Search

The three-dimensional structure of the human histocompatibility antigen HLA-A2 was determined at 3.5 A resolution by a combination of isomorphous replacement and iterative real-space averaging of two crystal forms. The monoclinic crystal form has now been refined by least-squares methods to an R-factor of 0.169 for data from 6 to 2.6 A resolution. A superposition of the structurally similar domains found in the heterodimer, alpha 1 onto alpha 2 and alpha 3 onto beta 2m, as well as the latter pair onto the ancestrally related immunoglobulin constant domain, reveals that differences are mainly in the turn regions. Structural features of the alpha 1 and alpha 2 domains, such as conserved salt-bridges that contribute to stability, specific loops that form contacts with other domains, and the antigen-binding groove formed from two adjacent helical regions on top of an eight-stranded beta-sheet, are analyzed. The interfaces between the domains, especially those between beta 2m and the HLA heavy chain presumably involved in beta 2m exchange and heterodimer assembly, are described in detail. A detailed examination of the binding groove confirms that the solvent-accessible amino acid side-chains that are most polymorphic in mouse and human alleles fill up the central and widest portion of the binding groove, while conserved side-chains are clustered at the narrower ends of the groove. Six pockets or sub-sites in the antigen-binding groove, of diverse shape and composition, appear suited for binding side-chains from antigenic peptides. Three pockets contain predominantly non-polar atoms; but others, especially those at the extreme ends of the groove, have clusters of polar atoms in close proximity to the "extra" electron density in the binding site. A possible role for beta 2m in stabilizing permissible peptide complexes during folding and assembly is presented.

The three-dimensional structure of the native unliganded form of the Leu/Ile/Val-binding protein (Mr = 36,700), an essential component of the high-affinity active transport system for the branched aliphatic amino acids in Escherichia coli, has been determined and further refined to a crystallographic R-factor of 0.17 at 2.4 A resolution. The entire structure consists of 2710 non-hydrogen atoms from the complete sequence of 344 residues and 121 ordered water molecules. Bond lengths and angle distances in the refined model have root-mean-square deviations from ideal values of 0.05 A and 0.10 A, respectively. The overall shape of the protein is a prolate ellipsoid with dimensions of 35 A x 40 A x 70 A. The protein consists of two distinct globular domains linked by three short peptide segments which, though widely separated in the sequence, are proximal in the tertiary structure and form the base of the deep cleft between the two domains. Although each domain is built from polypeptide segments located in both the amino (N) and the carboxy (C) terminal halves, both domains exhibit very similar supersecondary structures, consisting of a central beta-sheet of seven strands flanked on either side by two or three helices. The two domains are far apart from each other, leaving the cleft wide open by about 18 A. The cleft has a depth of about 15 A and a base of about 14 A x 16 A. Refining independently the structure of native Leu/Ile/Val-binding protein crystals soaked in a solution containing L-leucine at 2.8 A resolution (R-factor = 0.15), we have been able to locate and characterize an initial, major portion of the substrate-binding site of the Leu/Ile/Val-binding protein. The binding of the L-leucine substrate does not alter the native crystal structure, and the L-leucine is lodged in a crevice on the wall of the N-domain, which is in the inter-domain cleft. The L-leucine is held in place primarily by hydrogen-bonding of its alpha-ammonium and alpha-carboxylate groups with main-chain peptide units and hydroxyl side-chain groups; there are no salt-linkages. The charges on the leucine zwitterion are stabilized by hydrogen-bond dipoles. The side-chain of the L-leucine substrate lies in a depression lined with non-polar residues, including Leu77, which confers specificity to the site by stacking with the side-chain of the leucine substrate.(ABSTRACT TRUNCATED AT 400 WORDS)

Single, three-dimensional crystals of 50 S ribosomal subunits, from a mutant of Bacillus stearothermophilus that lacks the protein L11, have been characterized using a synchrotron X-ray source. The crystals of the mutated particles grow under the same conditions and are isomorphous to those of the wild type of the same bacteria. They are orthorhombic, contain at least one 2-fold screw axis, and have unit cell dimensions of a = 350(+/- 10) A, b = 670(+/- 10) A, and c = 910(+/- 10) A. They diffract to 15 to 18 A resolution at 4 degrees C and are stable in the synchrotron beam for several hours.

Large, well-ordered three-dimensional crystals of 50 S ribosomal subunits from Halobacterium marismortui have been obtained by seeding. The crystals have been characterized with synchrotron X-ray radiation as monoclinic, space group P2(1), with unit cell dimensions of a = 182(+/- 5) A, b = 584(+/- 10) A, c = 186(+/- 5) A, beta = 109 degrees. At 4 degrees C, the crystals (0.6 mm X 0.6 mm X 0.1 mm) diffract to 6 A resolution and are stable in the synchrotron beam for several hours. Compact packing is reflected from the crystallographic unit cell parameters and from electron micrographs of positively stained thin sections of embedded crystals.

The lectin from Erythrina corallodendron, specific for N-acetyllactosamine, crystallizes in the hexagonal space group P6(1) (P6(5)) with unit cell dimensions a = b = 136.3 A, c = 83.2 A and one dimer of Mr 60,000 in the asymmetric unit. The crystals are suitable for high-resolution work.

Single, three-dimensional crystals of the 50 S ribosomal subunit from Bacillus stearothermophilus (strain NCA) have been characterized using a synchrotron X-ray source. The crystals are orthorhombic with unit cell dimensions: a = 350 A, b = 670 A, c = 905 A, and contain at least one 2-fold screw axis. With cooling to -2 degrees C, the large crystals (1.0 mm X 0.2 mm X 0.1 mm) diffract to 15 to 18 A resolution and are stable in the synchrotron beam for several hours. Despite the large cell dimensions, the reflections are readily resolved when the X-ray diffraction patterns are densitometered with a 25 microns faster.

Crystals of the DNA tridecamer d(C-G-C-A-G-A-A-T-T-C-G-C-G) have been grown by the vapor-diffusion technique with 2-methyl-2,4-pentanediol as precipitant. They are monoclinic space group C2, with a = 79.6 A, b = 43.1 A, c = 24.9 A and beta = 98.7 degrees. Previous nuclear magnetic resonance studies predicted that this tridecamer forms a duplex similar to the B DNA dodecamer, d(C-G-C-G-A-A-T-T-C-G-C-G), except for an extra adenosine residue that is stacked within the helix but remains unpaired: (formula; see text) Preliminary X-ray diffraction studies confirmed that the tridecamer is in the B DNA conformation, consistent with the nuclear magnetic resonance results.