Molecular structure of r(GCG)d(TATACGC): a DNA--RNA hybrid helix joined to double helical DNA

High resolution structure of the RNA duplex [U(U-A)6A]2

RNA is involved in many biological functions, ranging from information storage and transfer to the catalysis of reactions involving both nucleic acids and proteins. Previous crystallographic studies on RNA oligomeric chains provide only averaged structures or information limited in resolution. The oligomer [U(U-A)6A]2 was chosen for the study of protein-RNA interactions in viruses. Its size and base composition mimic portions of the genomic RNA in alfalfa mosaic virus that bind to the amino terminus of the viral subunit. The actual sequence was designed to guarantee the formation of a single species of duplex and to facilitate the production of the pure oligomer in large quantities. The molecular structure, derived from the 2.25 A resolution X-ray diffraction data, allows the most detailed analysis of an A-RNA helix reported to date. Two kinks are observed that divide the duplex into three blocks, each close to a canonical A-helical conformation. A few intermolecular hydrogen bonds involving 2'-hydroxyl groups stabilize this peculiar conformation of the RNA, which may be related to the temperature used for the crystallization (35 degrees C). The structure demonstrates both the plasticity of the RNA molecule and the role of the 2'-hydroxyl groups in intermolecular interactions.

Three-dimensional structure of d(GGGATCCC) in the crystalline state

The structure of the self-complementary octamer d(GGGATCCC) has been analysed by single crystal X-ray diffraction methods at a nominal resolution of 2.5 A. With acceptable stereochemistry of the model the crystallographic R factor was 16.6% after restrained least-squares refinement. In the crystal, d(GGGATCCC) forms an A-DNA double helix with slightly varying conformation of the two strands. The average displacement of the base pairs from the helix axis is unusually large and is accompanied by pronounced sliding of the base pairs along their long axes at all dinucleotide steps except for the central AT. With 12 base pairs per complete turn the helix is considerably underwound. As observed with most oligodeoxyribonucleotides analysed by X-ray crystallography so far, the octamer displays reduced base pair tilt, increased rise per base pair and a more open major groove compared with canonical A-DNA. We propose that, based on these parameters, three A-helical sub-families may be defined; d(GGGATCCC) then is a representative of the class with intermediate tilt, rise, and major groove width.

Refinement of the solution structure of the RNA-DNA hybrid 5'-[r(GCA)d(TGC)]2. Combined use of nuclear magnetic resonance and restrained molecular dynamics

The solution conformation of the self-complementary RNA-DNA hybrid hexamer 5'-[r(GCA)d(TGC)]2 is investigated by NMR spectroscopy and restrained molecular dynamics. The 1H-NMR spectrum is assigned in a sequential manner using two-dimensional homonuclear Hartmann-Hahn and nuclear Overhauser enhancement spectroscopy. From the latter a set of 178 approximate interproton distance restraints are determined and used as the basis of a structure refinement by restrained molecular dynamics. Eight independent calculations are carried out, four from a classical A-type geometry and four from a classical B-type one. Convergence is achieved to very similar A-type structures with an average atomic root mean square difference between them of 1.0 +/- 0.2 A. The converged structures exhibit variations in helical parameters similar to those found previously for the analogue RNA hexamer 5'-r(GCAUGC)2 [(1988) Biochemistry 27, 1735-1743].

The role of modifications in oligonucleotides in sequence recognition by MvaI restriction endonuclease

The interaction of MvaI restriction endonuclease with 14-membered deoxyribonucleotide duplexes containing modifications within the recognition site (CCA/TGG) has been studied. Substitution of m5dC for the internal dC residue, as well as substitution of fl5dU or rU for dT did not influence the initial rate of hydrolysis (v0) of modified strands, whereas the hydrolysis of unmodified strands was inhibited in some cases. Furthermore, the substitution of a pyrophosphate bond for a scissile phosphodiester bond in one strand completely inhibited digestion in this strand without any decrease of the rate of hydrolysis of the unmodified strand. In contrast to EcoRII endonuclease, which recognizes the same DNA sequence, in the case of MvaI endonuclease substrate recognition is possible in a wide range of conformational, electronic and hydrophobic alterations within the recognition site.

Site-directed modification of DNA duplexes by chemical ligation

The efficiency of chemical ligation method have been demonstrated by assembling a number of DNA duplexes with modified sugar phosphate backbone. Condensation on a tetradecanucleotide template of hexa(penta)- and undecanucleotides differing only in the terminal nucleoside residue have been performed using water-soluble carbodiimide as a condensing agent. As was shown by comparing the efficiency of chemical ligation of single-strand breaks in those duplexes, the reaction rate rises 70 or 45 times if the 3'-OH group is substituted with an amino or phosphate group (the yield of products with a phosphoramidate or pyrophosphate bond is 96-100% in 6 d). Changes in the conformation of reacting groups caused by mismatched base pairs (A.A, A.C) as well as the hybrid rU.dA pair or an unpaired base make the template-directed condensation less effective. The thermal stability of DNA duplexes was assayed before and after the chemical ligation. Among all of the modified duplexes, only the duplex containing 3'-rU in the nick was found to be a substrate of T4 DNA ligase.

