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The enzyme 4-oxalocrotonate tautomerase catalyzes the ketonization of dienols, which after further processing become intermediates in the Krebs cycle. The enzyme uses a general acid–base mechanism for proton transfer: the amino-terminal proline has been shown to function as the catalytic base and Arg39 has been implicated as the catalytic acid. We report the results of molecular docking simulations of 4-oxalocrotonate tautomerase with two substrates, 2-hydroxymuconate and 5-carboxymethyl-2-hydroxymuconate. pKa calculations are also performed for the free enzyme. The predicted binding mode of 2-hydroxymuconate is in agreement with experimental data. A model for the binding mode of 5-carboxymethyl-2-hydroxymuconate is proposed which explains the lower catalytic efficiency of the enzyme toward this substrate. The pKa predictions and docking simulations support residue Arg39 as the general acid for the enzyme catalysis. © 1999 John Wiley & Sons, Inc. Biopoly 50: 319–328, 1999

The single-crystal x-ray analysis of orthorhombic CATGGCCATG has revealed a previously unrecognized mode of intrinsic bending in DNA. The decamer shows a smooth bend of 23 degrees over the central four base pairs, caused by preferential stacking interactions at guanine bases. The bend is produced by a roll of base pairs along their long axes, in a direction that compresses the wide major groove of the double helix. This major-groove-compressing bend at GGC, plus the abundant crystallographic evidence that runs of successive adenine bases (A-tracts) are straight and unbent, requires rethinking of the models most commonly invoked to explain A-tract bending. A decade of excellent experimental work involving gel migration experiments, cyclization kinetics, and nucleosome phasing has clearly established that introduction of short A-tracts into a general DNA sequence in synchrony with the natural repeat of the helix leads to bending. But it does not logically and inevitably follow that the actual bending is to be found within these introduced A-tracts or even at junctions with general-sequence B-DNA.

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.

X-ray analysis of the complex of netropsin with the B-DNA dodecamer of sequence C-G-C-G-A-A-T-T-BrC-G-C-G reveals that the antitumor antibiotic binds within the minor groove by displacing the water molecules of the spine of hydration. Netropsin amide NH furnish hydrogen bonds to bridge DNA adenine N-3 and thymine O-2 atoms occurring on adjacent base pairs and opposite helix strands, exactly as with the spine of hydration. The narrowness of the groove forces the netropsin molecule to sit symmetrically in the center, with its two pyrrole rings slightly non-coplanar so that each ring is parallel to the walls of its respective region of the groove. Drug binding neither unwinds nor elongates the double helix, but it does force open the minor groove by 0.5-2.0 A, and it bends back the helix axis by 8 degrees across the region of attachment. The netropsin molecule has an intrinsic twist that favors insertion into the minor groove of B-DNA, and it is given a small additional twist upon binding. The base specificity that makes netropsin bind preferentially to runs of four or more A X T base pairs is provided not by hydrogen bonding but by close van der Waals contacts between adenine C-2 hydrogens and CH groups on the pyrrole rings of the drug molecule. Substitution of one or more pyrroles by imidazole could permit recognition of G X C base pairs as well, and it could lead to a class of synthetic "lexitropsins," capable of reading any desired short sequence of DNA base pairs.

A systematic comparison of crystal structures of nine different B-DNA dodecamers, in three different space groups, with and without A-tracts, shows that crystal packing or lattice forces are of secondary importance for helix axis bending, minor-groove width, and propeller twist. While other local helix parameters may be influenced or even established by crystal packing, the properties just enumerated are determined primarily by base sequence. One and the same crystal packing scheme can accommodate a bend in one of two different directions, or no bend at all. A-tract regions of B-DNA are inherently straight and unbent, with base-pair inclination no different from that of general-sequence B-DNA. Where bends are observed at junctions between G.C and A.T regions, they always involve a roll about base-pair long axes in a direction that compresses the wide major groove and, hence, are 90 degrees away from that necessary for the correctness of the junction model of A-tract bending. The G.C/A.T junction appears to be a flexible hinge, capable of adopting either a straight or a bent conformation under the local influence of weak crystal packing forces. Such forces therefore are a source of information about DNA deformability and not a curse to be deplored. But as an indication of the weakness of crystal packing forces, introduction of a single bromine atom in the major groove is sufficient to eliminate a bend, although brominated and unbrominated crystals are isomorphous.