Angular reconstitution of ice embedded macromolecules with arbitrary point group symmetry

Author(s):  
Marin van Heel ◽  
Michael Schatz ◽  
Prakash Dube ◽  
Elena V. Orlova

Electron microscopy of individual non-crystallized (large) macromolecules is a very rapid technique for probing the three-dimensional (3D) structure of biological macromolecules. Since there is no need for extensive crystallization experiments, specimen preparation can be simple and fast. In particular the vitreous-ice embedding specimen preparation technique, in which the macromolecules are kept in a waterlike environment, has proved very suited for this purpose. One may extract three-dimensional information from the data - without ever collecting tilt series in the microscope - by exploiting thedifferent ("random") orientations the macromolecules have with respect to the grid. Collecting tilt series can be cumbersome and requires multiple exposure of the sensitive molecules. The only techniquewhich was available for such single-shot 3D microscopy was the common-lines technique for virusses with icosahedral symmetry [Crowther (1971), Fuller (1987)]. The other technique available for asymmetric non-crystalline specimens is the random conical tilt technique [Radermacher (1986)]. However, this technique is a tilt series technique requiring two exposures per specimen area. Moreover, it requiresthe molecules to be preferentially oriented with respect to the plane of the support film which - in turn - requires strong (and thus unfavourable) interactions between molecule and support.

Author(s):  
Prakash Dube ◽  
Holger Stark ◽  
Elena V. Orlova ◽  
Michael Schatz ◽  
Erich Beckmann ◽  
...  

Electron cryo-microscopy of individual non-crystallized macromolecules (“single particles”) is a very rapid technique for probing the three-dimensional (“3D”) structure of biological macromolecules. By exploiting the different orientations of the macromolecules in the embedding medium, one may extract 3D information from the data without ever collecting tilt series in the microscope. The angular reconstitution approach, designed for this purpose, was recently extended with a number of refinements which allow its use as a routine technique for finding 3D structures of macromolecules with arbitrary pointgroup symmetry, from entirely asymmetric ribosomes to viruses with icosahedral symmetry.The specimen preparation technique associated with the angular reconstitution approach is simple and fast since crystallization experiments are avoided altogether. The vitreous-ice embedding specimen preparation technique remains one of our favorite specimen preparation techniques. We are, however, currently experimenting with specimens embedded in glucose and ammonium molybdate or other heavy-metal salts. Collecting good micrographs can also be quite straightforward since the images are taken from untilted specimens, while exposing each image area only once.


2013 ◽  
Vol 69 (12) ◽  
pp. 2461-2467 ◽  
Author(s):  
Mohammad Syed Ahangar ◽  
Rajan Vyas ◽  
Nazia Nasir ◽  
Bichitra K. Biswal

Imidazoleglycerol-phosphate dehydratase (IGPD; HisB), which catalyses the conversion of imidazoleglycerol-phosphate (IGP) to imidazoleacetol-phosphate in the histidine biosynthesis pathway, is absent in mammals. This feature makes it an attractive target for herbicide discovery. Here, the crystal structure ofMycobacterium tuberculosis(Mtb) IGPD is reported together with the first crystal structures of substrate-bound and inhibited (by 3-amino-1,2,4-triazole; ATZ) forms of IGPD from any organism. The overall tertiary structure ofMtbIGPD, a four-helix-bundle sandwiched between two four-stranded mixed β-sheets, resembles the three-dimensional structures of IPGD from other organisms; however,MtbIGPD possesses a unique structural feature: the insertion of a one-turn 310-helix followed by a loop ten residues in length. The functional form of IGPD is 24-meric, exhibiting 432 point-group symmetry. The structure of the IGPD–IGP complex revealed that the imidazole ring of the IGP is firmly anchored between the two Mn atoms, that the rest of the substrate interacts through hydrogen bonds mainly with residues Glu21, Arg99, Glu180, Arg121 and Lys184 which protrude from three separate protomers and that the 24-mer assembly contains 24 catalytic centres. Both the structural and the kinetic data demonstrate that the inhibitor 3-amino-1,2,4-triazole inhibits IGPD competitively.


2019 ◽  
Vol 36 (7) ◽  
pp. 2237-2243
Author(s):  
Cyril F Reboul ◽  
Simon Kiesewetter ◽  
Dominika Elmlund ◽  
Hans Elmlund

Abstract Motivation No rigorous statistical tests for detecting point-group symmetry in three-dimensional (3D) charge density maps obtained by electron microscopy (EM) and related techniques have been developed. Results We propose a method for determining the point-group symmetry of 3D charge density maps obtained by EM and related techniques. Our ab initio algorithm does not depend on atomic coordinates but utilizes the density map directly. We validate the approach for a range of publicly available single-particle cryo-EM datasets. In straightforward cases, our method enables fully automated single-particle 3D reconstruction without having to input an arbitrarily selected point-group symmetry. When pseudo-symmetry is present, our method provides statistics quantifying the degree to which the 3D density agrees with the different point-groups tested. Availability and implementation The software is freely available at https://github.com/hael/SIMPLE3.0.