The TFIIIA recognition fragment d(GGATGGGAG).d(CTCCCATCC) is B-form in solution

The deoxyoligonucleotide d(GGATGGGAG).d(CTCCCATCC) is a portion of the gene recognition sequence of transcription factor IIIA (TFIIIA). The crystal structure of this oligonucleotide was shown to be A-form (Mc Call, M., Brown, T., Hunter, W.N., and Kennard, O. 1986 Nature 322, 661-664). The present study employs NMR, optical, chemical and enzymatic techniques to investigate the solution structure of this DNA 9-mer. NMR COSY experiments indicate 16 of the 18 residues are predominantly south (C2'-endo) sugar conformation. NMR NOESY indicates glycosidic angles in the range predicted for B-form DNA as opposed to A-form. Related DNA and RNA self-complementary 18-mer sequences, d(GGATGGGAGC-TCCCATCC), with U substituted for T in RNA, were studied by circular dichroism. CD spectra support B-form structures for the DNA 9-mer and the DNA 18-mer, and A-form for the RNA 18-mer. High trifluoroethanol concentrations induce a B- to A-form transition in the DNA oligonucleotides. Enzymatic and chemical probes also illustrate significant differences between the DNA and the RNA oligonucleotides. We find no evidence to support an A-form conformation for the TFIIIA recognition sequence d(GGATGGGAG).d(CTCCCATCC) in solution.

Preparation of covalently linked DNA-RNA hybrids and arabinocytidine containing DNA fragments

It will be demonstrated that 5'-O-DMT-N-acyl-deoxyribonucleosides, 5'-O-Lev-2'-O-MTHP-N-acyl-ribonucleosides and, also, 2'-O-MTHP-N-acyl-ara-cytidine can be coupled, via the hydroxybenzotriazole phosphotriester approach, to afford two types of DNA-RNA hybrids as well as ara-C containing DNA-fragments. The final removal of acid-labile DMT and MTHP groups could be effected by 1 h treatment with 80% acetic acid of the otherwise unprotected DNA-RNA hybrids. The same acidic hydrolysis did not result in complete removal of the 2'-O-MTHP group from the ara-C unit. Complete deblocking was accomplished after an additional 2 h aqueous HC1 (0.01 M; pH 2.00) treatment.

Hydrogen-bonding effects and 13C-NMR of the DNA double helix

13C-nmr chemical shifts of the nucleotides in DNA are sensitive to hydrogen bonding, especially for three of the carbons immediately bonded to exocyclic oxygen or nitrogen atoms acting as H-bond acceptors or donors. GuoC2, GuoC6 and ThdC4 are strongly deshielded (about 1 ppm) upon Watson-Crick pairing in oligodeoxynucleotide duplexes, regardless of the base sequence. Deshielding at these sites may be useful to distinguish bases involved in Watson-Crick pairs from unpaired bases.

Hydration of transfer RNA molecules: a crystallographic study

Four crystal structures of transfer RNA molecules were refined at 3 A resolution with the inclusion of the solvent molecules found in the difference maps: yeast tRNA-phe in the orthorhombic form, yeast tRNA-phe in the monoclinic form and yeast tRNA-asp in the A and B forms. Over 100 solvent molecules were located in each tRNA crystal. Several hydration schemes are found repeatedly in the 4 crystals. The tertiary interactions in the corner of the L-shaped molecule attract numerous solvent molecules which bridge the ribose hydroxyl O(2') atoms, base exocyclic atoms and phosphate anionic oxygen atoms. Conservation of bases leads to conservative localized hydration patterns. Several solvent molecules are found stabilizing unusual base pairs like the G-U pairs and those involving the pseudouridine base. Water bridges between the O(2') and the exocyclic atom O2 of pyrimidines or the N3 atom of purines are common. Water bridges occur frequently between successive anionic oxygen atoms of each strand as well as between N7 or other exocyclic atoms of successive bases in the major groove. Magnesium ions or spermine molecules are found to bind in the major groove of tRNA helices without specific interactions.

