The 1.19 A X-ray structure of 2'-O-Me(CGCGCG)(2) duplex shows dehydrated RNA with 2-methyl-2,4-pentanediol in the minor groove

The crystal and molecular structure of 2′-O-Me(CGCGCG)₂ has been determined at 1.19 Å resolution, at 100 K, using synchrotron radiation. The structure in space group P3₂12 is a half-turn right-handed helix that includes two 2-methyl-2,4-pentanediol (MPD) molecules bound in the minor groove. The structure deviates from A-form RNA. The duplex is overwound with an average value of 9.7 bp per turn, characterised as having a C3′-endo sugar pucker, very low base pair rise and high helical twist and inclination angles. The structure includes 65 ordered water molecules. Only a single row of water molecules is observed in the minor groove due to the presence of hydrophobic 2′-O-methyl groups. As many as five magnesium ions are located in the structure. Two are in the major groove and interact with O⁶ and N⁷ of guanosine and N⁴ of cytidine residues through their hydration spheres. This work provides the first example of molecular interactions of nucleic acids with MPD, which was used as a precipitant, cryo-solvent and resolution enhancing agent. The two MPD molecules intrude into the hydration network in the minor groove, each forming hydrogen bonds between their secondary hydroxyl group and exo-amino functions of guanosine residues. Comparison of the 2′-O-Me(CGCGCG)₂ structure in the P3₂12 and P6₁22 crystals delineates stability of the water network within the minor groove to dehydration by MPD and is of interest for evaluating factors governing small molecule binding to RNA. Intrusion of MPD into the minor groove of 2′-O-Me(CGCGCG)₂ is discussed with respect to RNA dehydration, a prerequisite of Z-RNA formation.     

Solution structure of RNA duplexes containing alternating CG base pairs: NMR study of r(CGCGCG)2 and 2'-O-Me(CGCGCG)2 under low salt conditions.

Structures of r(CGCGCG)2 and 2'-O-Me(CGCGCG)2 have been determined by NMR spectroscopy under low salt conditions. All protons and phosphorus nuclei resonances have been assigned. Signals of H5'/5" have been assigned stereospecifically. All 3JH,H and 3JP,H coupling constants have been measured. The structures were determined and refined using an iterative relaxation matrix procedure (IRMA) and the restrained MD simulation. Both duplexes form half-turn, right-handed helices with several conformational features which deviate significantly from a canonical A-RNA structure. Duplexes are characterised as having C3'-endo sugar pucker, very low base-pair rise and high helical twist and inclination angles. Helices are overwound with <10 bp per turn. There is limited inter-strand guanine stacking for CG steps. Within CG steps of both duplexes, the planes of the inter-strand cytosines are not parallel while guanines are almost parallel. For the GC steps this pattern is reversed. The 2'-O-methyl groups are spatially close to the 5'-hydrogens of neighbouring residues from the 3'-side and are directed towards the minor groove of 2'-O-Me(CGCGCG)2 forming a hydrophobic layer. Solution structures of both duplexes are similar; the effect of 2'-O-methylation on the parent RNA structure is small. This suggests that intrinsic properties imposed by alternating CG base pairs govern the overall conformation of both duplexes.     

Water structure around a left-handed Z-DNA fragment analyzed by cryo neutron crystallography

Even in high-quality X-ray crystal structures of oligonucleotides determined at a resolution of 1 Å or higher, the orientations of first-shell water molecules remain unclear. We used cryo neutron crystallography to gain insight into the H-bonding patterns of water molecules around the left-handed Z-DNA duplex [d(CGCGCG)]₂. The neutron density visualized at 1.5 Å resolution for the first time allows us to pinpoint the orientations of most of the water molecules directly contacting the DNA and of many second-shell waters. In particular, H-bond acceptor and donor patterns for water participating in prominent hydration motifs inside the minor groove, on the convex surface or bridging nucleobase and phosphate oxygen atoms are finally revealed. Several water molecules display entirely unexpected orientations. For example, a water molecule located at H-bonding distance from O6 keto oxygen atoms of two adjacent guanines directs both its deuterium atoms away from the keto groups. Exocyclic amino groups of guanine (N2) and cytosine (N4) unexpectedly stabilize waters H-bonded to O2 keto oxygens from adjacent cytosines and O6 keto oxygens from adjacent guanines, respectively. Our structure offers the most detailed view to date of DNA solvation in the solid-state undistorted by metal ions or polyamines.     

