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Biomedical subjects

H R Drew

Publications and source records attributed to H R Drew.

At least 37 records · Page 2Linked to original sources

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.

Base Sequence↗

Structural specificities of five commonly used DNA nucleases.

Five commonly used nucleases were surveyed for their ability to distinguish among several different DNA backbone configurations. The digestion data suggest that: (1) DNAase I binds across the minor groove; whereas (2) nuclease S1 and (3) micrococcal nuclease bind to an exposed single strand; (4) copper/phenanthroline seeks a base-pair step; and (5) DNAase II requires just a stacked single strand of limited exposure. Only micrococcal nuclease is demonstrably base-specific, with a strong preference for T, A over C, G in any structural context.

Autoradiography↗

Sequence-specific binding of echinomycin to DNA: evidence for conformational changes affecting flanking sequences.

The technique of DNAase I footprinting has been used to investigate preferred binding sites for echinomycin on a 160-base-pair DNA fragment from E. coli containing the tyr T promoter sequence. Six binding sites have been precisely located in the sequence; a seventh has been partially identified. The minimum site-size is six base pairs. All the binding sites contain the dinucleotide sequence CpG but no other regularities can be discerned. When the protected regions on each complementary strand are compared it is evident that they are staggered by 2-3 base-pairs towards the 3' end at each site. Footprinting with DNAase II reports a similar, though less precise, pattern of protection. Cutting by both enzymes is markedly enhanced at AT-rich regions flanking the antibiotic-binding sites. This increased susceptibility to nuclease attack can be attributed to an altered helix conformation in the vicinity of the bis-intercalated echinomycin molecule. It seems that certain sequences, mainly runs of A or runs of T, switch from a nuclease-resistant to a nuclease-sensitive form when echinomycin binds nearby.

Base Composition↗

The primary mode of binding of cisplatin to a B-DNA dodecamer: C-G-C-G-A-A-T-T-C-G-C-G.

When cisplatin [cis- diamminodichloroplatinum (II)] is diffused into pre-grown crystals of the B-DNA double-helical dodecamer C-G-C-G-A-A-T-T-C-G-C-G, it binds preferentially to the N7 positions of guanines, with what probably is an aquo bridge between Pt and the adjacent O6 atom of the same guanine. The entire guanine ring moves slightly toward the platinum site, into the major groove. Only three of the eight potential cisplatin binding sites on guanines actually are occupied, and this differential reactivity can be explained in terms of the relative freedom of motion of guanines toward the major groove. This shift of guanines upon ligation may weaken the glycosyl bond and assist in the depurination that leads to mismatch SOS repair and G.C. to T.A. transversion.

Base Sequence↗

DNA structural variations in the E. coli tyrT promoter.

X-ray studies have established that the structure of a right-handed, Watson-Crick double helix can change from place to place along its length as a function of base sequence. The base pairs transmit deformations out to the phosphate backbone, where they can then be recognized by proteins and other DNA-binding reagents. Here we have examined at single-bond resolution the interactions of three commonly used nucleases (DNAase I, DNAase II, and copper-phenanthroline) with a DNA of natural origin, the 160 bp tyrT promoter. All three of these reagents seem sensitive to DNA backbone geometry rather than base sequence per se. Their sequence-dependent patterns of cleavage provide evidence for structural polymorphism of several sorts: global variation in helix groove width, global variation in radial asymmetry, and local variation in phosphate accessibility. These findings explain how sequence zones of a certain base composition, or purine-pyrimidine asymmetry, can influence the recognition of DNA by protein molecules.

Base Sequence↗

Ordered water structure around a B-DNA dodecamer. A quantitative study.