Base sequence effects in double helical DNA. I. Potential energy estimates of local base morphology

A series of potential energy calculations have been carried out to estimate base sequence dependent structural differences in B-DNA. Attention has been focused on the simplest dimeric fragments that can be used to build long chains, computing the energy as a function of the orientation and displacement of the 16 possible base pair combinations within the double helix. Calculations have been performed, for simplicity, on free base pairs rather than complete nucleotide units. Conformational preferences and relative flexibilities are reported for various combinations of the roll, tilt, twist, lateral displacement, and propeller twist of individual residues. The predictions are compared with relevant experimental measures of conformation and flexibility, where available. The energy surfaces are found to fit into two distinct categories, some dimer duplexes preferring to bend in a symmetric fashion and others in a skewed manner. The effects of common chemical substitutions (uracil for thymine, 5-methyl cytosine for cytosine, and hypoxanthine for guanine) on the preferred arrangements of neighboring residues are also examined, and the interactions of the sugar-phosphate backbone are included in selected cases. As a first approximation, long range interactions between more distant neighbors, which may affect the local chain configuration, are ignored. A rotational isomeric state scheme is developed to describe the average configurations of individual dimers and is used to develop a static picture of overall double helical structure. The ability of the energetic scheme to account for documented examples of intrinsic B-DNA curvature is presented, and some new predictions of sequence directed chain bending are offered.

Crystal structure analysis of an A-DNA fragment at 1.8 A resolution: d(GCCCGGGC)

Single crystals of the self-complementary octadeoxyribonucleotide d(GCCCGGGC) have been analysed by X-ray diffraction methods at a resolution of 1.8 A. The tetragonal unit cell of space group P4(3)2(1)2 has dimensions of a = 43.25 A and c = 24.61 A and contains eight strands of the oligonucleotide. The structure was refined by standard crystallographic techniques to an R factor of 17.1% using 1359 3 sigma structure factor observations. Two strands of the oligonucleotide are related by the crystallographic dyad axis to form a DNA helix in the A conformation. The d(GCCCGGGC) helix is characterized by a wide open major groove, a near perpendicular orientation of base pairs to the helix axis and an unusually small average helix twist angle of 31.3 degrees indicating a slightly underwound helix with 11.5 base pairs per turn. Extensive cross-strand stacking between guanine bases at the central cytosine-guanine step is made possible by a number of local conformational adjustments including a fully extended sugar-phosphate backbone of the central guanosine nucleotide.

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.

Conformations of duplex structures formed by oligodeoxynucleotides covalently linked to the intercalator 2-methoxy-6-chloro-9-aminoacridine

A family of covalent complexes between oligonucleotides and derivatives of the intercalating agent 9-amino acridine has been synthesized (Asseline, U., Thuong, N.T. and Helene, C. (1983) C.R.Acad. Sci. (Paris) 297 (III), 369-372) and studied (Lancelot, G., Asseline, U., Thuong, N.T., and Helene, C. (1985) Biochemistry 24, 2521-2529; Lancelot, G., Asseline, U., Thuong, N.T., and Helene, C. (1985) J. Biomol. Str. Dyn. 3, 913-921) with a view to understand nucleic acid-nucleic acid recognition. In order to understand the nature of interactions between the intercalator and the oligonucleotides in such complexes and the sensitivity of such interactions to the polymorphic form of the DNA, we have carried out molecular mechanics simulations on duplex deoxyoligonucleotides d(A)6.d(T)6 (A and B forms) and d(TATC).d(GATA) (B form) covalently bound to 2-methoxy-6-chloro-9-aminoacridine through a pentamethylene linker chain. Structures in which the acridine derivative is end stacked (at the 3' and 5' ends) and in which the dye is intercalated between the terminal base pairs (at both the ends) and between second and third base pairs from the 3' end are all of reasonably low energy in both A and B forms of DNA. Our studies on 3' end complexes find that in the B form, intercalation of the dye between the second and third base pairs is preferred over the other two modes of binding, while in the A form, intercalation between the terminal base pairs is preferred. In the 5' end A and B form complexes, outside stacking and intercalation between the terminal base pairs are preferred, respectively. Our calculations suggest the possibility that the presence of the dye attached covalently to the DNA can induce conformational transitions in the DNA. For example, intercalation of the dye two base pairs from the end could induce an A----B transition.

Phase diagrams for DNA crystallization systems

Phase diagrams for several oligonucleotide duplex-spermine systems have been constructed. These diagrams characterize the duplex and spermine concentrations ranges in which crystalline precipitates are formed. All of them are wedge-like form. The slope of the upper branch of the diagram is determined by the oligonucleotide length. The position of the lower branch depends on both the nucleotide sequence and its length. The position of the lower branch depends on both the nucleotide sequence and its length. It has been shown that the addition to the system of MgCl2 and NaCl salts and MPD results in specific changes in the diagrams. A model for oligonucleotide duplex-spermine system has been suggested which explains the main characteristic features of the obtained phase diagrams. The experimental phase diagrams for the (pGpT)n (pApC)n-spermine system (n = 2,3,4) have been analyzed ion terms of this model and the values of the binding constants of spermine and Mg2+ ions binding to duplexes have been determined. It permitted to identify the complexes that precipitated in different regions of the phase diagrams under various conditions. The diagram obtained in the presence of a cobalt hexammine counterion is also considered. It has been shown that this phase diagram, in general, is similar to those obtained for the oligonucleotide duplex-spermine system.

