Projection Structure of Full Length Connexin 43 by Electron Cryo-Crystallography

We previously used electron cryo-crystallography to determine the three-dimensional structure of recombinant gap junction channels formed by a C-terminal truncation mutant of Cx43 (11). The dodecameric channel is formed by the end-to-end docking of two hexameric connexons, each comprised of 24 transmembrane α-helices. We have now generated two-dimensional crystals of the recombinant, full-length channel, as well as crystals in which the C-tail has been completely removed by trypsin digestion. Projection density maps at 7.5 Å resolution closely resemble our previous analysis of the C-terminal truncation mutant (9). A difference map between the full length and trypsin-treated channels suggests that there are small but significant shifts in protein density upon removal of the C-tail.     

Three-dimensional crystals of CaATPase from sarcoplasmic reticulum. Symmetry and molecular packing.

Structural studies of CaATPase from sarcoplasmic reticulum have so far been restricted to low resolution due to the poor order of two-dimensional crystal forms. However, we report that three-dimensional microcrystals of detergent-solubilized CaATPase diffract to 7.2 A in x-ray powder patterns and may therefore provide an opportunity to study CaATPase structure at higher resolutions. In the present study, we have characterized the symmetry and molecular packing of negatively stained crystals by electron microscopy (em). By altering the detergent-to-lipid ratio, different sized crystals were produced, which adhere to an em grid in different orientations. Thus, we obtained micrographs of three different projections and from these determined unit cell dimensions to be 151 X 51 X 158 A and the three-dimensional space group to be C2 with an angle beta very close to 90 degrees; x-ray powder patterns of hydrated, unstained crystals yielded dimensions of 166 X 58 X 164 A. Micrographs from each of two principal projections were averaged to produce two-dimensional density maps. Based on these maps and on the previously determined low-resolution structure of CaATPase, a packing diagram for these three-dimensional crystals is presented and major intermolecular contacts are proposed.     

Non-crystallographic symmetry in the crystal dimer of wheat germ agglutinin

Three isomorphous heavy atom derivatives of wheat germ agglutinin crystals, KAu(CN)₂, K₂Pt(NH₃)₂(NO)₂ and mersalyl, have been examined at high resolution. Heavy atom sites were located from difference Patterson maps in three dimensions at 2.15 Å resolution for the gold and platinum derivatives and with less certainty in the centrosymmetric [010] projection for the mersalyl derivative. These sites are distributed in the crystallographic asymmetric unit such that one half of them can be related to the other half by a 180 ° rotation about an axis parallel to a, and an additional translation of about 6.35 Å along that axis. It is suggested that the two subunits of the wheat germ agglutinin dimer, which represent the asymmetric unit of the C2 unit cell, are related by the same symmetry axis, causing heterologous subunit contacts due to the 6.35 Å translation of one relative to the other subunit.     

Effect of Lipid Head Groups on Double-Layered Two-Dimensional Crystals Formed by Aquaporin-0

Aquaporin-0 (AQP0) is a lens-specific water channel that also forms membrane junctions. Reconstitution of AQP0 with dimyristoyl phosphatidylcholine (DMPC) and E. coli polar lipids (EPL) yielded well-ordered, double-layered two-dimensional (2D) crystals that allowed electron crystallographic structure determination of the AQP0-mediated membrane junction. The interacting tetramers in the two crystalline layers are exactly in register, resulting in crystals with p422 symmetry. The high-resolution density maps also allowed modeling of the annular lipids surrounding the tetramers. Comparison of the DMPC and EPL bilayers suggested that the lipid head groups do not play an important role in the interaction of annular lipids with AQP0. We now reconstituted AQP0 with the anionic lipid dimyristoyl phosphatidylglycerol (DMPG), which yielded a mixture of 2D crystals with different symmetries. The different crystal symmetries result from shifts between the two crystalline layers, suggesting that the negatively charged PG head group destabilizes the interaction between the extracellular AQP0 surfaces. Reconstitution of AQP0 with dimyristoyl phosphatidylserine (DMPS), another anionic lipid, yielded crystals that had the usual p422 symmetry, but the crystals showed a pH-dependent tendency to stack through their cytoplasmic surfaces. Finally, AQP0 failed to reconstitute into membranes that were composed of more than 40% dimyristoyl phosphatidic acid (DMPA). Hence, although DMPG, DMPS, and DMPA are all negatively charged lipids, they have very different effects on AQP0 2D crystals, illustrating the importance of the specific lipid head group chemistry beyond its mere charge.     