Hydrogen and hydration of DNA and RNA oligonucleotides

In this paper, hydrogen bonding interaction and hydration in crystal structures of both DNA and RNA oligonucleotides are discussed. Their roles in the formation and stabilization of oligonucleotides have been covered. Details of the Watson-Crick base pairs G.C and A.U in DNA and RNA are illustrated. The geometry of the wobble (mismatched) G.U base pairs and the cis and almost trans conformations of the mismatched U.U base pairs in RNA is described. The difference in hydration of the Watson-Crick base pairs G.C, A.U and the wobble G.U in different sequences of codon-anticodon interaction in double helical molecules are indicative of the effect of hydration. The hydration patterns of the phosphate, the 2'-hydroxyl groups, the water bridges linking the phosphate group, N7 (purine) and N4 of Cs or O4 of Us in the major groove, the water bridges between the 2'-hydroxyl group and N3 (purine) and O2 (pyrimidine) in the minor groove are discussed.     

The structure of B-helical C-G-A-T-C-G-A-T-C-G and comparison with C-C-A-A-C-G-T-T-G-G. The effect of base pair reversals

The crystal structure of the DNA decamer C-G-A-T-C-G-A-T-C-G has been solved to a resolution of 1.5 A, with a final R-factor of 16.1% for 5,107 two-sigma reflections. Crystals are orthorhombic space group P2(1)2(1)2(1), with cell dimensions a = 38.93 A, b = 39.63 A, c = 33.30 A, and 10 base pairs/asymmetric unit. The final structure contains 404 DNA atoms, 142 water molecules treated as oxygen atoms, and two Mg(H2O)6(2+) complexes. Decamers stack atop one another to simulate continuous helical columns through the crystal, as with three previously solved monoclinic decamers, but the lateral contacts between columns are quite different in the orthorhombic and monoclinic cells. Narrow and wide regions of the minor groove exhibit a single spine or two ribbons of hydration, respectively, and the minor groove is widest when BII phosphate conformations are opposed diagonally across the groove. Phosphate conformation, in turn, appears to have a base sequence dependence. Twist, rise, cup, and roll are linked as has been observed in the three monoclinic decamers and can be characterized by high or low twist profiles. In all five known decamer crystal structures and eight representative dodecamers, a high twist profile is observed with G-C and G-A steps whereas all other R-R steps are low twist profiles (R = purine). A-T and A-C steps are intermediate in character whereas C-A and C-G exhibit behavior that is strongly influenced by the profiles of the preceding and following steps. When sufficient data are in hand, sequence/structure relationships for all helix parameters probably should be considered in a 4-base pair context. At this stage of limited information the problem is compounded because there are 136 unique 4-base steps x-A-B-y in a double helix as compared with only 10 2-base steps A-B.     

Structural principles of B-DNA grooves hydration in fibers as revealed by Monte Carlo simulations and X-ray diffraction

Being interested in possible effects of sequence-dependent hydration of B-DNA with mixed sequence in fibers, we performed a series of Monte Carlo calculations of hydration of polydeoxyribonucleotides in B form, considering all sequences with dinucleotide repeat. The computational results allow the ten base-stacking types to be classified in accordance with their primary hydration in the minor groove. As a rule, the minor groove is occupied by two water molecules per base pair in the depth of the groove, which are located nearly midway between the planes of successive base pairs and symmetrically according to the dyad there. The primary hydration of the major groove depends on the type of the given base pair. The coordinates of 3 water molecules per base pair in the depth of the major groove are determined by the type of this pair together with its position and orientation in the helix, and are practically independent on the adjacent base pairs. A/T-homopolymer tracts do not fit into this hydration pattern; the base pair edges are hydrated autonomously in both grooves. Analysis of the Li-B-DNA x-ray diffraction intensities reveals those two water positions in the minor groove. In the major groove, no electronic density peaks in sufficient distance from the base edges were found, thus confirming the absence of any helical invariance of primary hydration in this region. With the help of the rules proposed in this paper it is possible to position the water molecules of the first hydration shell in the grooves of canonical B-DNA for any given sequence.     