The crystal structure of the double-helical B-DNA dodecamer of sequence C-G-C-G-A-A-T-T-C-G-C-G has been solved and refined independently in three forms: (1) the parent sequence at room temperature; (2) the same sequence at 16 K; and (3) the 9-bromo variant C-G-C-G-A-A-T-TBrC-G-C-G at 7 degrees C in 60% (v/v) 2-methyl-2,4-pentanediol. The latter two structures show extensive hydration along the phosphate backbone, a feature that was invisible in the native structure because of high temperature factors (indicating thermal or static disorder) of the backbone atoms. Sixty-five solvent peaks are associated with the phosphate backbone, or an average of three per phosphate group. Nineteen other molecules form a first shell of hydration to base edge N and O atoms within the major groove, and 36 more are found in upper hydration layers. The latter tend to occur in strings or clusters spanning the major groove from one phosphate group to another. A single spermine molecule also spans the major groove. In the minor groove, the zig-zag spine of hydration that we believe to be principally responsible for stabilizing the B form of DNA is found in all three structures. Upper level hydration in the minor groove is relatively sparse, and consists mainly of strings of water molecules extending across the groove, with few contacts to the spine below. Sugar O-1' atoms are closely associated with water molecules, but these are chiefly molecules in the spine, so the association may reflect the geometry of the minor groove rather than any intrinsic attraction of O-1' atoms for hydration. The phosphate O-3' and O-5' atoms within the backbone chain are least hydrated of all, although no physical or steric impediment seems to exist that would deny access to these oxygen atoms by water molecules.

Chemical Phenomena↗

Reversible bending and helix geometry in a B-DNA dodecamer: CGCGAATTBrCGCG.

A double-helical B-DNA dodecamer has been analyzed by single crystal x-ray diffraction methods and refined independently in four variants: sequence CGCGAATTCGCG at 20 degrees C and at 16 K, and CGCGAATTBrCGCG in 60% methylpentanediol at 20 and at 7 degrees C. The first three forms show a 14-19 degrees bend in overall helix axis, but the fourth is straight and unbent. Detailed comparisons of the various forms have led to a better understanding of helix geometry and bending. Structural principles can be understood best if organized under four headings: 1) intrinsic geometry of the sugar rings, 2) stacking and relative motion of base pairs, 3) geometry of the connecting phosphate backbone, and 4) mechanics of bending in B-DNA. The observed bending is neither completely localized nor smooth and continuous, but an intermediate compromise that can be termed "annealed kinking."

DNA↗

The anatomy of A-, B-, and Z-DNA.

Recent advances in DNA synthesis methods have made it possible to carry out single-crystal x-ray analyses of double-stranded DNA molecules of predetermined sequence, with 4 to 12 base pairs. At least one example has been examined from each of the three known families of DNA helix: A, B, and Z. Each family has its own intrinsic restrictions on chain folding and structure. The observed solvent positions in these crystal structures have confirmed earlier fiber and solution measurements, and have led to proposals explaining the transitions from B to A and from B to Z helices. Prospects are improving for an understanding of the mode of bending of DNA in chromatin, and the way in which specific DNA sequences are recognized by drug molecules and repressor proteins.

Crystallography↗

A new model for DNA containing A.T and I.C base pairs.

DNA polymers containing exclusively A.T or I.C base pairs frequently exhibit D- or E-type X-ray diffraction patterns when dried. The distribution of intensities in fiber patterns appears to demand helical structures with 7 and 7.5 bp/turn, respectively, but it is not stereochemically possible to wind a right-handed antiparallel B-family helix this tightly. It is a simple matter, however, to build a left-handed helix with 7-7.5 bp/turn by incorporating Hoogsteen pairing into a Z helix framework. X-ray intensities calculated from this novel left-handed Hoogsteen model provide as reasonable a fit to the D-DNA diffraction pattern as do intensities calculated from previously proposed right-handed 8-fold models.

Adenine↗

Structure of a B-DNA dodecamer at 16 K.