Projection structure of full length connexin 43 by electron cryo-crystallography

We previously used electron cryo-crystallography to determine the three-dimensional structure of recombinant gap junction channels formed by a C-terminal truncation mutant of Cx43 (11). The dodecameric channel is formed by the end-to-end docking of two hexameric connexons, each comprised of 24 transmembrane alpha-helices. We have now generated two-dimensional crystals of the recombinant, full-length channel, as well as crystals in which the C-tail has been completely removed by trypsin digestion. Projection density maps at 7.5 A resolution closely resemble our previous analysis of the C-terminal truncation mutant (9). A difference map between the full length and trypsin-treated channels suggests that there are small but significant shifts in protein density upon removal of the C-tail.     

Refined atomic model of the four-layer aggregate of the tobacco mosaic virus coat protein at 2.4-A resolution.

Previous x-ray studies (2.8-A resolution) on crystals of tobacco mosaic virus coat protein grown from solutions containing high salt have characterized the structure of the protein aggregate as a dimer of a bilayered cylindrical disk formed by 34 chemically identical subunits. We have determined the crystal structure of the disk aggregate at 2.4-A resolution using x-ray diffraction from crystals maintained at cryogenic temperatures. Two regions of interest have been extensively refined. First, residues of the low-radius loop region, which were not modeled previously, have been traced completely in our electron density maps. Similar to the structure observed in the virus, the right radial helix in each protomer ends around residue 87, after which the protein chain forms an extended chain that extends to the left radial helix. The left radial helix appears as a long alpha-helix with high temperature factors for the main-chain atoms in the inner portion. The side-chain atoms in this region (residues 90-110) are not visible in the electron density maps and are assumed to be disordered. Second, interactions between subunits in the symmetry-related central A pair have been determined. No direct protein-protein interactions are observed in the major overlap region between these subunits; all interactions are mediated by two layers of ordered solvent molecules. The current structure emphasizes the importance of water in biological macromolecular assemblies.     

2．5分辨率单斜Al－（L－丙氨酸）胰岛素晶体结构研究

空间群为Ｐ２１的Ａ１－（Ｌ－丙氨酸）胰岛素晶胞内,一个不对称单位含有一个六聚体,应用差值Ｆｏｕｒｉｅｒ技术,立体化学制最小二来技术和Ｘ—ＰＬＯＲ程序并辅以电子密度图的人工拟合,解析了分辨率ＡＩ—（Ｌ－丙氨酸）胰岛素（Ａｌ－Ｌ－ＡｌａⅠ）的晶体结构。最终Ｒ因子为２０．６％,与标准键长与键角的均方根偏差分别为和４．１９°,从电子密度图与模型的拟合来看,六聚体中每条Ａ链的Ａｌ位置替换的Ｌ—Ａｌａ清晰可见,每条Ｂ链Ｎ端Ｂ１—Ｂ８伏段都为α螺旋构象,形成了Ｂ１—Ｂ１９的连续α螺旋段。     