Sequence dependent conformations of oligomeric DNA's in aqueous solutions and in crystals

In order to determine the sequence dependence of the conformation of deoxynucleotides, Raman spectra have been obtained for the following oligodeoxynucleotides in aqueous salt solutions and in crystals: d(CpG)(I), d(TGCGCGCA)(II), d(CACGCGTG)(III), d(CGTGCACG)(IV), d(CGCATGCG)(V), d(ACGCGCGT)(VI), d(CGCGTACGCG)(VII), d(CGCACGTGCG)(VIII) and d(CGTGCGCACG)(IX), d(GCTATAGC) (X), d(GCATATGC) (XI), d(GGTATACC) (XII) and d(GGATATCC) (XIII). The normal B type conformation is observed for all the oligomer DNA's at low salt (0.1-1.0 M NaCl) concentration in the temperature range of 0-25 degrees C. It was considered possible that all of the first nine oligomers could go into the Z form in aqueous high salt (5.0-6.0 M NaCl) solutions, and under these conditions the last four were considered candidates to go into the A form. The B-type conformation was found to exist in high salt solutions for (I), (IV), (V), (VI), (X), (XI) and (XIII); the Z or partial Z conformation appears in high salt solution for the oligomers, (II), (III), (VII), (VIII) and (IX); an A or partial A conformation appears in high salt solution for (XII). In the crystalline state, (IV), (VIII), (X), and (XI) stay in the B-form and all of the other oligomers adopt the complete Z-form except for (XII) which crystallizes in the A form. In both the crystal and in aqueous solutions, the identification of the conformation genus was made by means of Raman spectroscopy. In the crystal of (I), grown at pH7.0, guanosine is found to be in C3'-endo/syn conformation and cytidine in C2'-endo/anti, which may be taken as the ideal building block of the typical Z conformation. At pH4, (I) crystallizes in a conformation similar to the B genus. A study of the thermally induced B to Z transition has been carried out for (II) and (III). Based on the analysis of Raman spectra of the alternating pyrimidine-purine oligomers which might be expected to go into the Z form, the tendency for these oligonucleotides to adopt the Z form can be ranked as: d(CGCGCGCG) greater than (II) greater than (III) greater than (V) approximately (VI) greater than (IV) for octamers and (VII) greater than (VIII) greater than (IX) for the decamers. Similarly, those oligomers which might have a tendency to go into the A form could be ranked as (XII) greater than (XIII) approximately (X) greater than (XI). These data should provide help in formulating rules for predicting the sequence dependence of the B to A and B to Z transitions. Some possible rules are explored, but precautions should be taken.

A-DNA accommodates adducts derived from diol epoxides of polycyclic aromatic hydrocarbons bound in a "side-stacking" mode

The minor groove of undistorted A-DNA provides a good binding site for planar, hydrophobic moieties such as unmetabolized polycyclic aromatic hydrocarbons (PAHs), and the base pairs at the ends of short oligodeoxynucleotide helices. It also accommodates the chief adduct derived from the metabolically activated form of the carcinogen benzo[a]pyrene. B-DNA lacks such a site. Computerized models have been generated for the major (N2-guanine-linked) adducts formed at this site by both + and - enantiomers of anti-benzo[a]pyrene-7,8-dihydrodiol-9,10-epoxide (anti-BPDE) with poly(dG).poly(dC) in the A-DNA conformation. The BPDE adducts lie in the shallow, relatively hydrophobic minor groove of the A-DNA after empirical potential energy minimization using the program AMBER. We term this binding mode "side-stacking." The side-stacked + anti-BPDE may constitute the chief carcinogenic lesion derived from benzo[a]pyrene.

The potentially Z-DNA-forming sequence d(GTGTACAC) crystallizes as A-DNA

(GT)n/(CA)n sequences have stimulated much interest because of their frequent occurrence in eukaryotic DNA and their potential for forming the left-handed Z-DNA structure. We here report the X-ray crystal structure of a self-complementary octadeoxynucleotide, d(GTGTACAC), at 2.5 A resolution. The molecule adopts a right-handed double-helical conformation belonging to the A-DNA family. In this alternating purine-pyrimidine DNA minihelix the roll and twist angles show alternations qualitatively consistent with Calladine's rules. The average tilt angle of 9.3 degrees is between the values found in A-DNA (19 degrees) and B-DNA (-6 degrees) fibers. It is envisaged that such intermediate conformations may render diversity to genomic DNA. The base-pair tilt angles and the base-pair displacements from the helix axis are found to be correlated for the known A-DNA double-helical fragments.

