Demonstration of G . U wobble base pairs by Raman and IR spectroscopy

When guanine and uracil form hydrogen bonds in the pairing scheme first proposed by Crick one would expect that poly(A,G) will form an unperturbed double helix with poly U at room temperature in a dilute electrolyte solution (0.1 M NaCl). We have demonstrated by Raman- and IR-spectroscopy that the secondary structure of poly(A.G) · poly U is very similar to the structure of poly A · poly U; only the thermal stability of the double helix seems slightly lower than the stability of poly A · poly U, whereas the average helix length is unaffected by the dispersed G · U base pairs. From our input ratio of guanine and adenine we estimate that about every fourth base pair is a wobble pair.     

Three-dimensional structures of bulge-containing DNA fragments.

The three-dimensional structure of a DNA tridecamer d(CGCAGAATTCGCG)2 containing bulged adenine bases was determined by single crystal X-ray diffraction methods, at 120 K, to 2.6 A resolution. The structure is a B-DNA type double helix with a single duplex in the asymmetric unit. One of the bulged adenine bases loops out from the double helix, while the other stacks in to it. This is in contrast to our preliminary finding, which indicated that both adenine bases were looped out. This revised model was confirmed by the use of a covalently bound heavy-atom derivative. The conformation of the looped-out bulge hardly disrupts base stacking interactions of the bases flanking it. This is achieved by the backbone making a "loop-the-loop" curve with the extra adenine flipping over with respect to the other nucleotides in the strand. The looped-out base intercalates into the stacked-in bulge site of a symmetrically related duplex. The looped-out and stacked-in bases form an A.A reversed Hoogsteen base-pair that stacks between the surrounding base-pairs, thus stabilizing both bulges. The double helix is frayed at one end with the two "melted" bases participating in intermolecular interactions. A related structure, of the same tridecamer, after soaking the crystals with proflavin, was determined to 3.2 A resolution. The main features of this B-DNA duplex are basically similar to the native tridecamer but differ in detail especially in the conformation of the bulged-out base. Accommodation of a large perturbation such as that described here with minimal disruption of the double helix shows both the flexibility and resiliency of the DNA molecule.     

A directional nucleation-zipping mechanism for triple helix formation

A detailed kinetic study of triple helix formation was performed by surface plasmon resonance. Three systems were investigated involving 15mer pyrimidine oligonucleotides as third strands. Rate constants and activation energies were validated by comparison with thermodynamic values calculated from UV-melting analysis. Replacement of a T·A base pair by a C·G pair at either the 5′ or the 3′ end of the target sequence allowed us to assess mismatch effects and to delineate the mechanism of triple helix formation. Our data show that the association rate constant is governed by the sequence of base triplets on the 5′ side of the triplex (referred to as the 5′ side of the target oligopurine strand) and provides evidence that the reaction pathway for triple helix formation in the pyrimidine motif proceeds from the 5′ end to the 3′ end of the triplex according to the nucleation-zipping model. It seems that this is a general feature for all triple helices formation, probably due to the right-handedness of the DNA double helix that provides a stronger base stacking at the 5′ than at the 3′ duplex–triplex junction. Understanding the mechanism of triple helix formation is not only of fundamental interest, but may also help in designing better triple helix-forming oligonucleotides for gene targeting and control of gene expression.     

UDP-glucose dehydrogenase: substrate binding stoichiometry and affinity

Precise structural parameters of polyribonucleotides single stranded helices are determined as well as those of double stranded helices of poly 2′-O-methyl A and of poly A at neutral and acid pH. Infrared linear dichroism investigations indicate the similarity of the conformation of the sugar-phosphate backbone of these single and double stranded helices. The angles of the phosphate group for single stranded helix at neutral pH is found to be oriented at 48° for the 02P02 bisector and at about 65° for the 02–03 line to the helix axis. Similar values were found for double stranded poly A helix at acid pH. These structural parameters obtained for the first time on single stranded polynucleotide helices are proposed to be valid for other similar helical chains such as poly A segments of nuclear or messenger RNA and single stranded CCA acceptor end of transfer RNA.     

