Biomedical subjects
Publications and source records attributed to D S Goodsell.
Two-dimensional image processing techniques are used to create black and white illustrations from conventional z-buffer images. The illustrations appear to be composed of lines--outlines, contour lines, and hatched shading--but are calculated as grey-scale raster images. They have the advantage of faithful reproduction in publication and ease of display on workstations and laser printers. A FORTRAN source code is provided.
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The Metropolis technique of conformation searching is combined with rapid energy evaluation using molecular affinity potentials to give an efficient procedure for docking substrates to macromolecules of known structure. The procedure works well on a number of crystallographic test systems, functionally reproducing the observed binding modes of several substrates.
The structure of the DNA fluorochrome 4'-6-diamidine-2-phenyl indole (DAPI) bound to the synthetic B-DNA oligonucleotide C-G-C-G-A-A-T-T-C-G-C-G has been solved by single crystal x-ray diffraction methods, at a resolution of 2.4 A. The structure is nearly isomorphous with that of the native DNA molecule alone. With one DAPI and 25 waters per DNA double helix, the residual error is 21.5% for the 2428 reflections above the 2-sigma level. DAPI inserts itself edgewise into the narrow minor groove, displacing the ordered spine of hydration. DAPI and a single water molecule together span the four AT base pairs at the center of the duplex. The indole nitrogen forms a bifurcated hydrogen bond with the thymine O2 atoms of the two central base pairs, as with netropsin and Hoechst 33258. The preference of all three of these drugs for AT regions of B-DNA is a consequence of three factors: (1) The intrinsically narrower minor groove in AT regions than in GC regions of B-DNA, leading to a snug fit of the flat aromatic drug rings between the walls of the groove. (2) The more negative electrostatic potential within the minor groove in AT regions, attributable in part to the absence of electropositive-NH2 groups along the floor of the groove, and (3) The steric advantage of the absence of those same guanine-NH2 groups, thus permitting the drug molecule to sink deeper into the groove. Groove width and electrostatic factors are regional, and define the relative receptiveness of a section of DNA since they operate over several contiguous base pairs. The steric factor is local, varying from one base pair to the next, and hence is the means of fine-tuning sequence specificity.
The crystal structure of the synthetic DNA dodecamer CGCATATATGCG has been solved at 2.2-A resolution. Its central 6 base pairs adopt the alternating-B-DNA helix structure proposed nearly a decade ago. This alternating poly(AT) structure contrasts with the four known examples of what can be termed a poly(A) subfamily of B-DNA structures: CGCAAAAAAGCG, CGCAAATTTGCG, CGCGAATTCGCG, and CGCGAATTbrCGCG, their defining characteristic being a succession of two or more adenines along one strand, in a region of 4 or more A.T base pairs. All five helices show a characteristically narrow minor groove in their AT centers, but the mean propeller twist at A.T base pairs is lower in the alternating poly(AT) helix than in the poly(A) subfamily of helices. Three general principles emerge from x-ray analyses of B-DNA oligonucleotides: (i) GC and mixed-sequence B-DNA have a wide minor groove, whereas the minor groove is narrow in heteropolymer or homopolymer AT sequences. (ii) G.C base pairs have low propeller twist; A.T pairs can adopt a high propeller twist but need not do so. A high propeller twist can be stabilized by cross-strand hydrogen bonds in the major or minor groove, examples being the minor groove bonds seen in CCAAGATTGG and the major groove bonds that can accompany AA sequences in the poly(A) family. (iii) Homopolymer poly(A) tracts may be stiffer than are alternating AT or general-sequence DNA because of these cross-strand major groove hydrogen bonds. Poly(A) tracts appear internally unbent, but bends may occur at junctions with mixed-sequence DNA because of differences in propeller twist, base pair inclination, and base stacking on the two sides of the junction. Bending occurs most easily via base roll, favoring compression of the broad major groove.
One of the questions that constantly is asked regarding x-ray crystal structure analyses of macromolecules is: To what extent is the observed crystal structure representative of the molecular conformation when free in solution, and to what degree is the structure perturbed by intermolecular crystal forces? This can be assessed with DNA oligomers because of an unusual aspect of crystallization self-complementary oligomers should possess a twofold symmetry axis normal to their helix axis, yet more often than not crystal of such oligomers do not use this internal symmetry. The two ends of the helix are crystallographically distinct though chemically identical. Complexes of DNA oligomers with intercalating drugs such as triostin A tend to use their twofold symmetry when they crystallize, whereas complexes with non-intercalating, groove-binding drugs ignore this symmetry unless the drug molecule is very small. A detailed examination of crystal packing in the dodecamer C-G-C-G-A-A-T-T-C-G-C-G provides an explanation of all of the foregoing behavior in terms of the mechanism of nucleation of DNA or DNA-drug complexes on the surface of a growing crystal. Asymmetry of the ends of the DNA helix is the price that is paid for efficient lateral packing of helices within the crystal. The actual end-for-end variation in standard helix parameters is compared with the experimental noise level as gauged by independent re-refinement of the same oligonucleotide structure where available, and with the observed extent of variation of these same parameters along the helix. Oligomers analyzed are the B-DNA dodecamer C-G-C-G-A-A-T-T-C-G-C-G, the A-DNA octamer G-G-T-A-T-A-C-C, and the phosphorothioate analogue of the B-DNA hexamer G-C-G-C-G-C. End-for-end variation, presumably the result of crystal packing is typically double the experimental noise level, and half the variation in the same parameter along the helix. Analysis of crystal packing in the phosphorothioate hexamer, which uses the same P212121 space group as the dodecamer, shows that the highly unsymmetrical B1 vs. BII backbone conformation probably is to be ascribed to crystal packing forces, and not to the sequence of the hexamer.