Molecular topology in crystals and fibers of hemoglobin S

Several lines of evidence indicate a close correspondence between the linear double filaments in the crystal form of hemoglobin S grown from solutions containing polyethylene glycol and the seven pairs of helical filaments that occur in the 14-filament fibers of hemoglobin S. An analysis of the adjustments to the intermolecular contacts required to convert the double filaments from crystals to fibers is presented here. In addition, postulated contacts between the helical double filaments, which are distinct from any of the contacts of the crystals, are specified for the first time. The movements from crystals to fibers are described in terms of three rotation angles: α, the inclination of the filaments with respect to the fiber axis; δ, the tilt of successive molecules along the filaments; and ω, the rotation of successive molecules along the filaments. On the basis of the fiber structure determined by three-dimensional reconstruction of electron micrographs and the assignment of filament pairs from data on incomplete fibers, the various angles have been evaluated. For the filaments at various radii in the fibers, a varies from 3 ° to 12 °, δ varies from 1 ° to 4 ° and ω is constant at 9 °. The effects of the rotations on the contacts between molecules of hemoglobin S at various positions in the fibers are characterized using surface maps based on polar coordinates. For each residue on the surface of hemoglobin the centroid position of its side-chain is located by a longitude, a latitude and an altitude. Locations on the maps are assigned for the contacts within the helical double filaments, as well as 11 classes of new contacts describing the potential interaction sites between double filaments. The resulting maps (1) deduce roles for the various α mutants of hemoglobin known to influence fiber formation that have been identified by the Benesches; (2) distinguish effects for the α chain mutants on the same (cis) or opposite (trans) α₁β₁ dimer as the β6 Val in asymmetric tetramers; (3) propose new sites where effects of mutations on fiber formation may be found; and (4) suggest why some mutants may inhibit, while others enhance, fiber formation. Concerning the last point, the possibility of certain mutants “correcting” the effects of other mutants is proposed as a test of contact assignments.     

Structure of yeast hexokinase. 3. Low resolution structure of a second crystal form showing a different quaternary structure, heterologous interaction of subunits and substrate binding

A 7 Å resolution electron density map of a second crystal form (called BII) of yeast hexokinase B has been obtained. This crystal form, unlike the first crystal form (BI), binds nucleotide and sugar substrates. While the overall tertiary structure of each subunit appears to be largely the same in both crystal forms, the quaternary structure of the dimer is completely different in the two crystals. The two subunits in the crystallographic asymmetric unit of form BII are related by a molecular screw axis; that is, the two subunits are related by a 160 ° rotation and a 13 Å translation of one subunit relative to the other along the symmetry axis resulting in non-equivalent environments for the two chemically identical subunits. A deep cleft divides each subunit into two domains or lobes of roughly equal size. The helical regions which are clearly visible as rods of electron density in this map constitute at least 40 to 50% of the polypeptide chain and 70 to 80% of one of the lobes. At this resolution the molecule does not appear to be homologous in detail to other kinases such as phosphoglycerate kinase and adenylate kinase. Sugar substrates and inhibitors bind deeply in the cleft which separates the two lobes and produce substantial alterations in the protein structure.     

The aquaporin sidedness revisited

Aquaporins are transmembrane water channel proteins, which play important functions in the osmoregulation and water balance of micro-organisms, plants, and animal tissues. All aquaporins studied to date are thought to be tetrameric assemblies of four subunits each containing its own aqueous pore. Moreover, the subunits contain an internal sequence repeat forming two obversely symmetric hemichannels predicted to resemble an hour-glass. This unique arrangement of two highly related protein domains oriented at 180 degrees to each other poses a significant challenge in the determination of sidedness. Aquaporin Z (AqpZ) from Escherichia coli was reconstituted into highly ordered two-dimensional crystals. They were freeze-dried and metal-shadowed to establish the relationship between surface structure and underlying protein density by electron microscopy. The shadowing of some surfaces was prevented by protruding aggregates. Thus, images collected from freeze-dried crystals that exhibited both metal-coated and uncoated regions allowed surface relief reconstructions and projection maps to be obtained from the same crystal. Cross-correlation peak searches along lattices crossing metal-coated and uncoated regions allowed an unambiguous alignment of the surface reliefs to the underlying density maps. AqpZ topographs previously determined by AFM could then be aligned with projection maps of AqpZ, and finally with human erythrocyte aquaporin-1 (AQP1). Thereby features of the AqpZ topography could be interpreted by direct comparison to the 6 A three-dimensional structure of AQP1. We conclude that the sidedness we originally proposed for aquaporin density maps was inverted.     