Interactions between an anthracycline antibiotic and DNA: molecular structure of daunomycin complexed to d(CpGpTpApCpG) at 1.2-A resolution

The crystal structure of a daunomycin-d(CGTACG) complex has been solved by X-ray diffraction analysis and refined to a final R factor of 0.175 at 1.2-A resolution. The crystals are in a tetragonal crystal system with space group P4(1)2(1)2 and cell dimensions of a = b = 27.86 A and c = 52.72 A. The self-complementary DNA forms a six base pair right-handed double helix with two daunomycin molecules intercalated in the d(CpG) sequences at either end of the helix. Daunomycin in the complex has a conformation different from that of daunomycin alone. The daunomycin aglycon chromophore is oriented at right angles to the long dimension of the DNA base pairs, and the cyclohexene ring A rests in the minor groove of the double helix. Substituents on this ring have hydrogen-bonding interactions to the base pairs above and below the intercalation site. O9 hydroxyl group of the daunomycin forms two hydrogen bonds with N3 and N2 of an adjacent guanine base. Two bridging water molecules between the drug and DNA stabilize the complex in the minor groove. In the major groove, a hydrated sodium ion is coordinated to N7 of the terminal guanine and the O4 and O5 of daunomycin with a distorted octahedral geometry. The amino sugar lies in the minor groove without bonding to the DNA. The DNA double helix is distorted with an asymmetrical rearrangement of the backbone conformation surrounding the intercalator drug. The sugar puckers are C1,C2'-endo, G2,C1'-endo, C11,C1'-endo, and G12,C3'-exo. Only the C1 residue has a normal anti-glycosyl torsion angle (chi = -154 degrees), while the other three residues are all in the high anti range (average chi = -86 degrees). This structure allows us to identify three principal functional components of anthracycline antibiotics: the intercalator (rings B-D), the anchoring functions associated with ring A, and the amino sugar. The structure-function relationships of daunomycin binding to DNA as well as other related anticancer drugs are discussed.     

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.     

Self-replication of chemical systems based on recognition within a double or a triple helix: a realistic hypothesis.

A scenario is proposed by which non-enzymatic self-replication of short RNA molecules could occur. The hypothesis is illustrated for the self-replication of an oligopyrimidine (Y) strand. The successful replication of Y requires a series of plausible steps. The first, experimentally feasible, step involves the template-directed polynucleotide synthesis, based on Watson-Crick base pairing, of an oligopurine (R) strand using Y as the template, and chemically activated mononucleotides as the building blocks. This step will result in the formation of an oligopyrimidine.oligopurine (YR) double helix. The second step requires the use of the double helix as the template for the synthesis of a second oligopyrimidine (Y') strand from activated pyrimidine monomers. This synthesis could be facilitated by the binding of the monopyrimidines in the major groove of the YR double helix, via Hoogsteen-type base pairing with the R strand, establishing in that sense triple helix recognition. This step, if successful, should result in the formation of a new strand, Y', that runs parallel to the oligopurine strand. Y' differs from Y in that all 3'-5' phosphodiester linkages in Y are replaced by 5'-3' linkages in Y'. The resulting triple helix (YRY') is in dynamic equilibrium with YR and free Y'. In subsequent steps, unassociated Y' directs the synthesis of the complementary oligopurine (R') strand forming a new double helix Y'R' that may direct the synthesis of an oligopyrimidine strand, Y, that is expected to be identical to the first strand that started the whole sequence. An attempt is made to generalize the above hypothesis to mixed oligonucleotides containing all four bases and identify the limitations of this hypothesis.     

Local effects of partial adenine-N1-oxidation on poly A-poly U and poly A-2 poly U helix conformations

We prepared helices with noncomplementary bases by N1-oxidation of poly A, followed by reaction with poly U. Mixing curves indicate that doubly and triply helical structures form, with only the unmodified adenines involved in base pair formation. Circular dichroism spectra were examined particularly at the absorbance maximum of the adenine N1-oxide (A*). In the single strand poly (A,A*), there is a relatively strong pair of positive and negative CD bands from the A*. These are greatly reduced in the double helix, and abolished in the triple helix. We conclude that A* stacks in a conventional manner with A in the single strand, but is rotated out of the double and triple helix. In the double helix the A* probably maintains a preferred orientation with respect to the helix, but rotates randomly in the triple helix.     

