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Crystallization, crystal structure analysis and preliminary molecular model of the bilin binding protein from the insect Pieris brassicae.

The bilin binding protein of the butterfly Pieris brassicae has been prepared, crystallized and its crystal structure determined at high resolution using film and FAST area detector intensity data. The crystallographic asymmetric unit contains a tetramer of identical subunits with a molecular weight of about 90,000. The crystal structure was determined by isomorphous replacement. Use was made of the molecular symmetry to improve phases. A molecular interpretation of the electron density distribution and partial tracing of the polypeptide chain was possible without amino acid sequence information, as the fold is very similar to retinol binding protein. It is characterized by a beta-barrel formed by two orthogonal beta-sheets and an alpha-helix. The bilin pigment seems to be bound within the beta-barrel analogously to retinol in retinol binding protein. The tetramer in the crystal has C2 symmetry and is a dimer of dimers of quasi-equivalent subunits.

Amino Acid Sequence↗

Three-dimensional structure of a light chain dimer crystallized in water. Conformational flexibility of a molecule in two crystal forms.

The three-dimensional structure of an immunoglobulin light chain dimer (Mcg) crystallized in deionized water (orthorhombic form) was determined at 2.0 A resolution by phase extension and crystallographic refinement. This structure was refined side-by-side with that of the same molecule crystallized in ammonium sulfate (trigonal form). The dimer adopted markedly different structures in the two solvents. "Elbow bend" angles between pseudo 2-fold axes of rotation relating pairs of "variable" (V) and "constant" (C) domains were found to be 132 degrees in the orthorhombic form and 115 degrees in the trigonal form. Modes of association of the V domains and, to a lesser extent, the pairing interactions of the C domains were different in the two structures. Alterations in the V domain pairing were reflected in the shapes of the binding regions and in the orientations of the side-chains lining the walls of the binding sites. In the trigonal form, for instance, the V domain interface was compartmentalized into a main binding cavity and a deep pocket, whereas these spaces were continuous in the orthorhombic structure. Patterns of ordered water molecules were quite distinct in the two crystal types. In some cases, the solvent structures could be correlated with conformational changes in the proteins. For example, close contacts between V and C domains of monomer 1 of the trigonal form were not retained in orthorhombic crystals. Ordered water molecules filled the space created when the two domains moved apart.

Bence Jones Protein↗

Isolation, crystallization, crystal structure analysis and refinement of B-phycoerythrin from the red alga Porphyridium sordidum at 2.2 A resolution.

The light-harvesting pigment-protein complex B-phycoerythrin from the red alga Porphyridium sordidum has been isolated and crystallized. B-Phycoerythrin consists of three different subunits forming an (alpha beta)6 gamma aggregate. The three-dimensional structure of the (alpha beta)6 hexamer was solved by Patterson search techniques using the molecular model of C-phycocyanin from Fremyella diplosiphon. The asymmetric unit of the crystal cell (space group P3, with a = b = 111.2 A, c = 59.9 A, alpha = beta = 90 degrees, gamma = 120 degrees) contains two (alpha beta) monomers related by a local dyad. Three asymmetric units are arranged around the crystallographic 3-fold axis building an (alpha beta)6 hexamer, as in C-phycocyanin. The crystal structure has been refined by energy-restrained crystallographic refinement and model building. The conventional R-factor of the final model was 18.9% with data to 2.2 A resolution. The molecular structures of the alpha and beta-subunits resemble those of C-phycocyanin. Major changes in comparison to phycocyanin are caused by deletion or insertion of segments involved in protein-chromophore interactions. The singly linked phycoerythrobilin chromophores alpha-84, alpha-140a, beta-84 and beta-155 are each covalently bound to a cysteine by ring A. The doubly linked chromophore beta-50/beta-61 is attached at cysteine beta-50 through ring A and at cysteine beta-61 through ring D. B-Phycoerythrin contains additionally a 30 kDa gamma-subunit, which is presumably located in the central cavity of the hexamer. It is disordered, as a consequence of crystal and local symmetry averaging.

Amino Acid Sequence↗

Characterization and crystal structure of cadmium(II) halide complexes with amino acids and their derivatives VI. The comparison of crystal structures of cadmium(II) halide complexes with three kinds of piperidine carboxylic acids.