Hydration of RNA base pairs

The hydration patterns around the RNA Watson-Crick and non-Watson-Crick base pairs in crystals are analyzed and described. The results indicate that (i) the base pair hydration is mostly "in-plane"; (ii) eight hydration sites surround the Watson-Crick G-C and A-U base pairs, with five in the deep and three in the shallow groove, an observation which extends the characteristic isostericity of Watson-Crick pairs; (iii) while the hydration around G-C base pairs is well defined, the hydration around A-U base pairs is more diffuse; (iv) the hydration sites close to the phosphate groups are the best defined and the most recurrent ones; (v) a string of water molecules links the two shallow groove 2'-hydroxyl groups, and (vi) the water molecules fit into notches, the size and accessibility of which are almost as important as the number and strength of the hydrophilic groups lining the cavity. Residence times of water molecules at specific hydration sites, inferred from molecular dynamics simulations, are discussed in the light of present data.     

AT base pairs are less stable than GC base pairs in Z-DNA: The crystal structure of d(m5CGTAm5CG)

Two hexanucleoside pentaphosphates, 5-methyl and 5-bromo cytosine derivatives of d(CpGpTp-ApCpG) have been synthesized, crystallized, and their three-dimensional structure solved. They both form left-handed Z-DNA and the methylated derivative has been refined to 1.2 Å resolution. These are the first crystal Z-DNA structures that contain AT base pairs. The overall form of the molecule is very similar to that of the unmethylated or the fully methylated (dC-dG)₃ hexamer although there are slight changes in base stacking. However, significant differences are found in the hydration of the helical groove. When GC base pairs are present, the helical groove is systematically filled with two water molecules per base pair hydrogen bonded to the bases. Both of these water molecules are not seen in the electron density map in the segments of the helix containing AT base pairs, probably because of solvent disorder. This could be one of the features that makes AT base pairs form Z-DNA less readily than GC base pairs.     

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.     

Ordered transcription of RNA tumor virus genomes.

The crystal structure of sodium adenylyl-3′,5′-uridine (ApU) hexahydrate has been determined by X-ray diffraction procedures and refined to an R factor of 0.057. ApU crystallizes with two molecules per asymmetric unit in a monoclinic unit cell, space group P2₁, with cell dimensions: $\text{a = 18.025, b = 17.501, c = 9.677}\text{A}\text{?}\text{and}\text{β = 99.45 °}$. The two independent molecules of ApU form a small segment of right-handed antiparallel double-helical RNA in the crystal, with Watson-Crick base-pairing between adenine and uracil. This is the first time that this Watson-Crick base-pair has been seen unambiguously at atomic resolution and it is also the first time that a nucleic acid fragment with double-helical symmetry has been seen at atomic resolution. The distance between the C1′ atoma of the adenine-uracil base-pair is slightly shorter than the analogous distance seen in guanine-cytosine base-pairs. The bases in each strand are heavily stacked. One sodium cation binds to the phosphates, as expected; however, the other sodium cation binds on the dyad axis in the minor groove of the double helix. It is co-ordinated directly to the two uracil carbonyl groups which protrude into the minor groove and is shielded from the nearest phosphates by a shell of water. This binding appears to be sequence-specific for ApU. One of the adenines also forms a pair of hydrogen bonds to a nearby ribose, utilizing N6 and N7. The 12 water molecules per double-helical fragment are all part of the first co-ordination shell. The ions and the symmetry of the double-helical fragment are the major organizing elements of the solvent region.     

