACGTAC) has been analyzed by a single crystal X-ray diffraction method at 2.25 A resolution. The crystallographic R factor was 0.184 for all 1233 reflections at this resolution. In spite of the alternating purine-pyrimidine sequence, d(GTACGTAC) adopts the A-form conformation rather than the left-handed Z-form. The average helix twist and the mean rise per base pair are 32.1 degrees and 3.18 A, respectively. The d(GTACGTAC) helix is characterized by a wide open major groove and small base-pair tilt (9.7 degrees). The partial unwinding of the helix is observed only at the central pyrimidine-purine C-G step, but not at the other pyrimidine-purine T-A steps. Based on this study and six other X-ray studies, we propose a hypothesis that the A-DNA's are always unwound approximately 10 degrees at the C-G steps. Significant differences in base-pair stacking modes are seen between the purine-pyrimidine step and the pyrimidine-purine step. All deoxyribose rings adopt the C3'-endo conformation. All backbone torsion angles fall into the range expected for the A-DNA form, except for the nucleotide G5, whose alpha and gamma torsion angles adopt the trans, trans conformation instead of the common gauche-, gauche+ conformation.     

The influence of helix morphology on co-operative polyamide backbone conformational flexibility in peptide nucleic acid complexes.

A systematic analysis of peptide nucleic acid (PNA) complexes deposited in the Protein Data Bank has been carried out using a set of contiguous atom torsion angle definitions. The analysis is complemented by molecular mechanics adiabatic potential energy calculations on hybrid PNA-nucleic acid model systems. Hitherto unobserved correlations in the values of the (alpha and epsilon) dihedral angles flanking the backbone secondary amide bond are found. This dihedral coupling forms the basis of a PNA backbone conformation classification scheme. Six conformations are thus characterised in experimental structures. Helix morphology is found to exert a significant influence on backbone conformation and flexibility: Watson-Crick PNA strands in complexes with DNA and RNA, that possess A-like base-pair stacking, adopt backbone conformations distinct from those in PNA.DNA-PNA triplex and PNA-PNA duplex P-helix forms. Solvation effects on Watson-Crick PNA backbone conformation in heterotriplexes are discussed and the possible involvement of inter-conformational transitions and dihedral angle uncoupling in asymmetric heteroduplex base-pair breathing is suggested.     

Solution structure of a DNA double helix incorporating four consecutive non-Watson-Crick base-pairs

A series of DNA 21-mers containing a variety of the 4 x 4 internal loop sequence 5'-CAAG-3'/3'-ACGT-5' were studied using nuclear magnetic resonance (NMR) methodology and distance geometry (DG)/molecular dynamics (MD) approaches. Such oligomers exhibit excellent resolution in the NMR spectra and reveal many unusual NOEs (nuclear Overhauser effect) that allow for the detailed characterization of a DNA hairpin incorporating a track of four different non-Watson-Crick base-pairs in the stem. These include a wobble C.A base-pair, a sheared A.C base-pair, a sheared A.G base-pair, and a wobble G.T base-pair. Significantly different twisting angles were observed between the base-pairs in internal loop that results with excellent intra-strand and inter-strand base stacking within the four consecutive mismatches and the surrounding canonical base-pairs. This explains why it melts at 52 degrees C even though five out of ten base-pairs in the stem adopt non-Watson-Crick pairs. However, the 4 x 4 internal loop still fits into a B-DNA double helix very well without significant change in the backbone torsion angles; only zeta torsion angles between the tandem sheared base-pairs are changed to a great extent from the gauche(-) domain to the trans domain to accommodate the cross-strand base stacking in the internal loop. The observation that several consecutive non-canonical base-pairs can stably co-exist with Watson-Crick base-pairs greatly increases the limited repertoire of irregular DNA folds and reveals the possibility for unusual structural formation in the functionally important genomic regions that have potential to become single-stranded.     

Evolution of the primate beta-globin gene region. High rate of variation in CpG dinucleotides and in short repeated sequences between man and chimpanzee

A 5500 base-pair fragment including the beta-globin gene downstream from codon 122 and about 4000 base-pairs of its 5' flanking sequence was cloned from chimpanzee DNA and thoroughly sequenced before being compared with the corresponding human sequence: 88 point differences (83 substitutions and 5 deletions or insertions of 1 base-pair) were detected as well as seven more important deletion/insertion events. These changes occur preferentially in two kinds of structure. First, 40% of the CpG dinucleotides present in either human or chimpanzee sequences are affected by nucleotide variations. This corresponds to a divergence level considerably higher than that expected. Second, most short repeated sequences found in the 5' extragenic sequence are involved in mutational events (amplification or contraction of the number of basic motifs as well as point substitutions or deletions/insertions of 1 base-pair). Considering the very low level of nucleotide sequence divergence between these two closely related species, our data provide direct evidence for CpG and tandem array instability.     