An Experimental Tool to Estimate the Probability of a Nucleotide Presence in the Crystal Structures of the Nucleotide–Protein Complexes

A correlation between the ligand–protein affinity and the identification of the ligand in the experimental electron density maps obtained by X-ray crystallography has been tested for a number of RNA-binding proteins. Bacterial translation regulators ProQ, TRAP, Rop, and Hfq together with their archaeal homologues SmAP have been used. The equilibrium dissociation constants for the N-methyl-anthraniloyl-labelled adenosine and guanosine monophosphates titrated by the proteins have been determined by the fluorescent anisotropy measurements. The estimated stability of the nucleotide–protein complexes has been matched with a presence of the nucleotides in the structures of the proposed nucleotide–protein complexes. It has been shown that the ribonucleotides can be definitely identified in the experimental electron density maps at equilibrium dissociation constant <10 μM. At K_D of 20–40 μM, long incubation of the protein crystals in the nucleotide solution is required to obtain the structures of the complexes. The complexes with K_D value higher than 50 μM are not stable enough to survive in crystallization conditions.     

Monovalent cation binding to cubic insulin crystals.

Two localized monovalent cation binding sites have been identified in cubic insulin from 2.8 A-resolution difference electron density maps comparing crystals in which the Na+ ions have been replaced by Tl+. One cation is buried in a closed cavity between insulin dimers and is stabilized by interaction with protein carbonyl dipoles in two juxtaposed alternate positions related by the crystal dyad. The second cation binding site, which also involves ligation with carbonyl dipoles, is competitively occupied by one position of two alternate His B10 side chain conformations. The cation occupancy in both sites depends on the net charge on the protein which was varied by equilibrating crystals in the pH range 7-10. Detailed structures of the cation binding sites were inferred from the refined 2-A resolution map of the sodium-insulin crystal at pH 9. At pH 9, the localized monovalent cations account for less than one of the three to four positive counterion charges necessary to neutralize the negative charge on each protein molecule. The majority of the monovalent counterions are too mobile to show up in the electron density maps calculated using data only at resolution higher than 10 A. Monovalent cations of ionic radius less than 1.5 A are required for crystal stability. Replacing Na+ with Cs+, Mg++, Ca++ or La+++ disrupts the lattice order, but crystals at pH 9 with 0.1 M Li+, K+, NH4+, Rb+ or Tl+ diffract to at least 2.8 A resolution.     

Visualization of intracellular ice crystals formed in very rapidly frozen cells at −27 °C

Tumor cells of an ascites sarcoma of rat were primarily frozen very rapidly with the original host ascitic fluid at ?27 °C by the spraying method. Frozen specimens were fractured and replicated at about ?100 °C under vacuum by a special spray-sandwich method for freeze-etching, and the morphological appearance of ice crystals formed in and around the frozen cells were observed by electron microscopy.The cells cooled very rapidly at ?27 °C actually froze intracellularly, and intracellular ice crystals ranged from 0.03 to 0.5 μm in grain size due to the initial freezing rate of the specimens. In the cells having granulous intracellular ice crystals less than 0.05 μm in grain size, cytoplasmic organelles seemed to maintain their original structures.We suggested in our previous report that these tumor cells, frozen very rapidly at temperatures above ?30 °C, survived intracellular freezing as long as they remained translucent, and optically no ice crystals appeared within them, as seen in intact unfrozen cells. It may therefore be concluded that the tumor cells frozen very rapidly at temperatures near ?30 °C actually freeze intracellularly and probably maintain their viability as long as the size of individual intracellular ice-crystals is kept smaller than 0.05 μm, although the exact critical size of innocuous intracellular ice crystals is uncertain.     