Analysis of the stability and flexibility of RNA complexes containing bulge loops of different sizes

Molecular dynamics simulations of RNA molecules consisting of an antisense oligonucleotide forming a complex with a target strand thereby creating an internal bulge-loop with 3, 4, or 5 nucleotides have been performed with and without O2' methylation of the antisense strand. The methylation influcences minor groove hydration, in particular near guanines but also around the methylated O2', and it also reduces the flexibility of both RNA strands. A G.U wobble pair adjacent to the bulge-loop is also found to increase the flexibility of the bulge nucleotides, compared to the situation with a standard Watson-Crick G-C base-pair in the same position.     

Base pair buckling can eliminate the interstrand purine clash at the CpG steps in B-DNA caused by the base pair propeller twisting

Results of calculations using various empirical potentials suggest that base pair buckling, which commonly occurs in DNA crystal structures, is sufficient to eliminate the steric clash at CpG steps in B-DNA, originating from the base pair propeller twisting. The buckling is formed by an inclination of cytosines while deviations of guanines from a plane perpendicular to the double helix axis are unfavorable. The buckling is accompanied by an increased vertical separation of the base pair centers but the buckled arrangement of base pairs is at least as stable as when the vertical separation is normal and buckle zero. In addition, room is created by the increased vertical separation for the bases to propeller twist as is observed in DNA crystal structures. Further stabilization of base stacking is introduced into the buckled base pair arrangement by roll opening the base pairs into the double helix minor groove. The roll may lead to the double helix bending and liberation of guanines from the strictly perpendicular orientation to the double helix axis. The liberated guanines further contribute to the base pair buckling and stacking improvement. This work also suggests a characteristic very stable DNA structure promoted by nucleotide sequences in which runs of purines follow runs of pyrimidine bases.     

Crystal structure of an RNA octamer duplex r(CCCIUGGG)2 incorporating tandem I.U wobbles.

The crystal structure of the RNA octamer duplex r(CCCIUGGG)2has been elucidated at 2.5 A resolution. The crystals belong to the space group P21and have unit cell constants a = 33.44 A, b = 43.41 A, c = 49.39 A and beta = 104.7 degrees with three independent duplexes (duplexes 1-3) in the asymmetric unit. The structure was solved by the molecular replacement method and refined to an Rwork/Rfree of 0.185/0.243 using 3765 reflections between 8.0 and 2.5 A. This is the first report of an RNA crystal structure incorporating I.U wobbles and three molecules in the asymmetric unit. Duplex 1 displays a kink of 24 degrees between the mismatch sites, while duplexes 2 and 3 have two kinks each of 19 degrees and 27 degrees, and 24 degrees and 29 degrees, respectively, on either side of the tandem mismatches. At the I.U/U.I mismatch steps, duplex 1 has a twist angle of 33.9 degrees, close to the average for all base pair steps, but duplexes 2 and 3 are underwound, with twist angles of 24.4 degrees and 26.5 degrees, respectively. The tandem I.U wobbles show intrastrand purine-pyrimidine stacking but exhibit interstrand purine-purine stacking with the flanking C.G pairs. The three independent duplexes are stacked non-coaxially in a head-to-tail fashion to form infinite pseudo-continuous helical columns which form intercolumn hydrogen bonding interactions through the 2'-hydroxyl groups where the minor grooves come together.     

Crystal structure of a bulged RNA tetraplex at 1.1 a resolution: implications for a novel binding site in RNA tetraplex

Bulges are an important structural motif in RNA and can be used as recognition and interaction sites in RNA-protein interaction and RNA-RNA interaction. Here we report the first crystal structure of a bulged RNA tetraplex at 1.1 A resolution. The hexamer r(U)(BrdG)r(UGGU) forms a parallel tetraplex with the uridine sandwiched by guanines bulging out. The bulged uridine adopts the syn glycosidic conformation and its O2 and N3 atoms face outwards, serving as an effective recognition and interaction site. The bulge formation both widens the groove width and changes the groove hydrogen-bonding pattern on its 5' side. However, the bulge does not make any bends or kinks in the tetraplex structure. The present study demonstrates the dramatic difference between uridine and guanine in forming tetraplex structure. In addition, both G(syn) tetrad and G(anti) tetrad have been observed. They display the same base-pairing pattern and similar C1'-C1' distance but different hydrogen-bonding patterns in the groove.     