Six cadmium(II) halide complexes with dl-piperidine-2-carboxylic acid (DL-Hpipe-2), dl-piperidine-3-carboxylic acid (DL-Hpipe-3), and piperidine-4-carboxylic acid (Hpipe-4), have been prepared and characterized by means of IR and Raman spectra and thermal analysis. The crystal structures of [CdCl2(DL-Hpipe-2)(H2O)], [CdBr2(DL-Hpipe-3)], and [CdCl2(Hpipe-4)] have been determined by X-ray diffraction. These three complexes have one-dimensional polymer structures bridged by halide atoms. The crystal of [CdCl2(DL-Hpipe-2)(H2O)] is orthorhombic with the space group Pca2(1). The cadmium atom is in an octahedral geometry, ligated by a carboxyl oxygen atom, two bridging chlorine atoms, a terminal chlorine atom, a water molecule and a carboxyl oxygen atom of a neighboring molecule. The carboxyl oxygen atoms of DL-Hpipe-2 are coordinated to two cadmium atoms. The unit cell consists of two types of one-dimensional polymer structures: [CdCl2(D-Hpipe-2)(H2O)] and [CdCl2(L-Hpipe-2)(H2O)]. Therefore, it is better to write [CdCl2(DL-Hpipe-2)(H2O)] as [CdCl2(D-Hpipe-2)(H2O)][CdCl2(L-Hpipe-2)(H2O)]. The crystal structure of [CdBr2(DL-Hpipe-3)] is monoclinic with space group P2(1). The cadmium atom is in a distorted octahedral geometry ligated by two carboxyl oxygen atoms and four bridging bromine atoms. This complex consists of either D-Hpipe-3 or L-Hpipe-3. Therefore [CdBr2(DL-Hpipe-3)] is written as [CdBr2(D or L-Hpipe-3)]. The crystal of [CdCl2(Hpipe-4)] is monoclinic with space group P2(1)/n. The structure is similar to that of [CdBr2(D or L-Hpipe-3)].

Amino Acids↗

Design and crystal structures of triple helicates with crystallographic idealized D3 symmetry: the role of side chain effect on crystal packing.

Novel crystallographic D3-symmetric binuclear triple molecular helices [Co2L(1)3][BF4]4 (1), [Zn2L(1)3][BF4]4 (2), [Mn2L(1)3][BF4]4 (3), [Co2L(2)3][BF4]4 (4), [Zn2L(2)3][BF4]4 (5), and [Mn2L(2)3][BF4]4 (6) have been achieved to establish the side chain effect on molecular packing, where L1 is [(C5H4N)C(CH3)=N-(C6H4)-]2CH2 and L2 is [(C5H4N)C(CH3)=N-(C6H4)-]2O, respectively. Crystal structure analyses show that each helix crystallizes in a hexagonal crystal system with space group Pc1 and the general axis of the helix occupies the crystallographic 3-fold axial position with the other three crystallographic 2-fold symmetries perpendicular to it. Each metal center is bound to three pyridylimine units to attain C3 pseudooctahedral coordination geometry with respective equivalent metal-N (CH=N) and metal-N (pyridyl) bonds. It is speculated that the existence of the methyl group might minimize the potential intermolecular interactions, which would be the essential factor controlling the helices formed in idealized crystallographic D3 symmetry. Moreover, crystallographic idealized C3-symmetric helicates [Co2L(3)3][BF4]4 (7), [Zn2L(3)3][BF4]4 (8), [Ni2L(3)3][BF4]4 (9), and [Cu2L(3)3][BF4]4 (10) were also structurally characterized for comparison, where L3 is [(C5H4N)C(CH3)=N-]2. All the results indicate that the existence of the methyl group in the side chain of aromatic ligands could effectively reduce the potential - intermolecular interactions and the side chain effect of the methyl group in crystal packing is robust enough to be exchanged from one network structure to another, which ensures the generality and predictability of the crystallographic idealized symmetry formation to a certain extent.

Journal Article↗

Single-crystal-to-single-crystal transformation of diolefin derivatives in nanocrystals.

Topochemical [2 + 2] cycloaddition polymerization of methyl p-phenylenediacrylate and 2,5-distyrylpyridine in nanocrystals, prepared by the reprecipitation method, were investigated in comparison with those in bulk crystals. The bulk single crystals, larger than 1 mum in size, broke into microcrystals with variety of size and shape in the course of polymerization. Interestingly, however, these nanocrystals show single-crystal-to-single-crystal transformation.

Journal Article↗

Nonclassical crystallization: mesocrystals and morphology change of CaCO3 crystals in the presence of a polyelectrolyte additive.

Crystallization of calcite from differently concentrated calcium chloride solutions by the CO2 gas diffusion technique in the presence of polystyrene sulfonate yields crystal superstructures with unusual morphology. From the typical calcite rhombohedra as a starting situation, the morphology can be systematically varied via rounded edges and truncated triangles to finally concavely bended lens-like superstructures. Although these "crystals" are apparently well-faceted in light microscopy, electron microscopy analysis and BET reveal that the structures are highly porous and are composed of almost perfectly 3D-aligned calcite nanocrystals scaffolded to the final, partly nicely curved superstructures. At high supersaturations, superstructures with changed symmetry indicative of dipolar interaction potentials between the building blocks are found. The present model case also gives evidence for the importance of nonclassical, mesoscopic processes in crystallization in general.