Author(s):  
Maksym Seredyuk ◽  
M. Carmen Muñoz ◽  
José A. Real ◽  
Turganbay S. Iskenderov

The title complex, poly[dodeca-μ-cyanido-diiron(III)triplatinum(II)], [FeIII2{PtII(CN)4}3], has a three-dimensional polymeric structure. It is built-up from square-planar [PtII(CN)4]2−anions (point group symmetry 2/m) bridging cationic [FeIIIPtII(CN)4]+∞layers extending in thebcplane. The FeIIatoms of the layers are located on inversion centres and exhibit an octahedral coordination sphere defined by six N atoms of cyanide ligands, while the PtIIatoms are located on twofold rotation axes and are surrounded by four C atoms of the cyanide ligands in a square-planar coordination. The geometrical preferences of the two cations for octahedral and square-planar coordination, respectively, lead to a corrugated organisation of the layers. The distance between neighbouring [FeIIIPtII(CN)4]+∞layers corresponds to the lengtha/2 = 8.0070 (3) Å, and the separation between two neighbouring PtIIatoms of the bridging [PtII(CN)4]2−groups corresponds to the length of thecaxis [7.5720 (2) Å]. The structure is porous with accessible voids of 390 Å3per unit cell.


Author(s):  
Nataliia Yu. Strutynska ◽  
Marina A. Bondarenko ◽  
Ivan V. Ogorodnyk ◽  
Vyacheslav N. Baumer ◽  
Nikolay S. Slobodyanik

Potassium rubidium cobalt(II)/titanium(IV) tris(orthophosphate), Rb0.743K0.845Co0.293Ti1.707(PO4)3, has been obtained using a high-temperature crystallization method. The obtained compound has a langbeinite-type structure. The three-dimensional framework is built up from mixed-occupied (Co/TiIV)O6octahedra (point group symmetry .3.) and PO4tetrahedra. The K+and Rb+cations are statistically distributed over two distinct sites (both with site symmetry .3.) in the large cavities of the framework. They are surrounded by 12 O atoms.


Author(s):  
Ghaleb Alhakmi ◽  
Abderrazzak Assani ◽  
Mohamed Saadi ◽  
Lahcen El Ammari

Two new orthophosphates, BaMn2Fe(PO4)3[barium dimanganese(II) iron(III) tris(orthophosphate)] and SrMn2Fe(PO4)3[strontium dimanganese(II) iron(III) tris(orthophosphate)], were synthesized by solid-state reactions. They are isotypic and crystallize in the orthorhombic system with space group typePbcn. Their crystal structures comprise infinite zigzag chains of edge-sharing FeO6octahedra (point group symmetry .2.) and Mn2O10double octahedra running parallel to [001], linked by two types of PO4tetrahedra. The so-formed three-dimensional framework delineates channels running along [001], in which the alkaline earth cations (site symmetry .2.) are located within a neighbourhood of eight O atoms.


Author(s):  
R. M. Glaeser ◽  
K. H. Downing

Methods of image acquisition and image processing have been improved to such an extent in recent years that it is now possible to obtain electron micrographs of well ordered monolayer crystals of biological macromolecules at 3.5 Å resolution or better. Similar images must be recorded at high tilt angles, preferably up to 60°, in order to reconstruct a three-dimensional density map with comparable resolution. In order to record images at the highest tilt angles it is essential that the specimen be almost perfectly planar, perhaps to a tolerance as low as ±0.1°. In the case of crystalline arrays of bacteriorhodopsin, such a high degree of specimen flatness, or planarity, is seldom achieved by current techniques of specimen preparation, and this fact is a major impediment in advancing the current status of the structure analysis. It is likely that similar problems in achieving adequate specimen flatness will be encountered with monolayer crystals of other biological macromolecules.A physical analysis of the role of surface tension forces and interfacial energies in the preparation of glucose-embedded specimens suggests that flat specimens could hypothetical be obtained on either hydrophilic or hydrophobic carbon films. In practise, we have so far had success with hydrophilic carbon in reliably obtaining strongly diffracting specimens of purple membrane that are flat to better than ±0.5° only when a glow discharge in H2O vapor was used as the process for creating a hydrophilic surface (Figure 1). While this represents progress, the result is still not as good as it needs to be. When using hydrophobic carbon, we have obtained a striking improvement in the consistency of our results by applying the specimen to the wet side of the grid, immediately after picking up a small square of carbon from the surface of a glucose solution with a 400 mesh grid. After mixing, some of the excess solution and sample is removed with the pipette, and the remainder is blotted off by pressing the grid bars directly onto filter paper (see Figure 2). Freshly evaporated carbon can be used immediately after converting it to a state of increased hydrophobicity by heating the carbon, on mica, in a drying oven at 80°C or higher, for a period of one hour or more. Some optimization of the glucose concentration is needed, ranging from 2 percent to 20 percent, apparently depending on residual variation in the surface properties of the carbon film. In the best case up to half of the membranes that “look” flat are indeed flat enough to give diffraction patterns that are isotropically sharp at tilt angles up to 60° (Figure 3). In virtually all cases, however, an acceptable fraction, rarely less than one percent, of the membranes that look flat are, in fact, extremely flat. A new problem encountered at this point, however, is that the specimens become substantially wrinkled when cooled to -120°, as evidenced by the fact that the diffraction pattern is no longer isotropically sharp at high tilt angles. Current research is investigating whether this latest problem can be overcome by using hydrophobic polymer films, rather than carbon, as their coefficient of thermal expansion should be more similar to that of protein crystal than is the case for evaporated carbon.