Index to Authors,Volume 3

Abstract

Results of calculations using various empirical potentials suggest that base pair buckling, which commonly occurs in DNA crystal structures, is sufficient to eliminate the steric clash at CpG steps in B-DNA, originating from the base pair propeller twisting. The buckling is formed by an inclination of cytosines while deviations of guanines from a plane perpendicular to the double helix axis are unfavorable. The buckling is accompanied by an increased vertical separation of the base pair centers but the buckled arrangement of base pairs is at least as stable as when the vertical separation is normal and buckle zero. In addition, room is created by the increased vertical separation for the bases to propeller twist as is observed in DNA crystal structures. Further stabilization of base stacking is introduced into the buckled base pair arrangement by roll opening the base pairs into the double helix minor groove. The roll may lead to the double helix bending and liberation of guanines from the strictly perpendicular orientation to the double helix axis. The liberated guanines further contribute to the base pair buckling and stacking improvement. This work also suggests a characteristic very stable DNA structure promoted by nucleotide sequences in which runs of purines follow runs of pyrimidine bases.     

Hydration and recognition of methylated CpG steps in DNA.

The analysis of the hydration pattern around methylated CpG steps in three high resolution (1.7, 2.15 and 2.2 A) crystal structures of A-DNA decamers reveals that the methyl groups of cytosine residues are well hydrated. In comparing the native structure with two structurally distinct forms of the decamer d(CCGCCGGCGG) fully methylated at its CpG steps, this study shows also that in certain structural and sequence contexts, the methylated cytosine base can be more hydrated that the unmodified one. These water molecules seem to be stabilized in front of the methyl group through the formation C-H...O interactions. In addition, these structures provide the first observation of magnesium cations bound to the major groove of A-DNA and reveal two distinct modes of metal binding in methylated and native duplexes. These findings suggest that methylated cytosine bases could be recognized by protein or DNA polar residues through their tightly bound water molecules.     

C-C-A-G-G-C-m5C-T-G-G. Helical fine structure, hydration, and comparison with C-C-A-G-G-C-C-T-G-G.

The self-complementary DNA duplex C-C-A-G-G-C-m5C-T-G-G has been refined against 1.75-A x-ray diffraction data to an R value of 17.4%. In the crystal of space group P6, 10-base pair DNA fragments with characteristic sequence-related fine structure stack end to end to form long antiparallel B-type double helices. As shown by a structure analysis at lower resolution (Heinemann, U., and Alings, C. (1991) EMBO J. 10, 35-43), the overall geometry of C-C-A-G-G-C-m5C-T-G-G is similar to that of the unmethylated analog C-C-A-G-G-C-C-T-G-G despite a different crystal environment. The present high resolution structure analysis permits a detailed comparison of the two duplexes and their hydration spheres. Helical parameters are significantly correlated between both molecules, with the exception of the base pair propeller. Sugar pucker and backbone torsion angles alpha, gamma, delta, and chi show similar mean values, but their individual values deviate significantly between duplexes. In contrast, torsion angles beta, epsilon, and zeta change along the strands of both duplexes in much the same way. The effect of single-site methylation on DNA conformation appears to be small and limited to the base pairs directly involved. Methylation tends to push base pairs toward the minor groove of the helix. A regular minor groove hydration pattern involves dual hydrogen bonding of water molecules to O-4' and base atoms of C-C-A-G-G-C-m5C-T-G-G.     