Principles of sequence-dependent flexure of DNA

The curvature of a bent rod may be defined in several different, but equivalent ways. The best way of describing the curvature of double-helical DNA is by an angle of turning per base step. Curvature comes mainly from the angle of roll between successive base-pairs, and this is defined as positive when the angle opens up on the minor groove side of the bases. DNA forms a plane curve if the roll angle values along the molecule alternate periodically between positive and negative, with a complete period equal to the helical repeat. It is known from studies of crystallized oligomers that the roll angles for particular dinucleotide steps have preferred values, or lie in preferred ranges of values. Therefore the formation of a plane curve will be easier with some base sequences of DNA than with others. We set up a computer algorithm for determining the ease with which DNA of given sequence will adopt a curved form. The algorithm has two different sets of constants: in model 1 the base step parameters come from an inspection of crystallized oligomers, and in model 2 data from a statistical survey of the incidence of dinucleotide steps in a large number of samples of chicken erythrocyte core DNA is incorporated. Both forms of the algorithm successfully locate the dyad of the nucleosome sequence (modulo 10) in a frog gene, and suggest strongly that sequence-dependent flexural properties of DNA play a part in the recognition of binding sites by nucleosome cores.

Different behavior of the octadeoxynucleotides d(A-T)4 and d(T-A)4 at high concentrations of cesium fluoride

High CsF concentrations induce a zig-zag double helix, which we call X-DNA, in poly d(A-T) and also in the octadeoxynucleotide d(T-A)4 while d(A-T)4 remains fixed in a B-DNA form. Intermolecular contacts promote the B-X isomerization of the former oligonucleotide but induce aggregation of the latter. This indicates that there is an intramolecular factor, presumably base stacking in the T-A steps, stabilizing the X-DNA conformation.

Conformational analysis of the octamer d(G-G-C-C-G-G-C-C) in aqueous solution. A one-dimensional and two-dimensional proton NMR study at 300 MHz and 500 MHz

Proton NMR studies in H2O and 2H2O were carried out on the self-complementary DNA octamer d(G-G-C-C-G-G-C-C) and compared with similar studies on the dimethylated analogue d(G-G-m5C-m5C-G-G-C-C) [Sanderson, M. R., Mellema, J.-R., van der Marel, G. A., Wille, G., van Boom, J. H. & Altona, C. (1983) Nucleic Acids Res. 11, 3333-3346]. Base, H1', H2' and H2" resonances were assigned by means of two-dimensional nuclear Overhauser spectroscopy (NOESY) and correlated spectroscopy (COSY) experiments. Chemical shift vs temperature profiles were used to analyze the temperature-dependent conformational behaviour and to extract thermodynamic parameters for the duplex-to-coil transition. Analysis of proton-proton couplings were used to discriminate between J1'2' and J1'2" and between the H2' and H2" resonances as well as to obtain conformational parameters of the sugar rings. From the NOESY and COSY experiments, the temperature profiles and the analysis of the coupling data it is concluded that: (a) the compound adopts a B-DNA-type helix in solution; (b) the sugar rings in the intact duplex display limited conformational freedom; (c) methylation of the cytosine bases at the C5 position has no measurable effect on the conformational behaviour of the octamer, nor on the conformation of the sugar rings; however, methylation does increase the stability of the duplex in aqueous solution under conditions of low salt concentration.

DNA-RNA hybrid secondary structures

DNA-RNA and DNA-DNA duplexes are even more polymorphic than observed previously. DNA-RNA hybrids can have secondary structures like A-DNA or A-RNA, but double helices of the synthetic DNA-RNA hybrids poly(dA) X poly(rU) and poly(dI) X poly(rC), respectively, form 11-fold and 10-fold double-helical structures in which the two chains have quite different conformations. Extensive X-ray fiber diffraction analyses show that in both structures the DNA chains have C-2'-endo-puckered furanose rings, while the anti-parallel RNA chains have C-3'-endo-puckered rings. The bidirectional properties of such duplexes may be important in the transfer of biological information from nucleic acids.

Ordered water structure in an A-DNA octamer at 1.7 A resolution

The crystal structure of the deoxyoctamer d(G-G-Br U-A-BrU-A-C-C) was refined to a resolution of 1.7 A using combined diffractometer and synchrotron data. The analysis was carried out independently in two laboratories using different procedures. Although the final results are identical the comparison of the two approaches highlights potential problems in the refinement of oligonucleotides when only limited data are available. As part of the analysis the positions of 84 solvent molecules in the asymmetric unit were established. The DNA molecule is highly solvated, particularly the phosphate-sugar back-bone and the functional groups of the bases. The major groove contains, in the central BrU-A-BrU-A region, a ribbon of water molecules forming closed pentagons with shared edges. These water molecules are linked to the base O and N atoms and to the solvent chains connecting the O-1 phosphate oxygen atoms on each strand. The minor groove is also extensively hydrated with a continuous network in the central region and other networks at each end. The pattern of hydration is briefly compared with that observed in the structure of a B-dodecamer.