The energetics of small internal loops in RNA

The energetics of small internal loops are important for prediction of RNA secondary and tertiary structure, selection of drug target sites, and understanding RNA structure-function relationships. Hydrogen bonding, base stacking, electrostatic interactions, backbone distortion, and base-pair size compatibility all contribute to the energetics of small internal loops. Thus, the sequence dependence of these energetics are idiosyncratic. Current approximations for predicting the free energies of internal loops consider size, asymmetry, closing base pairs, and the potential to form GA, GG, or UU pairs. The database of known three-dimensional structures allows for comparison with the models used for predicting stability from sequence.     

Molecular dynamics simulations of B-DNA: An analysis of the role of initial molecular configuration,randomly assigned velocity distribution,long integration times,and nonconstrained termini

Molecular dynamics simulations of three DNA sequences using the AMBER 3.0 force field were performed with implicit inclusion of water through a distance-dependent dielectric constant and solvated counterions. Simulations of the self-complementary DNA dodecamer d(CGCGAATTCGCG) were started from a regular B-DNA structure and the x-ray single crystal B-DNA structure. Although mean convergence during the 89-ps calculation was confirmed, localized differences in backbone torsionals and base-pair helicoidals were observed. A nanosecond simulation of the nonself-complementary 14 base-pair DNA d(GGCGGAATTGGCGG) indicates that most structural parameters stabilize within the first 100–200 ps, while isolated features show low-frequency oscillations throughout the calculation. The lack of harmonic constraints on the ends of the molecules was shown not to perturb the structural dynamics of the internal oligonucleotide beyond the external 2 base pairs. Comparison of three simulations of the nonself-complementary 14 base-pair DNA d(GGCGAAATTCGCGG), identical in all respects other than the assignment of initial Maxwellian atomic velocity distributions, revealed the inherent systematic variability. The three calculations result in nearly superimposable global structures, with localized variations in torsionals and helicoidals. Our results provide a basis for performing a comparative analysis of the effect of DNA sequence on localized structure. © 1993 John Wiley & Sons, Inc.     

Structural features and hydration of d(C-G-C-G-A-A-T-T-A-G-C-G); a double helix containing two G.A mispairs

Single crystal X-ray diffraction techniques have been used to characterise the molecular structure of the title compound to 2.5A resolution. The structure consists of ten standard Watson-Crick base pairs and two G.A mismatched base pairs. The purine-purine mismatches have guanine in the usual anti orientation with respect to the sugar and adenine in syn orientation. There are two hydrogen bonds formed between the mismatch bases, N-1 and O-6 of guanine with N-7 and N-6 of adenine respectively. The bulky purine-purine mismatches are accommodated with minor perturbation of the sugar-phosphate backbone. There is a slight improvement in base pair overlap at the mismatch sites. Details of the backbone conformation, base stacking interactions and hydration are presented and compared with those of the parent compound d(C-G-C-G-A-A-T-T-C-G-C-G).     

A proposal for a specific double-helical structure in which the polynucleotide strands intercalate instead of forming base-pairs

Double helices, since the discovery of the DNA structure by Watson and Crick, represent the single most important secondary structural form of nucleic acids. The secondary structures of a variety of polynucleotide helices have now been well characterised with hydrogen-bonded base-pairs as building blocks. We wish to propose here the possibility, in a specific case, of a double stranded helical structure without any base-pair, but having a repeat unit of two nucleotides with their bases stacked through intercalation. The proposal comes from the initial models we have built for poly(dC) using the stacking patterns found in the crystal structures of 5'-dCMPNa2 which crystallises in two forms depending on the degree of hydration. These structures have pairs of nucleotides with the cytosine rings partially overlapping and separated by 3.3A. Using these as repeat units one could generate a model for poly(dC) with parallel strands, having a turn angle of 30 degrees and a base separation of 6.6A along each strand. Both right and left handed models with these parameters can be built in a smooth fashion without any obviously unreasonable stereochemical contacts. The helix diameter is about 13.5A, much smaller than that of normal helices with base-pair repeats. The changes in the sugar-phosphate backbone conformation in the present models compared to normal duplexes only reflect the torsional flexibility available for extension of polynucleotide chains as manifested by the crystal structures of drug-inserted oligonucleotide complexes. Intercalation proposed here could have some structural relevance elsewhere, for instance to the base-mismatched regions on the double helix and the packing of noncomplementary single strands as found in the filamentous bacteriophage Pf1.     