Unusual duplex formation in purine rich oligodeoxyribonucleotides

The purine rich oligodeoxyribonucleotides 1C, d(ATGACGGAATA) and 2C, d(ATGAGCGAATA) alone exhibit highly cooperative melting transitions. Analysis of the concentration dependence of melting, and electrophoretic studies indicate that these oligomers can form an unusual purine rich offset double helix. The unusual duplex is predicted to contain four A.T, two G.C, and four G.A mismatch base pairs as well as a single A base stacked on the 3' end of each chain of the helix. Other possible models for the duplex are unlikely because they are predicted to contain many base pairs of low stability. Changing the central sequence to CGG or GGG should destabilize the duplex and this is observed. The unusual duplex of 2C is more stable than the duplex of 1C indicating that the stability of G.A base pairs is quite sensitive to the surrounding sequence. Addition of 1C and 2C to their complementary pyrimidine strands results in normal duplexes of similar stability. We feel that the unusual duplexes are significantly stabilized by the intrinsic stacking tendency of purine bases.     

Experimental support for a right-handed vertical double helix

The experimentally observed geometry of a miniature double helix of high anti (χCN fixed ? 120°) nucleic acid structure indicates substantial interstrand base stacking with little intrastrand base stacking. This geometry is consistent with the right-handed vertical double helix in which the base planes are parallel to helical axis proposed by Olson [(1977) Proc. Natl. Acad. Sci. USA 74 , 1775] from theoretical calculations. The experimental data do not agree with the left-handed model in which the base planes are perpendicular to helical axis that has been proposed by Yathindra and Sundaralingam [(1976) Nucl. Acids Res. 3 , 729]. The theoretically computed chemical shift changes for the various double-helical configurations show that for the system examined, only the vertical model can explain the experimentally observed shift trends. The melting curve for the helix–coil transition for high anti dinucleoside monophosphate has been observed for the first time. Even though the experimental data support vertical double helices when χCN is fixed at 120°, data on naturally occurring nucleic acid structures indicate that they have no proclivity to enter into vertically stabilized double-helical arrays.     

Experiment acknowledged the Watson-Crick hypothesis: a review of B-DNA double helix structural features at atomic resolution

The dodecamer d(CGCGAATTCGCG) forms a right-handed B-DNA double helix of a Watson-Crick type both in crystal and solution. It is the first piece of DNA longer than one helix turn whose molecular structure has become known at the atomic resolution. The article reviews qualitative aspects of its structure with a special emphasis on local variations in the disposition of base pairs in the double helix.     

Vibrational fluctuations of hydrogen bonds in a DNA double helix with nonuniform base pairs.

The Green's function technique is applied to a study of breathing modes in a DNA double helix which contains a region of different base pairs from the rest of the double helix. The calculation is performed on a G-C helix in the B conformation with four consecutive base pairs replaced by A-T. The average stretch in hydrogen bonds is found amplified around the A-T base pair region compared with that of poly(dG)-poly(dC). This is likely related to the A-T regions lower stability against hydrogen bond melting. The A-T region may be considered to be the initiation site for melting in such a helix.     

Interactions of quinoxaline antibiotic and DNA: the molecular structure of a triostin A-d(GCGTACGC) complex

The crystal structure of a DNA octamer d(GCGTACGC) complexed to an antitumor antibiotic, triostin A, has been solved and refined to 2.2 A resolution by x-ray diffraction analysis. The antibiotic molecule acts as a true bis intercalator surrounding the d(CpG) sequence at either end of the unwound right-handed DNA double helix. As previously observed in the structure of triostin A-d(CGTACG) complex (A.H.-J. Wang, et. al., Science, 225, 1115-1121 (1984)), the alanine amino acid residues of the drug molecule form sequence-specific hydrogen bonds to guanines in the minor groove. The two central A.T base pairs are in Hoogsteen configuration with adenine in the syn conformation. In addition, the two terminal G.C base pairs flanking the quinoxaline rings are also held together by Hoogsteen base pairing. This is the first observation in an oligonucleotide of. Hoogsteen G.C base pairs where the cytosine is protonated. The principal functional components of a bis-intercalative compound are discussed.     

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.     

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.     

Longitudinal displacements of base pairs in DNA and effects on the dynamics of nonlinear excitations

A model of the DNA is proposed and studied analytically and numerically. The model is an extension of a well known model and describes the double helix as two chains of pendula (each pendulum representing a base). Each base (or pendulum) can rotate and translate along the helix axis. In the continuum limit the system is described by the perturbed Sine–Gordon equation describing the twist of the bases and by a nonlinear partial differential equation (PDE) describing the longitudinal displacements of the bases. This coupled system of PDEs was studied analytically using different approaches and the corresponding results were tested through numerical simulations. It was found that if the coupling parameters satisfy a well defined relationship, then there exist bounded travelling wave solutions.     

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.