Facile cruciform formation by an (A-T)34 sequence from a Xenopus globin gene

We have studied the structure adopted by an (A-T)34 sequence from a Xenopus globin gene when present in a negatively supercoiled plasmid. A variety of enzyme and chemical probing experiments and electrophoretic migration shift methods reveal that the sequence adopts cruciform geometry at moderate levels of supercoiling. The structure has the lowest free energy of formation yet observed for a cruciform, and no detectable kinetic barrier preventing rapid interconversion between extruded and unextruded conformations. Analysis of band-shift experiments reveals a twist change on cruciform formation of -5.8, slightly smaller than the -6.5 we would predict on the basis of a transition from B DNA. An attractive explanation consistent with this discrepancy is that the (A-T)34 stretch is locally underwound to about 11.7 base-pairs/helical turn at low levels of supercoiling. This calculation is made on the assumption that the cruciform junction is structurally similar to those examined previously, which is supported by the nuclease digestion results. This perturbed helical structure could be of considerable biological significance.

Two-dimensional nuclear Overhauser enhancement investigation of the solution structure and dynamics of the DNA octamer [d(GGTATACC)]2

The resonances of nearly all 70 of the non-exchangeable protons of the duplex [d(GGTATACC)]2 in aqueous solution are assigned by proton two-dimensional nuclear Overhauser enhancement (2D NOE) spectra obtained in pure absorption phase at 500 MHz. Experimental and theoretical 2D NOE spectra are compared at each mixing time (100, 175, 250 and 400 ms) using two B-DNA structures: a standard B-form and an energy-minimized form. The GG and CC ends of the octamer duplex are well represented by the regular B-DNA structure. But large discrepancies from these models are observed for the 'TATA' box. All 2D NOE data are consistent with nanosecond correlation times, as indicated by non-selective proton spin-lattice relaxation times, but small variations in the correlation time are observed, suggesting that there are some local differences in mobility within the octamer duplex structure in solution.

The structure of the double-stranded RNA pentamer 5'(CACAG) . 5'(CUGUG) determined by nuclear Overhauser enhancement measurements: interproton distance determination and structure refinement on the basis of X-ray coordinates

The structure in solution of the duplex RNA pentamer 5'(CACAG) . 5'(CUGUG), comprising the stem of the T psi C loop of yeast tRNAPhe, has been investigated by means of one- and two-dimensional nuclear Overhauser enhancement measurements. All non-exchangeable base and sugar proton resonances with the exception of the H5'/H5" sugar resonances are assigned in a sequential manner. From the relative intensities of the cross-peaks obtained in the pure-phase absorption two-dimensional nuclear Overhauser enhancement spectra at several mixing times, it is deduced that the RNA pentamer adopts an A-type conformation in solution. Cross-relaxation rates and interproton distances are determined from the time dependence of the nuclear Overhauser effects, principally by one-dimensional measurements. The structure of the RNA pentamer is then refined by restrained least-squares minimization on the basis of both distance and planarity restraints using fibre diffraction data as an initial model. The refined structure of the RNA pentamer is of the A type but exhibits local structural variations in glycosidic bond and backbone torsion angles as well as in propeller twist, base roll and base tilt angles.

Regularities in formation of the spine of hydration in the DNA minor groove and its influence on the DNA structure

Computer calculations as well as an analysis of space-filling models and literature data allowed the following conclusions to be made: an ordered spine of water in the DNA minor groove, similar to that revealed in the CGCGAATTCGCG crystal, seems to exist in DNA crystals, fibers and solutions; it is shown that this spine may be formed on A/T runs containing no TA step while on the TA step the spine is disrupted; the existence of this spine changes the double helix structure stabilizing a definite DNA conformation; the spine of hydration makes the DNA more stable to conformational transitions. These conclusions permit us to interpret a large body of experimental data on DNA crystals, fibers and solutions. The role of water bridges constituting the first hydration shell of the ordered spine of water is discussed in connection with the B-to-A transition.

The crystal structure of d(G-G-G-G-C-C-C-C). A model for poly(dG).poly(dC)

The structure of the DNA oligomer d(G-G-G-G-C-C-C-C) has been determined at a resolution of 2.5 A by single-crystal X-ray methods. There are two strands in the asymmetric unit, and these coil about each other to form a right-handed double-helix of the A-type with Watson-Crick hydrogen bonds between base-pairs. The helix has a shallow minor groove and a deep, water-filled major groove; almost all exposed functional groups on the DNA are hydrated, and 106 ordered solvent molecules have been found. The two d(G-G-G-G).d(C-C-C-C) segments in the octamer exhibit similar and uniform structures, but there is a slight discontinuity at the GpC step between them. A recurring feature of the structure is the overlap of adjacent guanine bases in each GpG step, with the five-membered ring of one guanine stacking on the six-membered ring of its neighbour. There is little or no overlap between adjacent cytosine rings. Conformational parameters for these GpG steps are compared with those from other single-crystal X-ray analyses. In general, GpG steps exhibit high slide, low roll and variable twist. Models for poly(dG).poly(dC) were generated by applying a simple rotation and translation to each of the unmodified d(G-G-G-G).d(C-C-C-C) units. Detailed features of these models are shown to be compatible with various assays of poly(dG).poly(dC) in solution, and are useful in understanding the polymorphic behaviour of this sequence under a variety of experimental conditions.