The crystal structure of the B-DNA dodecamer C-G-C-G-A-A-T-T-C-G-C-G, previously solved and refined at room temperature (290 K), has been analyzed at 16 K (-257 degrees C). The end-to-end winding of the helix does not vary with temperature but remains constant at 10.1 base pairs per turn. Negatively charged phosphate groups throughout the structure do move closer together on cooling, however, probably because of increase in the dielectric constant of water as the temperature is lowered. This has the two-fold effect of reducing the spacing between neighboring double helices from 24.0 to 22.9 A and of narrowing the helix grooves within any isolated molecule. Overall lattice displacements as deduced from crystallographic temperature factors are very much decreased in the 16 K structure, yet displacements at phosphates continue to exceed those of deoxyribose sugars by B = 9 A2 and those of base pairs by B = 22 A2, even at this very low temperature at which practically all thermal motion has been eliminated. These differences, formerly interpreted as evidence for thermal vibration, must now be attributed to static disorder.

DNA↗

Kinematic model for B-DNA.

X-ray structure analysis of B-DNA double helix with sequence C-G-C-G-A-A-T-T-C-G-C-G has revealed several sequence-dependent structural features. Four of these are shown in this paper to be related to one another by simple structural or kinematic principles: (i) the correlation between glycosyl torsion and chi and main chain C4'--C3' torsion angle delta, (ii) the observations that purines prefer larger phi and delta angles than do pyrimidines, (iii) the anticorrelation of phi or of delta angles between sugars associated with one base pair, and (iv) the observation that successive base planes in purine-pyrimidine steps open up the angle between them toward the major groove, whereas pyrimidine-purine steps open toward the minor groove. These features offer the beginning of an understanding of the way in which specific base sequences can perturb the structure of a B-DNA double helix so as to be "read" by intercalating drugs, repressors, and other recognition proteins.

Base Sequence↗

Structure of a B-DNA dodecamer: conformation and dynamics.

The crystal structure of the synthetic DNA dodecamer d(CpGpCpGpApApTpTpCpGpCpG) has been refined to a residual error of R = 17.8% at 1.9-A resolution (two-sigma data). The molecule forms slightly more than one complete turn of right-handed double-stranded B helix. The two ends of the helix overlap and interlock minor grooves with neighboring molecules up and down a 2(1) screw axis, producing a 19 degrees bend in helix axis over the 11-base-pair steps of the dodecamer. In the center of the molecule, where perturbation is least, the helix has a mean rotation of 36.9 degrees per step, or 9.8 base pairs per turn. The mean propeller twist (total dihedral angle between base planes) between A . T base pairs in the center of the molecule is 17.3 degrees, and that between C . G pairs on the two ends averages 11.5 degrees. Individual deoxyribose ring conformations as measured by the C5'-C4'-C3'-O3' torsion angle delta, exhibit an approximately Gaussian distribution centered around the C1'-exo position with delta avg = 123 degrees and a range of 79 degrees to 157 degrees. Purine sugars cluster at high delta values, and pyrimidine sugars cluster at lower delta. A tendency toward 2-fold symmetry in sugar conformation about the center of the molecule is detectable in spite of the destruction of ideal 2-fold symmetry by the molecular bending. More strikingly, sugar conformations of paired based appear to follow a "principle of anticorrelation," with delta values lying approximately the same distance to either side of the center value, delta = 123 degrees. This same anticorrelation is also observed in other DNA and DNA . RNA structures.

Deoxyribose↗

The unfolding of the cytochromes c in methanol and acid.

The cytochromes c are a family of hemoproteins that share a number of structural features: a thioether linkage between the protein and the heme, histidine and methionine as the fifth and sixth iron ligands, and a tertiary structure known as the "cytochrome fold." These proteins follow a common mechanism of equilibrium unfolding in methanol and acid, differing only in their reactivity to the denaturing conditions. The reduced cytochromes c exhibit an increased conformational stability which is consistent with the presence of a strengthened iron-methionine linkage in the reduced state.

Animals↗