Evidence for "unseen" transposase--DNA contacts

In this study, evidence of novel, important interactions between a hyperactive Tn5 transposon recognition end sequence and hyperactive Tn5 transposase (Tnp) are presented. A hyperactive Tn5 end sequence, the mosaic end (ME), was isolated previously. The ME and a wild-type end sequence, the outside end (OE), differ at only three positions, yet transposition on the ME is tenfold higher than on the OE in vivo. Also, transposition on the ME is much more efficient than transposition on the OE in vitro. Here, we show that the decreased activity observed for the OE is caused by a defect in paired ends complex (PEC) formation resulting from the orientation of the A-T base-pair at position 4 of this end. Efficient PEC formation requires an interaction between the C5-methyl group (C5-Me) on the non-transferred strand thymine base at position 4 (T4) and Tnp. PEC formation on nicked substrates is much less affected by the orientation of the A-T base-pair at position 4, indicating that the C5-Me group is important only for steps preceding nicking. A recently determined co-crystal structure of Tn5 Tnp with the ME is discussed and a model explaining possible roles for the base-pair at position 4 is explored.     

Crystallographic study of one turn of G/C-rich B-DNA

The DNA decamer d(CCAGGCCTGG) has been studied by X-ray crystallography. At a nominal resolution of 1.6 A, the structure was refined to R = 16.9% using stereochemical restraints. The oligodeoxyribonucleotide forms a straight B-DNA double helix with crystallographic dyad symmetry and ten base-pairs per turn. In the crystal lattice, DNA fragments stack end-to-end along the c-axis to form continuous double helices. The overall helical structure and, notably, the groove dimensions of the decamer are more similar to standard, fiber diffraction-determined B-DNA than A-tract DNA. A unique stacking geometry is observed at the CA/TG base-pair step, where an increased rotation about the helix axis and a sliding motion of the base-pairs along their long axes leads to a superposition of the base rings with neighboring carbonyl and amino functions. Three-center (bifurcated) hydrogen bonds are possible at the CC/GG base-pair steps of the decamer. In their common sequence elements, d(CCAGGCCTGG) and the related G.A mismatch decamer d(CCAAGATTGG) show very similar three-dimensional structures, except that d(CCAGGCCTGG) appears to have a less regularly hydrated minor groove. The paucity of minor groove hydration in the center of the decamer may be a general feature of G/C-rich DNA and explain its relative instability in the B-form of DNA.     

Structure of a eukaryotic decoding region A-site RNA

The aminoglycoside antibiotics target a region of highly conserved nucleotides in the aminoacyl-tRNA site (A site) of 16 S RNA on the 30 S subunit. The structures of a prokaryotic decoding region A-site oligonucleotide free in solution and bound to the aminoglycosides paromomycin and gentamicin C1A have been determined. Here, the structure of a eukaryotic decoding region A-site oligonucleotide has been determined using homonuclear and heteronuclear NMR spectroscopy, and compared to the unbound prokaryotic rRNA structure. The two structures are similar, with a U1406-U1495 base-pair, a C1407-G1494 Watson-Crick base-pair, and a G1408-A1493 base-pair instead of the A1408-A1493 base-pair of the prokaryotic structure. The two structures differ in the orientation of the 1408 position with respect to A1493; G1408 is rotated toward the major groove, which is the binding pocket for aminoglycosides. The structures also differ in the stacking geometry of G1494 on A1493, which could have slight long-range conformational effects.     

Structural Features and Hydration of d(C-G-C-G-A-A-T-T-A-G-C-G); a Double Helix Containing Two G.A Mispairs

Abstract

Single crystal X-ray diffraction techniques have been used to characterise the molecular structure of the title compound to 2.5Å resolution. The structure consists of ten standard Watson-Crick base pairs and two G.A mismatched base pairs. The purine-purine mismatches have guanine in the usual anti orientation with respect to the sugar and adenine in syn orientation. There are two hydrogen bonds formed between the mismatch bases, N-l and 0–6 of guanine with N-7 and N-6 of adenine respectively. The bulky purine-purine mismatches are accommodated with minor perturbation of the sugar-phosphate backbone. There is a slight improvement in base pair overlap at the mismatch sites. Details of the backbone conformation, base stacking interactions and hydration are presented and compared with those of the parent compound d(C-G-C-G-A-A-T-T-C-G-C-G).     

The conformational effect of para-substituted C8-arylguanine adducts on the B/Z-DNA equilibrium

The B form of DNA exists in equilibrium with the Z form and is mainly affected by sequence, electrostatic interactions, and steric effects. C8-purine substitution shifts the equilibrium toward the Z form though how this interaction overcomes the unfavorable electrostatic interactions and decrease in stacking in the Z form has not been determined. Here, a series of C8-arylguanine derivatives, bearing a para-substituent were prepared and the B/Z equilibrium determined. B/Z ratios were measured by CD and conformational effects of the aryl substitution determined by NMR spectroscopy and molecular modeling. The para-substituent was found to have a significant effect on the B/Z DNA equilibrium caused by altering base-pair stacking of the B form and modifying the hydration/ion shell of the B form. A unique melting temperature versus salt concentration was observed and provides evidence relevant to the mechanism of B/Z conformational interconversion.