Carbon-13 NMR in conformational analysis of nucleic acid fragments. 4. The torsion angle distribution about the C3'-O3' bond in DNA constituents

Carbon-13 and proton NMR spectra of a series of oligodeoxynucleotides (d(CT), d(CC), d(TA), d(AT), d(CG), d(GC), d(AG), d(AAA), d(TATA) and d(GGTAAT] were measured at various temperatures. The three coupling constants that are related to the magnitude of backbone angle epsilon (J(C4'-P), J(C2'-P) and J(H3'-P] are analyzed in terms of a three-state equilibrium about this bond. Two epsilon (trans) angles occur, which differ in magnitude depending on the conformation (N or S) of the adjoining deoxyribose ring. The S-type deoxyribose ring is associated with a smaller epsilon (trans) angle: epsilon (t,S) = 192 degrees. The N-type deoxyribose ring is associated with a larger epsilon (trans) angle epsilon (t,N) = 212 degrees. The third rotamer participating in the conformational equilibrium, is a gauche(-) (epsilon (-] conformer and occurs exclusively in combination with the S-type sugar ring (epsilon (-,S) = 266 degrees). Within the limits of experimental error, the magnitude of these three angles appears to be independent of the particular base sequence, except in the case of d(CG) where a slightly larger epsilon (t,S) angle (197 degrees) is indicated. A simple equation is proposed which may be used to calculate the population of epsilon (t,S) conformer in cases where only J(H3'-P) is known.

Flexibility of 3',5' deoxyribonucleoside diphosphates

In 3',5' deoxyribonucleoside diphosphates, in addition to the nature of the base and the sugar puckering, there are six single bond rotations. However, from the analysis of crystal structure data on the constituents of nucleic acids, only three rotational angles, that are about glycosyl bond, about C4'-C5' and about C3'-O3' bonds, are flexible. For a given sugar puckering and a base, potential energy calculations using non-bonded, electrostatic and torsional functions were carried out by varying the three torsion angles. The energies are represented as isopotential energy surfaces. Since the availability of the real-time color graphics, it is possible to analyse these isopotential energy surfaces. The calculations were carried out for C3' exo and C3' endo puckerings for deoxyribose and also for four bases. These calculations throw more light not only on the allowed regions for the three rotational angles but also on the relationships among them. The dependence of base and the puckering of the sugar on these rotational angles and thereby the flexibility of the 3',5' deoxyribonucleoside diphosphates is discussed. From our calculations, it is now possible to follow minimum energy path for interconversion among various conformers.

The specificity of antibodies elicited by poly(dG).poly(dC)

Antibodies have been raised to the synthetic DNA polymer poly(dG).poly(dC). These antibodies have the ability to distinguish this right-handed polymer from natural mixed sequence DNA, as well as from other right- and left-handed synthetic DNA polymers. They show reduced but measurable binding to synthetic polymers which contain various combinations of guanine and cytosine polynucleotides suggesting that both helical shape and sequence are recognized by this antiserum.

Sequence-dependent structural variation in single-helical DNA. Proton NMR studies of d(T-A-T-A) and d(A-T-A-T) in aqueous solution

The two deoxyribotetranucleoside triphosphates d(T-A-T-A) and d(A-T-A-T) were investigated in aqueous solution by one- and two-dimensional proton NMR at 300 and 500 MHz. It is demonstrated that both compounds occur predominantly in the single-helical form. Accurate coupling constants are obtained by computer simulation of several 500-MHz spectra. The data are interpreted in terms of N and S pseudorotational ranges. The geometry of the major S-type conformers displays a clear sequence dependence, as expressed by variation of the endocyclic backbone angle delta (C5'-C4'-C3'-O3'). A simple sum rule is proposed to predict delta variation in single-helical DNA fragments. Comparisons are made with other sequence-dependent geometries as observed in a double-helical B-DNA fragment in the crystalline state. Furthermore, one- and two-dimensional nuclear Overhauser effect (NOE) spectroscopy was carried out on d(T-A-T-A). An inventory is made of the observed intra- and inter-residue NOEs. The NOE data confirm the presence of a highly stacked single-helical conformation of d(T-A-T-A) in solution. No indications are found for the formation of a bulge-out structure as observed for analogous alternating purine-pyrimidine oligoribonucleotides.