Oxygen-bound Hell's gate globin I by classical versus LB nanotemplate method

X‐ray atomic structure of recombinant Hell's gate globin I (HGbI) from Methylacidophilum infernorum was calculated from the X‐ray diffraction data of two different types of crystals: obtained by classical hanging drop and by LB nanotemplate method under the same crystallization conditions. After the accurate comparison of crystallographic parameters and electron density maps of two structures they appears to be quite similar, while the quality of the crystals grown by LB nanotemplate method was higher then of those grown by classical method. Indeed, the resolution of the LB crystal structure was 1.65 Å, while classical crystals showed only 3.2 Å resolution. Moreover, the reproducibility of this result in the case of LB crystals was much better—nine crystals from 10 gave the same structural results, while only two of 10 classical crystals were appropriate for the X‐ray structure resolution. J. Cell. Biochem. 113: 2543–2548, 2012. © 2012 Wiley Periodicals, Inc.     

Cluster analysis of time-dependent crystallographic data: Direct identification of time-independent structural intermediates

The initial output of a time-resolved macromolecular crystallography experiment is a time-dependent series of difference electron density maps that displays the time-dependent changes in underlying structure as a reaction progresses. The goal is to interpret such data in terms of a small number of crystallographically refinable, time-independent structures, each associated with a reaction intermediate; to establish the pathways and rate coefficients by which these intermediates interconvert; and thereby to elucidate a chemical kinetic mechanism. One strategy toward achieving this goal is to use cluster analysis, a statistical method that groups objects based on their similarity. If the difference electron density at a particular voxel in the time-dependent difference electron density (TDED) maps is sensitive to the presence of one and only one intermediate, then its temporal evolution will exactly parallel the concentration profile of that intermediate with time. The rationale is therefore to cluster voxels with respect to the shapes of their TDEDs, so that each group or cluster of voxels corresponds to one structural intermediate. Clusters of voxels whose TDEDs reflect the presence of two or more specific intermediates can also be identified. From such groupings one can then infer the number of intermediates, obtain their time-independent difference density characteristics, and refine the structure of each intermediate. We review the principles of cluster analysis and clustering algorithms in a crystallographic context, and describe the application of the method to simulated and experimental time-resolved crystallographic data for the photocycle of photoactive yellow protein.     

Determination of the X-ray structure of the snake venom protein omwaprin by total chemical synthesis and racemic protein crystallography

The 50‐residue snake venom protein L ‐omwaprin and its enantiomer D ‐omwaprin were prepared by total chemical synthesis. Radial diffusion assays were performed against Bacillus megaterium and Bacillus anthracis; both L ‐ and D ‐omwaprin showed antibacterial activity against B. megaterium. The native protein enantiomer, made of L ‐amino acids, failed to crystallize readily. However, when a racemic mixture containing equal amounts of L ‐ and D ‐omwaprin was used, diffraction quality crystals were obtained. The racemic protein sample crystallized in the centrosymmetric space group P2₁/c and its structure was determined at atomic resolution (1.33 Å) by a combination of Patterson and direct methods based on the strong scattering from the sulfur atoms in the eight cysteine residues per protein. Racemic crystallography once again proved to be a valuable method for obtaining crystals of recalcitrant proteins and for determining high‐resolution X‐ray structures by direct methods.     

X-ray diffraction study of di and tetra-ligated T-state hemoglobin from high salt crystals.