A molecular dynamics study of the effect of G.T mispairs on the conformation of DNA in solution

The effect of G.T mispair incorporation into a double-helical environment was examined by molecular dynamics simulation. The 60-ps simulations performed on the two hexanucleotide duplexes d (G3C3)2 and d(G3TC2)2 included 10 Na+ counterions and first hydration shell waters. The resulting backbone torsional angle trajectories were analyzed to select time spans representative of conformational domains. The average backbone angles and helical parameters of the last time span for both duplexes are reported. During the simulation the hexamers retained B-type DNA structures that differed from typical A- or B-DNA forms. The overall helical structures for the two duplexes are vary similar. The presence of G.T mispairs did not alter the overall helical structure of the oligonucleotide duplex. Large propeller twist and buckle angles were obtained for both duplexes. The purine/pyrimidine crossover step showed a large decrease in propeller twist in the normal duplex but not in the mismatch duplex. Upon the formation of wobble mispairs in the mismatched duplex, the guanines moved into the minor groove and the thymines moved into the major groove. This helped prevent purine/purine clash and created a deformation in the relative orientation of the glycosidic bonds. It also exposed the free O4 of the thymines in the major groove and N2 of the guanines in the minor groove to interactions with solvent and counterions. These factors seemed to contribute to the apparently higher rigidity of the mismatched duplex during the simulation.     

Synthesis and crystal structure of an octamer RNA r(guguuuac)/r(guaggcac) with G.G/U.U tandem wobble base pairs: comparison with other tandem G.U pairs

We have determined the crystal structure of the RNA octamer duplex r(guguuuac)/r(guaggcac) with a tandem wobble pair, G·G/U·U (motif III), to compare it with U·G/G·U (motif I) and G·U/U·G (motif II) and to better understand their relative stabilities. The crystal belongs to the rhombohedral space group R3. The hexagonal unit cell dimensions are a = b = 41.92 Å, c = 56.41 Å, and γ = 120°, with one duplex in the asymmetric unit. The structure was solved by the molecular replacement method at 1.9 Å resolution and refined to a final R factor of 19.9% and R_free of 23.3% for 2862 reflections in the resolution range 10.0–1.9 Å with F ≥ 2σ(F). The final model contains 335 atoms for the RNA duplex and 30 water molecules. The A-RNA stacks in the familiar head-to-tail fashion forming a pseudo-continuous helix. The uridine bases of the tandem U·G pairs have slipped towards the minor groove relative to the guanine bases and the uridine O2 atoms form bifurcated hydrogen bonds with the N1 and N2 of guanines. The N2 of guanine and O2 of uridine do not bridge the ‘locked’ water molecule in the minor groove, as in motifs I and II, but are bridged by water molecules in the major groove. A comparison of base stacking stabilities of motif III with motifs I and II confirms the result of thermodynamic studies, motif I > motif III > motif II.     

Crystal and molecular structure of the sodium salt of the dinucleotide duplex d(CpG)

The crystal and molecular structure of the sodium salt of deoxycytidylyl-(3H-5H)-deoxyguanosine has been determined from X-ray diffraction data. The crystal, obtained from an aqueous gamma-butyrolactone solution at pH = 5.3 are orthorhombic, P212121, a = 10.640(2), b = 11.184(2) and c = 44.618(4)A. The structure was refined to an R = 0.041. The d(CpG) structure is similar to the ammonium salt solved by Cruse et al.(1). Both structures form a parallel self base paired mini-double helix. In d(CpG).Na+ one of the two paired cytosines is protonated on N(3). The cytosines form 3 hydrogen bonds while the guanines form only 2. The Na+ ion is coordinated with five groups: two water molecules, O(6) of guanine A, N(7) of guanine B and 0(5') of cytosine B, forming a square pyramid. The hydration shell around the mini-helix is analysed and compared with that of the ammonium salt, d(CpG).Na+ is the second d(CpG) oligonucleotide found with a self base pairing arrangement despite of the fact that the crystallization conditions and counterion were different in both cases. The hypothesis that self base pairing is not only a crystallization artifact but may play a role under physiological conditions as a source of transversion mutations is discussed.