Base-stacking interactions in double-helical DNA structures: experiment versus theory

Atom-atom potential energy calculations have been undertaken for deriving stacking energies in double-helical structures. A comparison between the energy patterns of A- and B-type double-helical fragments determined by single-crystal X-ray diffraction methods versus idealized uniform models based on fibre diffraction data shows that the van der Waals stacking energy is largely sensitive to local changes in the relative orientation of adjacent base pairs. The sequence-dependent conformational variability observed in the high-resolution structures appears to be a consequence of the equipartitioning of the stacking energy along the double helix. The large energy variations expected for a uniform structure are dampened considerably in the observed structures by means of local changes in conformational features such as helix rotation and roll angles between base pairs.

A base-centred explanation of the B-to-A transition in DNA

In the traditional view, the bistable feature responsible for the switch between the B and A forms of DNA was the sugar-phosphate backbone. Several recent assays of the sequence-dependent structure of DNA are not compatible with that hypothesis. Here we show that certain kinds of base-pair step, mainly those of the pyrimidine-purine variety, can stack in a "bistable" fashion so as to produce one of two overall helix shapes A or B. Further, we suggest that the passive, elastic stiffness of the backbone is responsible for communicating the stacking configuration from bistable steps to their "neutral" neighbours. The role of water molecules, in stabilizing the B form of DNA over the A, may simply be to form hydrogen-bonded bridges with the minor-groove edges of neutral steps in the B configuration.

Conformational analysis of the single-helical DNA fragment d(T-A-A-T) in aqueous solution. The combined use of NMR proton chemical shifts and coupling constants obtained at 300 MHz and 500 MHz

Proton NMR studies at 300 MHz and 500 MHz were carried out on the tetranucleoside trisphosphate d(T-A-A-T). The thermodynamics of the three stacking interactions, derived from chemical shift versus temperature profiles, were used to extrapolate the observed coupling constants, measured at a range of temperatures, to values appropriate to the fully stacked forms of the molecule. The data were interpreted in terms of N and S pseudorotational ranges [ Altona , C. and Sundaralingham , M. (1972) J. Am. Chem. Soc. 94, 8205-8212]. It is shown that the stacked state of the molecule cannot be described by one conformer, but consists of one major structure (60%) in which all sugar rings have S-type geometry and another structure (30%) in which residue dT(4) has an N-type sugar. The remainder of the stacked states consists of one or more conformers with two or three sugar residues in the N-type pseudorotational range. Detailed geometrical models are proposed for the major stacked conformers encountered in aqueous solution.

Helix geometry and hydration in an A-DNA tetramer: IC-C-G-G

The DNA oligomer of sequence IC-C-G-G has been synthesized, and its X-ray crystal structure solved at a resolution of 2.0 A, using anomalous scattering from iodines in phase analysis: 48 cycles of Jack-Levitt restrained least-squares refinement resulted in a residual error of 19.9% over all data, or 16.5% for two-sigma data. Two double-helical tetramers stack in the crystal to form a continuous octamer, except for the two missing phosphate connections across the center. The octamer has a mean helix rotation of 33.7 degrees (10.7 base-pairs per turn), rise of 2.87 A, mean inclination angle of base-pairs of 14 degrees, and mean base-pair propeller twist of +16.3 degrees. Local variations in both helix rotation and base plane roll angles, including those across the center of the octamer, are as predicted from base sequence by sum functions sigma 1 and sigma 2. The three known DNA octamers: IC-C-G-G/IC-C-G-G, G-G-T-A-T-A-C-C and G-G-C-C-G-G-C-C, make up a graded series in this order, with monotonically changing structural parameters. An exhaustive comparison of torsion angle correlations among the known A helices confirms some structural expectations and reveals some new features. 86 water molecules have been located per double-helical IC-C-G-G tetramer (the asymmetric unit), of which 451/2 per tetramer lie within a first hydrogen-bonded shell of hydration. No ordered water structure is observed comparable to the minor groove spine of hydration in B-DNA.

Crystallization of transfer ribonucleic acids

A compilation of crystallization experiments of tRNAs published in literature as well as original results are given and discussed in this paper. Up to now 17 different tRNA species originating from Escherichia coli and from the yeast Saccharomyces cerevisiae have been crystallized. All structural tRNA families are represented, namely the tRNAs with large or small extra-loops and among them the initiator tRNAs. The tRNAs with small variable loops (4 to 5 nucleotides), e.g. tRNAAsp and tRNAPhe, yield the best diffracting crystals. Crystalline polymorphism is a common feature; about 100 different crystal forms have been observed, but only 6 among them enabled structure determination studies by X-ray diffraction. Crystallization strongly depends upon experimental parameters such as the presence of polyamines and magnesium as well as upon the purity and the molecular integrity of the tRNAs. Crystals are usually obtained by vapour diffusion methods using salts (e.g. ammonium sulfate), organic solvents (e.g. isopropanol, dioxane or 2-methyl-2,4-pentane diol) or polyethylene glycol as precipitants. A methodological strategy for crystallyzing new tRNA species is described.