Journal Article↗

The polymorphic drug substances of the European pharmacopoeia. Part 9. Physicochemical properties and crystal structure of acetazolamide crystal forms.

The crystal structure of acetazolamide modification I (mod. I) was determined, and its differences compared with the already known crystal structure of the triclinic modification II (mod. II) are discussed. The monoclinic mod. I crystallizes in space group P2(1)/n with four molecules in the unit cell: a = 4.7674, b = 21.956, and c = 8.186 A, beta = 104.23 degrees. In both modifications, the molecules form hydrogen-bonded centrosymmetric dimers. The two modifications differ distinctly in the spatial arrangement of these pairs and in the hydrogen bonds formed between them. The thermodynamic relationship between the two modifications is demonstrated by a semischematic energy/temperature diagram, based on the results of thermal analysis and solubility experiments. Mod. II is the thermodynamically stable modification at 20 degrees C and enantiotropically related to mod. I. The thermodynamic transition point lies between 120 and 148 degrees C. The solid-state properties of acetazolamide are mainly directed by the strong intermolecular hydrogen bond forces. Thus, the metastable mod. I exhibits a higher density than mod. II and a very high kinetic stability at 20 degrees C. Both modifications can be crystallized from water and the solubility differences are very small, so, in addition to mod. II, the metastable but extremely resistant mod. I is suggested to be suitable for use in solid pharmaceutical formulations.

Acetazolamide↗

Pretilt angle of liquid crystals and liquid-crystal alignment on microgrooved polyimide surfaces fabricated by soft embossing method.

In this study, the soft embossing method is proposed to fabricate periodical microgrooved structure on polyimide surfaces. These microgrooved polyimide surfaces are assembled to form liquid-crystal cells. It is found that the director of liquid crystals uniformly aligns along the groove direction even when the groove width is as high as 3 microm. The anchoring energy of these microgrooved polyimide surfaces is higher than that of the typical rubbed surfaces. The pretilt angle of liquid crystals is adjusted by tuning the surface polarity of the polyimide alignment layer, which is identified by the advancing contact angle of water. The surface polarity of polyimide alignment layers is manipulated by simply mixing two kinds of polyimide: a more hydrophilic one and a more hydrophobic one. It is found that the pretilt angle of liquid crystals increases along with the advancing contact angle of water on the alignment layer under the condition of a fixed surface topography.

Journal Article↗

Intramitochondrial yolk-crystals of frog oocytes. I. Formation of yolk-crystal inclusions by mitochondria during bullfrog oogenesis.

Electron microscope examination of thin sections of bullfrog (Rana catesbeiana) ovarian oocytes has shown the presence of mitochondria containing yolk-crystal inclusions in oocytes of all sizes, from 160 to 1500 micro mean diameter. The hexagonally shaped yolk-crystals have major periodicities of 73.8 +/- 10.7 A (n = 100). Several forms of modified mitochondria, observed in the smaller oocytes, may be arranged into a series of structurally intermediate forms between standard oocyte mitochondria and the typical mitochondria with yolk-crystal inclusions. The observation of such intermediate forms is consistent with proposals that the yolk-crystal inclusions arise within a limited portion of the oocyte chondriome by a complex process of mitochondrial differentiation.

Animals↗

Blue phases of cholesteric liquid crystals as thermotropic photonic crystals

The study of dye-doped low pitch cholesteric liquid crystals in their blue phases as an example of tunable "weak" photonic crystals is proposed and demonstrated. The presence of the blue phases in cholesterics can be tuned with temperature, and this allows for an easy in situ comparison of the emission and/or absorption of the dyes with or without an enwrapping lattice of disclination lines. The fluorescence emission of the dyes is shown to be affected by the presence of the blue phases. Although unlikely to be suitable for real applications (due to the natural low refractive index contrast), these systems may represent unique examples of tunable photonic crystals. It is proposed that single crystals of dye-doped blue phases should provide a very interesting testing ground for the study of optical emission anisotropies which can, on the other hand, be controlled by an external parameter.

Journal Article↗

Further evidence of spinodal decomposition during the induction period of polymer crystallization: time-resolved small-angle x-ray scattering prior to crystallization of poly(ethylene naphthalate)

Aiming to clarify spinodal decomposition of polymers in the induction period of crystallization, time-resolved small-angle x-ray scattering measurements have been made in situ for poly(ethylene naphthalate) while it was crystallized from the glass, or in the case of the so-called glass crystallization. It is confirmed for this polymer that in the very beginning of the induction period a scattering peak appears at around 0.03 A (-1) in scattering vector q, which corresponds to a characteristic wavelength of 200 A in density fluctuations, and grows with time. Time evolution of this scattering peak is described by the kinetics of the spinodal decomposition as previously reported for the glass crystallization of poly(ethylene terephthalate).