2015 ◽  
Vol 71 (5) ◽  
pp. m116-m117
Author(s):  
Weilun Wang ◽  
Jingwen Ran

The title compound, [Cu4(C11H13NO4)4]·CH3CH2OH·2.5H2O, is an electronically neutral tetranuclear copper(II) complex with a cubane-like Cu4O4core. The complete molecule has point group symmetry 2. The phenol hydroxy group and one of the three alcohol hydroxy groups of each 2-{[tris(hydroxymethyl)methyl]iminomethyl}phenol ligand are deprotonated, while the secondary amine and the other two hydroxy groups remain unchanged. The CuIIatoms in the Cu4O4core are connected by four μ3-O atoms from the deprotonated alcohol hydroxy groups. Each of the pentacoordinated CuIIions has an NO4distorted square-pyramidal environment through coordination to the tridentate Schiff base ligands. The Cu—N/O bond lengths span the range 1.902 (4)–1.955 (4) Å, similar to values reported for related structures. There are O—H...O hydrogen-bond interactions between the complex molecules and the ethanol and water solvent molecules, leading to the formation of a three-dimensional network. The ethanol solvent molecule is disordered about a twofold rotation axis. One of the two independent water molecules is also located on this twofold rotation axis and shows half-occupancy.


Author(s):  
Ahmed Ould Saleck ◽  
Abderrazzak Assani ◽  
Mohamed Saadi ◽  
Cyrille Mercier ◽  
Claudine Follet ◽  
...  

The title compound, sodium trimagnesium bis(hydrogen phosphate) phosphate, was obtained under hydrothermal conditions. In the crystal, two types of [MgO6] octahedra, one with point group symmetry 2, share edges to build chains extending parallel to [10-1]. These chains are linked together by two kinds of phosphate tetrahedra, HPO4and PO4, the latter with point group symmetry 2. The three-dimensional framework delimits two different types of channels extending along [001]. One channel hosts the Na+cations (site symmetry 2) surrounded by eight O atoms, with Na—O bond lengths varying between 2.2974 (13) and 2.922 (2) Å. The OH group of the HPO4tetrahedron points into the other type of channel and exhibits a strong hydrogen bond to an O atom of the PO4tetrahedron on the opposite side.


2014 ◽  
Vol 70 (12) ◽  
pp. 510-514 ◽  
Author(s):  
Erik Hennings ◽  
Horst Schmidt ◽  
Wolfgang Voigt

The title compounds, strontium perchlorate trihydrate {di-μ-aqua-aquadi-μ-perchlorato-strontium, [Sr(ClO4)2(H2O)3]n}, strontium perchlorate tetrahydrate {di-μ-aqua-bis(triaquadiperchloratostrontium), [Sr2(ClO4)4(H2O)8]} and strontium perchlorate nonahydrate {heptaaquadiperchloratostrontium dihydrate, [Sr(ClO4)2(H2O)7]·2H2O}, were crystallized at low temperatures according to the solid–liquid phase diagram. The structures of the tri- and tetrahydrate consist of Sr2+cations coordinated by five water molecules and four O atoms of four perchlorate tetrahedra in a distorted tricapped trigonal–prismatic coordination mode. The asymmetric unit of the trihydrate contains two formula units. Two [SrO9] polyhedra in the trihydrate are connected by sharing water molecules and thus forming chains parallel to [100]. In the tetrahydrate, dimers of two [SrO9] polyhedra connected by two sharing water molecules are formed. The structure of the nonahydrate contains one Sr2+cation coordinated by seven water molecules and by two O atoms of two perchlorate tetrahedra (point group symmetry ..m), forming a tricapped trigonal prism (point group symmetrym2m). The structure contains additional non-coordinating water molecules, which are located on twofold rotation axes. O—H...O hydrogen bonds between the water molecules as donor and ClO4tetrahedra and water molecules as acceptor groups lead to the formation of a three-dimensional network in each of the three structures.


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