X-ray diffraction difference electron density maps at 3 A resolution obtained from di and tetra-ligated T-state hemoglobin (Hb) crystals are reported. Crystals isomorphous with native deoxyhemoglobin were obtained from ammonium sulfate solutions incubated with the synthetic allosteric effector RSR-56. RSR-56 binds at two symmetry-related Hb central water cavity sites and each molecule has major interactions with three different subunit side-chains; one effector with Arg141 alpha 2 HC3, Lys99 alpha 1 G6 and Asn108 beta 1 and the other with the symmetry related residues, Arg141 alpha 1 Lys99 alpha 2 and Asn108 beta 2. Crystals mounted in a nitrogen filled glove box were di-ligated as previously found with polyethyleneglycol Hb crystals. Crystals mounted in air under a layer of mother liquor were bright red and showed all four heme groups ligated. The difference electron density from the di-ligated crystals showed atomic movements to be restricted to the immediate neighborhood of the heme groups and the allosteric effector. By contrast, the tetra-ligated structure showed extended difference electron density near amino acid residues around both alpha and beta heme groups and along the alpha 1/beta 2 interface. Ligation of the beta heme group appears to magnify the difference density around the alpha heme groups. There is no evidence of breakage of the Bohr salt bridge, His146 beta HC3----Asp94 beta FG1, in the crystal. The observed difference electron density maps may help to clarify the way the allosteric mechanism is triggered.     

Averaging data derived from images of helical structures with different symmetries.

There are many examples of macromolecules that form helical tubes or crystals, which are useful for structure determination by electron microscopy and image processing. Helical crystals can be thought of as two-dimensional crystals that have been rolled into a cylinder such that two lattice points are superimposed. In many real cases, helical crystals of a particular macromolecule derive from an identical two-dimensional lattice but have different lattice points superimposed, thus producing different helical symmetries which cannot be simply averaged in Fourier-space. When confronted with this situation, one can select images corresponding to one of the observed symmetries at the expense of reducing the number of images that can be used for data collection and averaging, or one can calculate separate density maps from each symmetry, then align and average them together in real-space. Here, we present a third alternative, which is based on averaging of the Fourier-Bessel coefficients, gn,l(r), and which allows the inclusion of data from all symmetry groups derived from a common two-dimensional lattice. The method is straightforward and simple in practice and is shown, through a specific example with real data, to give results comparable to real-space averaging.     

Structural changes within unit cell subunits in crosslinked alpha-chymotrypsin crystals.

The structural effects of bifunctional and polyfunctional protein crosslinking agents on protein molecules are, in principle, studied most exactly by modifying and examining a repeating ordered array of protein molecules, i.e. as in single crystals. While X-ray crystallography was possible with crosslinked carboxypeptidase A (Quiocho &; Richards, 1964), with other protein crystals disorder frequently obscured any reasonably resolvable electron density map. We have examined α-chymotrypsin crystals using electron spin resonance spin labels as a probe of the active site region only, i.e. observing one local region of a protein (crystal) structure in the midst of a (potentially) overall disordered structure. The methods and techniques of handling spin-labeled protein crystals were outlined by Bauer &; Berliner (1979).     

Structure of yeast hexokinase. II. A 6 angstrom resolution electron density map showing molecular shape and heterologous interaction of subunits

An electron density map of yeast hexokinase has been calculated at 6 Å resolution using six heavy atom derivatives. The map shows each of the enzyme's two 51,000 molecular weight subunits to consist of two separate lobes connected by a narrow bridge of density. Furthermore, these two subunits are related to each other in the asymmetric unit of the crystal by a quasi-2-fold rather than a true 2-fold axis. That is, they are related by a rotation of 180 ° plus a relative translation of 3.6 Å along the symmetry axis. This gives rise to a heterologous subunit interaction and a possibility of non-identical structure and function for these chemically identical subunits. The molecule is quite asymmetric, having dimensions of 150 Å × 45 Å × 55 Å. Each subunit is about 80 Å × 40 Å × 50 Å.A portion of an electron density map at 3 Å resolution has been also calculated, based on phases from two heavy atom derivatives. Polypeptide backbone and side chains are visible in this map.