Journal Article↗

Coupling of the TE and TM modes of electromagnetic waves in two-dimensional photonic crystals with surface defects of liquid crystals.

We theoretically demonstrate the coupling of the TE and TM modes of electromagnetic waves in two-dimensional photonic crystals with surface defects of liquid crystals. Due to anisotropies of liquid crystals, the TE and TM modes cannot be classified generally in the surface defects, which causes the coupling of the TE and TM modes. The coupling of the TE and TM modes occurs strongly at frequencies at which group velocities of electromagnetic waves become zero, especially at surface defect modes. Possibility of the sharp tunability and the switching of the transmittance in this system has been demonstrated theoretically by the control of directors of liquid crystals by applied electric field due to their anisotropy.

Journal Article↗

TE-TM mode coupling in two-dimensional photonic crystals composed of liquid-crystal rods.

We theoretically demonstrate the TE-TM mode coupling in two-dimensional photonic crystals composed of liquid-crystal rods due to anisotropies of liquid crystals. In such structures, the classification of the TE and TM modes is generally impossible, that is, the TE-TM mode coupling occurs. Frequencies of the mode coupling are investigated by the plane-wave expansion method, and the mode coupling is discussed by transmittance calculated by the finite-difference time-domain method. Changes of transmittance by rotating directors of liquid crystals are also discussed.

Journal Article↗

Self-alignment of liquid crystals in three-dimensional photonic crystals.

We report on the observation of self-alignment of nematic liquid crystals into colloidal photonic crystals, over distances much larger than the typical size of the voids between the spheres. We observe that the infiltrated structure possesses a unique optical axis that is determined by an intrinsic structural anisotropy of photonic crystal opals. We develop a simple model to describe this self-alignment based on the connectivity of the pores. The resulting structure constitutes a polarization dependent photonic crystal that can be controlled electrically.

Journal Article↗

Direct visualization of random crystallization and melting in arrays of nanometer-size polymer crystals.

Using tapping mode atomic force microscopy, we visualized in direct space and time resolved the changes in viscoelastic properties during crystallization and melting of polyethyleneoxide in 12 nm spheres of a block copolymer mesophase. All spheres crystallized individually and independently, randomly distributed sphere by sphere. Melting of the confined crystals also proceeded in a stochastic manner. Not all spheres melted at the same temperature, indicating different degrees of order of the individual nanometer-size polymer crystals. The independence of the spheres opens the possibility to manipulate material properties of surfaces at the nanometer scale.

Journal Article↗

Analysis of voids in crystal structures: the methods of 'dual' crystal chemistry.

The theoretical basics of the analysis of voids in crystal structures by means of Voronoi-Dirichlet polyhedra (VDP) and of the graph theory are stated. Topological relations are considered between VDPs and atomic domains in a crystal field. These relations allow the separation of two non-intersecting topological subspaces in a crystal structure, whose connectednesses are defined by two finite 'reduced' graphs. The first, 'direct', subspace includes the atoms (VDP centres) and the network of interatomic bonds (VDP faces), the second, 'dual', one comprises the void centres (VDP vertices) and the system of channels (VDP edges) between them. Computer methods of geometrical-topological analysis of the 'dual' subspace are developed and implemented within the program package TOPOS. They are designed for automatically restoring the system of channels, visualizing and sizing voids and void conglomerates, dimensional analysis of continuous void systems, and comparative topological analysis of 'dual' subspaces for various substances. The methods of analysis of 'dual' and 'direct' subspaces are noted to differ from each other only in some details that allows the term 'dual' crystal chemistry to be introduced. The efficiency of the methods is shown with the analysis of compounds of different chemical nature: simple substances, ionic structures, superionic conductors, zeolites, clathrates, organic supramolecular complexes.

Journal Article↗

General rules for the packing of hydrogen-bonded crystals as derived from the analysis of squaric acid anions: aminoaromatic nitrogen base co-crystals.

Preparation and single-crystal X-ray structure determination of three co-crystals of hydrogen squarate, HSQ(-), with 2-aminopyrimidine, 3-aminopyridine and 4-aminopyridine, and one of squarate, SQ(2-), with 8-aminoquinoline are reported. Their crystal packings are analyzed and discussed in terms of the intermolecular O--H...O, N--H...O/N and C--H...O hydrogen bonds formed. Although the fine details of the supramolecular architecture are barely rationalizable, the comparative analysis of the data makes it possible to suggest some simple rules that may be of general application for the packing of hydrogen-bonded crystals, i.e. Rule 1: 'All hydrogen-bond acceptors available in a molecule will be engaged in hydrogen bonding as far as there are available donors'; Rule 2: 'The hydrogen-bond acceptors will be saturated in order of decreasing strength of the hydrogen bonds formed'.

Journal Article↗